Yb∶GdScO₃晶体光谱参数计算 增强出版

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"bio": [ { "lang": "zh", "text": [ "张庆礼（1973-），男，云南会泽人，博士，研究员，博士生导师，2001年于中国科学技术大学获得博士学位，主要从事光学材料的晶体生长技术及发光物理等领域的研究。" ], "graphic": [ { "print": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599202&type=", "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599202&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599202&type=", "width": "24.89199829", "height": "29.88732910", "fontsize": "" } ], "data": [ [ { "name": "text", "data": "张庆礼" }, { "name": "text", "data": "（1973-），男，云南会泽人，博士，研究员，博士生导师，2001年于中国科学技术大学获得博士学位，主要从事光学材料的晶体生长技术及发光物理等领域的研究。" } ] ] } ], "email": "zql@aiofm.ac.cn", "deceased": false }, { "name": [ { "lang": "zh", "surname": "孙", "givenname": "贵花", "namestyle": "eastern", "prefix": "" }, { "lang": "en", "surname": "SUN", "givenname": "Gui-hua", "namestyle": "eastern", "prefix": "" } ], "stringName": [], "aff": [ { "rid": "aff1", "text": "1" }, { "rid": "aff2", "text": "2" } ], 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"text": "2" } ], "role": [], "deceased": false }, { "name": [ { "lang": "zh", "surname": "罗", "givenname": "建乔", "namestyle": "eastern", "prefix": "" }, { "lang": "en", "surname": "LUO", "givenname": "Jian-qiao", "namestyle": "eastern", "prefix": "" } ], "stringName": [], "aff": [ { "rid": "aff1", "text": "1" }, { "rid": "aff2", "text": "2" } ], "role": [], "deceased": false }, { "name": [ { "lang": "zh", "surname": "孙", "givenname": "彧", "namestyle": "eastern", "prefix": "" }, { "lang": "en", "surname": "SUN", "givenname": "Yu", "namestyle": "eastern", "prefix": "" } ], "stringName": [], "aff": [ { "rid": "aff1", "text": "1" }, { "rid": "aff2", "text": "2" } ], "role": [], "deceased": false } ], "aff": [ { "id": "aff1", "intro": [ { "lang": "zh", "label": "1", "text": "中国科学院合肥物质科学研究院安徽光学精密机械研究所 安徽省光子器件与材料重点实验室， 安徽 合肥　230031", "data": [ { "name": "text", "data": "中国科学院合肥物质科学研究院安徽光学精密机械研究所 安徽省光子器件与材料重点实验室， 安徽 合肥　230031" } ] }, { "lang": "en", "label": "1", "text": "The Key Laboratory of Photonic Devices and Materials， Anhui Province， Anhui Institute of Optics and Fine Mechanics， Hefei Institutes of Physical Science， Chinese Academy of Sciences， Hefei 230031， China", "data": [ { "name": "text", "data": "The Key Laboratory of Photonic Devices and Materials， Anhui Province， Anhui Institute of Optics and Fine Mechanics， Hefei Institutes of Physical Science， Chinese Academy of Sciences， Hefei 230031， China" } ] } ] }, { "id": "aff2", "intro": [ { "lang": "zh", "label": "2", "text": "先进激光技术安徽省实验室， 安徽 合肥　230031", "data": [ { "name": "text", "data": "先进激光技术安徽省实验室， 安徽 合肥　230031" } ] }, { "lang": "en", "label": "2", "text": "Advanced Laser Technology Laboratory of Anhui Province， Hefei 230031， China", "data": [ { "name": "text", "data": "Advanced Laser Technology Laboratory of Anhui Province， Hefei 230031， China" } ] } ] }, { "id": "aff3", "intro": [ { "lang": "zh", "label": "3", "text": "中国科学技术大学， 安徽 合肥　230026", "data": [ { "name": "text", "data": "中国科学技术大学， 安徽 合肥　230026" } ] }, { "lang": "en", "label": "3", "text": "University of Science and Technology of China， Hefei 230026， China", "data": [ { "name": "text", "data": "University of Science and Technology of China， Hefei 230026， China" } ] } ] }, { "id": "aff4", "intro": [ { "lang": "zh", "label": "4", "text": "安徽工业大学 数理科学与工程学院， 安徽 马鞍山　243002", "data": [ { "name": "text", "data": "安徽工业大学 数理科学与工程学院， 安徽 马鞍山　243002" } ] }, { "lang": "en", "label": "4", "text": "School of Science and Engineering of Mathematics and Physics， Anhui University of Technology， Maanshan 243002， China", "data": [ { "name": "text", "data": "School of Science and Engineering of Mathematics and Physics， Anhui University of Technology， Maanshan 243002， China" } ] } ] } ] }, "abstracts": [ { "lang": "zh", "data": [ { "name": "p", "data": [ { "name": "text", "data": "采用提拉法生长了质量优良的Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶体，对样品的X射线粉末衍射进行了Rietveld精修，给出了晶体计算密度及掺杂浓度。Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "的有效分凝系数计算为1.04。室温下测量了其吸收光谱、发射光谱和荧光寿命，首次计算了GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "基质中Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "的吸收、发射振子强度、谱线强度、跃迁概率、能级寿命和积分发射截面等重要光谱参数，对其激光性能进行了初步评估。结果表明，Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "易于输出1 030 nm和1 060 nm波段附近的激光，而对于1 000 nm附近的激光输出则只有在高粒子数反转情况下才可能实现。" } ] } ] }, { "lang": "en", "data": [ { "name": "p", "data": [ { "name": "text", "data": "A high quality Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " crystal was grown by Czochralski method. The X-ray diffraction was refined by Rietveld method， and the calculated crystal density and doping concentration were obtained. The effective segregation coefficient of Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": " is calculated to be 1.04.Its absorption spectrum， emission spectrum and fluorescence lifetime were measured at room temperature. The absorption， emission oscillator strength， spectral line strength， transition probability， energy level lifetime and integral emission cross section of Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": " in GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " matrix were calculated for the first time. The laser performance is preliminarily evaluated. The results show that Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " is easy to output laser near 1 030 nm and 1 060 nm， while the laser output near 1 000 nm is only possible under the condition of high population inversion." } ] } ] } ], "keyword": [ { "lang": "zh", "data": [ [ { "name": "text", "data": "Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] } ], [ { "name": "text", "data": "吸收光谱" } ], [ { "name": "text", "data": "发射光谱" } ], [ { "name": "text", "data": "光跃迁" } ] ] }, { "lang": "en", "data": [ [ { "name": "text", "data": "Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] } ], [ { "name": "text", "data": "absorption spectrum" } ], [ { "name": "text", "data": "emission spectrum" } ], [ { "name": "text", "data": "optical transition" } ] ] } ], "highlights": [], "body": [ { "name": "sec", "data": [ { "name": "sectitle", "data": { "title": [ { "name": "text", "data": "1　引　　言" } ], "level": "1", "id": "s1" } }, { "name": "p", "data": [ { "name": "text", "data": "钪酸钆（GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": ")是一种优良的激光基质材料，具有钙钛矿结构（" }, { "name": "italic", "data": [ { "name": "text", "data": "AB" } ] }, { "name": "text", "data": "O" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "、GdFeO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "型)，属正交晶系，空间群为" }, { "name": "italic", "data": [ { "name": "text", "data": "Pnma" } ] }, { "name": "text", "data": "（No.62)" }, { "name": "sup", "data": [ { "name": "text", "data": " [" }, { "name": "blockXref", "data": { "data": [ { "name": "xref", "data": { "text": "1", "type": "bibr", "rid": "R1", "data": [ { "name": "text", "data": "1" } ] } }, { "name": "text", "data": "-" }, { "name": "xref", "data": { "text": "7", "type": "bibr", "rid": "R7", "data": [ { "name": "text", "data": "7" } ] } } ], "rid": [ "R1", "R2", "R3", "R4", "R5", "R6", "R7" ], "text": "1-7", "type": "bibr" } }, { "name": "text", "data": "]" } ] }, { "name": "text", "data": "。其较低的最高声子能量 （452 cm" }, { "name": "sup", "data": [ { "name": "text", "data": "-1" } ] }, { "name": "text", "data": ")以及较宽的带隙，可以最大限度地减少相邻能级之间的非辐射弛豫，从而提升发光效率。此外，该晶体具有较好的热力学特性和化学稳定性，有利于开展高功率泵浦激光研究和应用。特别地，因为Gd" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "与其他稀土离子大小非常接近，因此掺杂的稀土离子可以有效地进入到晶格中，从而可以降低由于掺杂而产生的缺陷和晶格应力的形成，有利于实现高浓度掺杂，进而提高激光效率" }, { "name": "sup", "data": [ { "name": "text", "data": "[" }, { "name": "blockXref", "data": { "data": [ { "name": "xref", "data": { "text": "8", "type": "bibr", "rid": "R8", "data": [ { "name": "text", "data": "8" } ] } }, { "name": "text", "data": "-" }, { "name": "xref", "data": { "text": "13", "type": "bibr", "rid": "R13", "data": [ { "name": "text", "data": "13" } ] } } ], "rid": [ "R8", "R9", "R10", "R11", "R12", "R13" ], "text": "8-13", "type": "bibr" } }, { "name": "text", "data": "]" } ] }, { "name": "text", "data": "。" } ] }, { "name": "p", "data": [ { "name": "text", "data": "Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "能级结构简单，电子构型为[Xe]4f" }, { "name": "sup", "data": [ { "name": "text", "data": "13" } ] }, { "name": "text", "data": "，可视为一个等价空穴，其共轭电子态为4f" }, { "name": "sup", "data": [ { "name": "text", "data": "1" } ] }, { "name": "text", "data": "，相应地仅有两个电子态，即基态" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "7/2" } ] }, { "name": "text", "data": "和激发态" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "5/2" } ] }, { "name": "text", "data": "，两者的能量间隔约为10 000 cm" }, { "name": "sup", "data": [ { "name": "text", "data": "-1[" }, { "name": "blockXref", "data": { "data": [ { "name": "xref", "data": { "text": "14", "type": "bibr", "rid": "R14", "data": [ { "name": "text", "data": "14" } ] } }, { "name": "text", "data": "-" }, { "name": "xref", "data": { "text": "25", "type": "bibr", "rid": "R25", "data": [ { "name": "text", "data": "25" } ] } } ], "rid": [ "R14", "R15", "R16", "R17", "R18", "R19", "R20", "R21", "R22", "R23", "R24", "R25" ], "text": "14-25", "type": "bibr" } }, { "name": "text", "data": "]" } ] }, { "name": "text", "data": "。在晶体场作用下产生斯塔克（Stark)能级分裂后，基态和激发态分别最多分裂为4个和3个子能级，形成准三或准四能级的激光运行机制，不存在激发态吸收、频率上转换和交叉弛豫等过程，避免浓度猝灭效应，光-光转换效率高" }, { "name": "sup", "data": [ { "name": "text", "data": "[" }, { "name": "blockXref", "data": { "data": [ { "name": "xref", "data": { "text": "26", "type": "bibr", "rid": "R26", "data": [ { "name": "text", "data": "26" } ] } }, { "name": "text", "data": "-" }, { "name": "xref", "data": { "text": "33", "type": "bibr", "rid": "R33", "data": [ { "name": "text", "data": "33" } ] } } ], "rid": [ "R26", "R27", "R28", "R29", "R30", "R31", "R32", "R33" ], "text": "26-33", "type": "bibr" } }, { "name": "text", "data": "]" } ] }, { "name": "text", "data": "。其Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "基态Stark分裂较大，导致锁模（ ML )激光器具有宽的波长可调谐性和产生超短脉冲" }, { "name": "sup", "data": [ { "name": "text", "data": "[" }, { "name": "blockXref", "data": { "data": [ { "name": "xref", "data": { "text": "34", "type": "bibr", "rid": "R34", "data": [ { "name": "text", "data": "34" } ] } }, { "name": "text", "data": "-" }, { "name": "xref", "data": { "text": "37", "type": "bibr", "rid": "R37", "data": [ { "name": "text", "data": "37" } ] } } ], "rid": [ "R34", "R35", "R36", "R37" ], "text": "34-37", "type": "bibr" } }, { "name": "text", "data": "]" } ] }, { "name": "text", "data": "。它的吸收带在900~1 000 nm波长范围，能与InGaAs（发射波长870~1 100 nm)半导体激光二极管（LD)泵浦源有效耦合，无需严格的温度控制即可获得相位匹配的泵浦源的泵浦波长" }, { "name": "sup", "data": [ { "name": "text", "data": "[" }, { "name": "blockXref", "data": { "data": [ { "name": "xref", "data": { "text": "38", "type": "bibr", "rid": "R38", "data": [ { "name": "text", "data": "38" } ] } }, { "name": "text", "data": "-" }, { "name": "xref", "data": { "text": "44", "type": "bibr", "rid": "R44", "data": [ { "name": "text", "data": "44" } ] } } ], "rid": [ "R38", "R39", "R40", "R41", "R42", "R43", "R44" ], "text": "38-44", "type": "bibr" } }, { "name": "text", "data": "]" } ] }, { "name": "text", "data": "。因而，Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "是LD泵浦的有效激光工作物质。上海光机所Zhang等报道了基于 3 mm×3 mm×5 mm（3%)的Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶体实现了波长为1 063.9 nm的13.45 W连续激光输出" }, { "name": "sup", "data": [ { "name": "text", "data": "[" }, { "name": "xref", "data": { "text": "45", "type": "bibr", "rid": "R45", "data": [ { "name": "text", "data": "45" } ] } }, { "name": "text", "data": "]" } ] }, { "name": "text", "data": "。对于特定激光晶体来说，掺杂离子浓度决定了其光谱特性和激光性能。本文采用提拉法生长了（5%)Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "单晶，测量了其吸收和发射光谱，首次计算了Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "在GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "基质中的光谱参数，并对晶体的激光性能进行了评估，为下一步实现高效、低阈值激光输出提供了重要的参考。" } ] } ] }, { "name": "sec", "data": [ { "name": "sectitle", "data": { "title": [ { "name": "text", "data": "2　实　　验" } ], "level": "1", "id": "s2" } }, { "name": "p", "data": [ { "name": "text", "data": "采用Czochralski法在氮气氛围中沿[100]方向生长了Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶体。用于生长的设备为JGD800单晶炉，晶体生长的放肩和等径都采用自动控制。所生长的晶体无色、透明、无裂纹，表明晶体质量良好，如" }, { "name": "xref", "data": { "text": "图1", "type": "fig", "rid": "F1", "data": [ { "name": "text", "data": "图1" } ] } }, { "name": "text", "data": "所示。" } ] }, { "name": "fig", "data": { "id": "F1", "caption": [ { "lang": "zh", "label": [ { "name": "text", "data": "图1" } ], "title": [ { "name": "text", "data": "Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "单晶照片" } ] }, { "lang": "en", "label": [ { "name": "text", "data": "Fig.1" } ], "title": [ { "name": "text", "data": "Photograph of the as-grown Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " single crystal" } ] } ], "subcaption": [], "note": [], "graphics": [ { "print": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599204&type=", "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599211&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599206&type=", "width": "63.09982300", "height": "54.34432983", "fontsize": "" } ] } }, { "name": "sec", "data": [ { "name": "sectitle", "data": { "title": [ { "name": "text", "data": "2.1　样品Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶体的X射线衍射" } ], "level": "2", "id": "s2a" } }, { "name": "p", "data": [ { "name": "text", "data": "取少量的晶体样品研磨成粉末，用于测试晶体的X射线衍射，测试仪器为荷兰飞利浦公司生产的X'Pert PROX射线衍射仪，测试角度范围为10°~90°，步进间隔为0.033°。为了获取准确的结构信息，得到Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "在GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "中的浓度用于光谱参数计算，对Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "的晶体粉末X射线衍射图谱进行了Reitveld全谱精修拟合。拟合软件为GSAS。掺杂激活离子Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "与基质中的Gd" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "都是稀土离子，价态相同（都是+3价离子），并且离子半径接近（Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "半径为 0.098 5 nm，Gd" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "半径为0.105 3 nm，Gd" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "/ Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "两者的配位数均为CN=8）， Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "离子在引入Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶格中应取代Gd" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "离子进入其所在的格位。因此在精修时，使用GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶胞结构数据作为初始参考数据，其空间群为" }, { "name": "italic", "data": [ { "name": "text", "data": "Pnma" } ] }, { "name": "text", "data": "，Gd/Yb格位为8个氧原子（GdO" }, { "name": "sub", "data": [ { "name": "text", "data": "8" } ] }, { "name": "text", "data": ")配位的十二面体，Sc格位为6个氧原子（ScO" }, { "name": "sub", "data": [ { "name": "text", "data": "6" } ] }, { "name": "text", "data": "）配位的八面体" }, { "name": "sup", "data": [ { "name": "text", "data": "[" }, { "name": "blockXref", "data": { "data": [ { "name": "xref", "data": { "text": "46", "type": "bibr", "rid": "R46", "data": [ { "name": "text", "data": "46" } ] } }, { "name": "text", "data": "-" }, { "name": "xref", "data": { "text": "51", "type": "bibr", "rid": "R51", "data": [ { "name": "text", "data": "51" } ] } } ], "rid": [ "R46", "R47", "R48", "R49", "R50", "R51" ], "text": "46-51", "type": "bibr" } }, { "name": "text", "data": "]" } ] }, { "name": "text", "data": "。按化学式（Gd" }, { "name": "sub", "data": [ { "name": "text", "data": "0.95" } ] }, { "name": "text", "data": "Yb" }, { "name": "sub", "data": [ { "name": "text", "data": "0.05" } ] }, { "name": "text", "data": "）ScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "固定晶胞中Gd、Yb、Sc和O原子的占有率，对其晶格常数、原子位置坐标、各向同性温度因子（" }, { "name": "italic", "data": [ { "name": "text", "data": "U" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "iso" } ] }, { "name": "text", "data": "）进行了精修。精修结果如" }, { "name": "xref", "data": { "text": "图2", "type": "fig", "rid": "F2", "data": [ { "name": "text", "data": "图2" } ] } }, { "name": "text", "data": "所示，收敛时加权剩余方差因子" }, { "name": "italic", "data": [ { "name": "text", "data": "R" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "wp" } ] }, { "name": "text", "data": "和剩余方差因子" }, { "name": "italic", "data": [ { "name": "text", "data": "R" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "p" } ] }, { "name": "text", "data": "分别为4.97%和3.64%，均小余10%，说明计算值和实验值符合很好。拟合结果结构参数如" }, { "name": "xref", "data": { "text": "表1", "type": "table", "rid": "T1", "data": [ { "name": "text", "data": "表1" } ] } }, { "name": "text", "data": "，晶胞参数" }, { "name": "italic", "data": [ { "name": "text", "data": "a" } ] }, { "name": "text", "data": "= 0.575 731 7 nm, " }, { "name": "italic", "data": [ { "name": "text", "data": "b" } ] }, { "name": "text", "data": "=0.794 584 3 nm, " }, { "name": "italic", "data": [ { "name": "text", "data": "c" } ] }, { "name": "text", "data": "=0.548 934 6 nm," }, { "name": "italic", "data": [ { "name": "text", "data": "α" } ] }, { "name": "text", "data": "=" }, { "name": "italic", "data": [ { "name": "text", "data": "β" } ] }, { "name": "text", "data": "=" }, { "name": "italic", "data": [ { "name": "text", "data": "γ" } ] }, { "name": "text", "data": "=90°，晶胞体积" }, { "name": "italic", "data": [ { "name": "text", "data": "V" } ] }, { "name": "text", "data": "=0.251 119 6 nm" }, { "name": "sup", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "。计算得到Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "的密度" }, { "name": "italic", "data": [ { "name": "text", "data": "ρ" } ] }, { "name": "text", "data": " = 6.622 82 g/cm" }, { "name": "sup", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "。" } ] }, { "name": "fig", "data": { "id": "F2", "caption": [ { "lang": "zh", "label": [ { "name": "text", "data": "图2" } ], "title": [ { "name": "text", "data": "GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶体XRD数据Rietveld精修结果（cal，obs， bckgr和diff表示计算值、实验值、背底以及实验值和计算值之间的误差）" } ] }, { "lang": "en", "label": [ { "name": "text", "data": "Fig.2" } ], "title": [ { "name": "text", "data": "Rietveld refinement results of the GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3 " } ] }, { "name": "text", "data": "crystal obtained from the XRD data（cal， obs， bckgr， and diff mean calculated data， observed data， background， and the difference between observed data and calculated data）" } ] } ], "subcaption": [], "note": [], "graphics": [ { "print": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599214&type=", "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599221&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599217&type=", "width": "69.29306030", "height": "59.22044373", "fontsize": "" } ] } }, { "name": "table", "data": { "id": "T1", "caption": [ { "lang": "zh", "label": [ { "name": "text", "data": "表1" } ], "title": [ { "name": "text", "data": "Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "的Rietveld精细结构参数" } ] }, { "lang": "en", "label": [ { "name": "text", "data": "Tab.1" } ], "title": [ { "name": "text", "data": "Structural parameters from the Rietveld refinement of Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] } ] } ], "note": [], "table": [ { "head": [ [ { "align": "center", "style": "border-top:solid;border-bottom:solid;", "data": [ { "name": "text", "data": "Atom" } ] }, { "align": "center", "style": "border-top:solid;border-bottom:solid;", "data": [ { "name": "text", "data": "Multiplicity Wyckoff letter" } ] }, { "align": "center", "style": "border-top:solid;border-bottom:solid;", "data": [ { "name": "italic", "data": [ { "name": "text", "data": "x" } ] } ] }, { "align": "center", "style": "border-top:solid;border-bottom:solid;", "data": [ { "name": "italic", "data": [ { "name": "text", "data": "y" } ] } ] }, { "align": "center", "style": "border-top:solid;border-bottom:solid;", "data": [ { "name": "italic", "data": [ { "name": "text", "data": "z" } ] } ] }, { "align": "center", "style": "border-top:solid;border-bottom:solid;", "data": [ { "name": "text", "data": "Occupancy" } ] }, { "align": "center", "style": "border-top:solid;border-bottom:solid;", "data": [ { "name": "italic", "data": [ { "name": "text", "data": "U" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "iso" } ] } ] } ] ], "body": [ [ { "align": "center", "data": [ { "name": "text", "data": "O1" } ] }, { "align": "center", "data": [ { "name": "text", "data": "4c" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.470 876" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.250 000" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.081 371" } ] }, { "align": "center", "data": [ { "name": "text", "data": "1.567 7" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.100 79" } ] } ], [ { "align": "center", "data": [ { "name": "text", "data": "Sc1" } ] }, { "align": "center", "data": [ { "name": "text", "data": "4b" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.000 000" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.000 000" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.500 000" } ] }, { "align": "center", "data": [ { "name": "text", "data": "1.056 2" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.051 78" } ] } ], [ { "align": "center", "data": [ { "name": "text", "data": "O2" } ] }, { "align": "center", "data": [ { "name": "text", "data": "8d" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.208 495" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.583 306" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.201 682" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.935 8" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.057 90" } ] } ], [ { "align": "center", "data": [ { "name": "text", "data": "Gd1" } ] }, { "align": "center", "data": [ { "name": "text", "data": "4c" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.442 395" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.750 000" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.516 818" } ] }, { "align": "center", "data": [ { "name": "text", "data": "1.025 2" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.021 93" } ] } ], [ { "align": "center", "data": [ { "name": "text", "data": "Yb1" } ] }, { "align": "center", "data": [ { "name": "text", "data": "4c" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.178 142" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.750 000" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.693 908" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.063 4" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.039 20" } ] } ], [ { "colspan": "7", "align": "justify", "style": "border-bottom:solid;", "data": [ { "name": "p", "data": [ { "name": "text", "data": "Lattice parameters " }, { "name": "italic", "data": [ { "name": "text", "data": "a " } ] }, { "name": "text", "data": "= 0.575 731 7 nm， " }, { "name": "italic", "data": [ { "name": "text", "data": "b" } ] }, { "name": "text", "data": " =0.794 584 3 nm， " }, { "name": "italic", "data": [ { "name": "text", "data": "c" } ] }, { "name": "text", "data": " =0.548 934 6 nm" } ] }, { "name": "p", "data": [ { "name": "italic", "data": [ { "name": "text", "data": "ρ" } ] }, { "name": "text", "data": " = 6.622 82 g/ cm" }, { "name": "sup", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "， " }, { "name": "italic", "data": [ { "name": "text", "data": "V" } ] }, { "name": "text", "data": " = 0.251 119 6 nm" }, { "name": "sup", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "， space group： " }, { "name": "italic", "data": [ { "name": "text", "data": "Pnma" } ] }, { "name": "text", "data": " （No.62）" } ] }, { "name": "p", "data": [ { "name": "italic", "data": [ { "name": "text", "data": "R" } ] }, { "name": "text", "data": " factor " }, { "name": "italic", "data": [ { "name": "text", "data": " R" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "p" } ] }, { "name": "text", "data": " = 3.64%， " }, { "name": "italic", "data": [ { "name": "text", "data": "R" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "wp" } ] }, { "name": "text", "data": " = 4.97%" } ] } ] } ] ], "foot": [ [ { "colspan": "7", "align": "left", "style": "border-bottom:solid;", "data": [] } ] ] } ], "graphics": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599226&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599223&type=", "width": "162.79998779", "height": "58.78195190", "fontsize": "" } } } ] }, { "name": "sec", "data": [ { "name": "sectitle", "data": { "title": [ { "name": "text", "data": "2.2　Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶体的组成和分凝系数" } ], "level": "2", "id": "s2b" } }, { "name": "p", "data": [ { "name": "text", "data": "用LA-ICP-MS（美国Agilent 公司生产的Agilent 7500a）仪器测量生长晶体中Yb、Gd和Sc元素的浓度，精度为0.001‰。通过LA-ICP-MS测试得到所生长晶体中Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "、Gd" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "、Sc" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "离子的浓度，如" }, { "name": "xref", "data": { "text": "表2", "type": "table", "rid": "T2", "data": [ { "name": "text", "data": "表2" } ] } }, { "name": "text", "data": "所示。因此，有效分凝系数" }, { "name": "italic", "data": [ { "name": "text", "data": "k" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "eff" } ] }, { "name": "text", "data": "可以用方程" }, { "name": "italic", "data": [ { "name": "text", "data": "k" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "eff" } ] }, { "name": "text", "data": "=" }, { "name": "italic", "data": [ { "name": "text", "data": "C" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "s" } ] }, { "name": "text", "data": "/" }, { "name": "italic", "data": [ { "name": "text", "data": "C" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "l" } ] }, { "name": "text", "data": "计算。其中 " }, { "name": "italic", "data": [ { "name": "text", "data": "C" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "s" } ] }, { "name": "text", "data": "和" }, { "name": "italic", "data": [ { "name": "text", "data": "C" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "l" } ] }, { "name": "text", "data": "分别是晶体和熔体中的掺杂剂浓度。经计算，GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "主体中Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "离子的" }, { "name": "italic", "data": [ { "name": "text", "data": "k" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "eff" } ] }, { "name": "text", "data": "为1.04，比较大，有利于生长均匀掺杂晶体。" } ] }, { "name": "table", "data": { "id": "T2", "caption": [ { "lang": "zh", "label": [ { "name": "text", "data": "表2" } ], "title": [ { "name": "text", "data": "ICPMS分析得到的Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶体组成" } ] }, { "lang": "en", "label": [ { "name": "text", "data": "Tab.2" } ], "title": [ { "name": "text", "data": "Composition of Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3 " } ] }, { "name": "text", "data": "crystal obtained from ICP‐MS analysis" } ] } ], "note": [], "table": [ { "head": [ [ { "align": "center", "style": "border-top:solid;border-bottom:solid;", "data": [ { "name": "text", "data": "Ions" } ] }, { "align": "center", "style": "border-top:solid;border-bottom:solid;", "data": [ { "name": "italic", "data": [ { "name": "text", "data": "C" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "l" } ] }, { "name": "text", "data": "/%" } ] }, { "align": "center", "style": "border-top:solid;border-bottom:solid;", "data": [ { "name": "italic", "data": [ { "name": "text", "data": "C" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "s" } ] }, { "name": "text", "data": "/%" } ] }, { "align": "center", "style": "border-top:solid;border-bottom:solid;", "data": [ { "name": "italic", "data": [ { "name": "text", "data": "k" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "eff" } ] } ] } ] ], "body": [ [ { "align": "center", "data": [ { "name": "text", "data": "Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] } ] }, { "align": "center", "data": [ { "name": "text", "data": "5" } ] }, { "align": "center", "data": [ { "name": "text", "data": "5.2" } ] }, { "align": "center", "data": [ { "name": "text", "data": "1.040 0" } ] } ], [ { "align": "center", "data": [ { "name": "text", "data": "Gd" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] } ] }, { "align": "center", "data": [ { "name": "text", "data": "95" } ] }, { "align": "center", "data": [ { "name": "text", "data": "94.8" } ] }, { "align": "center", "data": [ { "name": "text", "data": "0.997 8" } ] } ], [ { "align": "center", "style": "border-bottom:solid;", "data": [ { "name": "text", "data": "Sc" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] } ] }, { "align": "center", "style": "border-bottom:solid;", "data": [ { "name": "text", "data": "100" } ] }, { "align": "center", "style": "border-bottom:solid;", "data": [ { "name": "text", "data": "122.70" } ] }, { "align": "center", "style": "border-bottom:solid;", "data": [ { "name": "text", "data": "1.227 0" } ] } ] ], "foot": [] } ], "graphics": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599232&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599229&type=", "width": "77.69583130", "height": "19.12274170", "fontsize": "" } } } ] }, { "name": "sec", "data": [ { "name": "sectitle", "data": { "title": [ { "name": "text", "data": "2.3　Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶体的光谱分析" } ], "level": "2", "id": "s2c" } }, { "name": "p", "data": [ { "name": "text", "data": "截取厚度为2 mm的薄片，样品经切割、粗磨、细磨、两面抛光用于透射光谱测试，抛光后测试样品的厚度为1.425 mm。用荧光分光光度计（Edinburgh FLSP-920）在450 W Xe灯下测量其荧光光谱，以916 nm闪光灯作为光源，激发得到荧光衰减曲线。用Perkin Elmer公司的Lamda950紫外-可见-红外分光光度计在室温下进行透射光谱测量，光谱分辨率为0.5 nm。" } ] }, { "name": "p", "data": [ { "name": "xref", "data": { "text": "图3", "type": "fig", "rid": "F3", "data": [ { "name": "text", "data": "图3" } ] } }, { "name": "text", "data": "是Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶体在916 nm波长激发下的室温（300 K）发射光谱。986，999，1 030， 1 060 nm处的发射峰分别对应Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "离子的" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "5/2" } ] }, { "name": "text", "data": "（2） →" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "7/2" } ] }, { "name": "text", "data": "（3）、" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "5/2" } ] }, { "name": "text", "data": "（1） →" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "7/2" } ] }, { "name": "text", "data": "（2）、" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "5/2" } ] }, { "name": "text", "data": "（0） →" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "7/2" } ] }, { "name": "text", "data": "（2）、" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "5/2" } ] }, { "name": "text", "data": "（0） →" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "7/2" } ] }, { "name": "text", "data": "（3）的跃迁，" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "7/2" } ] }, { "name": "text", "data": "和" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "5/2" } ] }, { "name": "text", "data": "的晶场能级分裂均为二度简并，" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "italic", "data": [ { "name": "sup", "data": [ { "name": "text", "data": "S" } ] } ] }, { "name": "sup", "data": [ { "name": "text", "data": "+1" } ] }, { "name": "italic", "data": [ { "name": "text", "data": "L" }, { "name": "sub", "data": [ { "name": "text", "data": "J" } ] } ] }, { "name": "text", "data": "（" }, { "name": "italic", "data": [ { "name": "text", "data": "n" } ] }, { "name": "text", "data": "）中的" }, { "name": "italic", "data": [ { "name": "text", "data": "n" } ] }, { "name": "text", "data": "表示每个Stark能级由低到高的序号，序号从0开始。Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "的最强荧光峰位于999 nm处。能级图如" }, { "name": "xref", "data": { "text": "图4", "type": "fig", "rid": "F4", "data": [ { "name": "text", "data": "图4" } ] } }, { "name": "text", "data": "所示。" } ] }, { "name": "fig", "data": { "id": "F3", "caption": [ { "lang": "zh", "label": [ { "name": "text", "data": "图3" } ], "title": [ { "name": "text", "data": "Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶体在916 nm激光激发下的室温发射光谱" } ] }, { "lang": "en", "label": [ { "name": "text", "data": "Fig.3" } ], "title": [ { "name": "text", "data": "Emission spectrum of Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " crystal excited by 916 nm laser" } ] } ], "subcaption": [], "note": [], "graphics": [ { "print": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599236&type=", "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599242&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599239&type=", "width": "65.12023926", "height": "53.80624390", "fontsize": "" } ] } }, { "name": "fig", "data": { "id": "F4", "caption": [ { "lang": "zh", "label": [ { "name": "text", "data": "图4" } ], "title": [ { "name": "text", "data": "Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "能级分裂图" } ] }, { "lang": "en", "label": [ { "name": "text", "data": "Fig.4" } ], "title": [ { "name": "text", "data": "Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " energy level splitting diagram" } ] } ], "subcaption": [], "note": [], "graphics": [ { "print": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599244&type=", "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599250&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599247&type=", "width": "68.54733276", "height": "47.91656494", "fontsize": "" } ] } }, { "name": "p", "data": [ { "name": "text", "data": "在室温下，以916 nm闪光灯作为光源，监测999 nm发光，测试了Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶体的荧光寿命，结果如" }, { "name": "xref", "data": { "text": "图5", "type": "fig", "rid": "F5", "data": [ { "name": "text", "data": "图5" } ] } }, { "name": "text", "data": "所示。经过单指数拟合得到Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "的" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "5/2" } ] }, { "name": "text", "data": "→" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "7/2" } ] }, { "name": "text", "data": "跃迁的荧光寿命为1 060 µs。与其他Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "掺杂的激光材料相比，如Yb∶YAG的荧光寿命为970 µs，Yb∶GGG的荧光寿命为800 µs，Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶体具有较长的荧光寿命，这将有利于增加布居激光上能级粒子数，利于储能获得高峰值功率调" }, { "name": "italic", "data": [ { "name": "text", "data": "Q" } ] }, { "name": "text", "data": "激光输出。" } ] }, { "name": "fig", "data": { "id": "F5", "caption": [ { "lang": "zh", "label": [ { "name": "text", "data": "图5" } ], "title": [ { "name": "text", "data": "Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶体Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "的" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "5/2" } ] }, { "name": "text", "data": "→" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "7/2" } ] }, { "name": "text", "data": "跃迁的荧光衰减 曲线" } ] }, { "lang": "en", "label": [ { "name": "text", "data": "Fig.5" } ], "title": [ { "name": "text", "data": "Fluorescence decay curves of the " }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "5/2" } ] }, { "name": "text", "data": "→" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "7/2 " } ] }, { "name": "text", "data": "transition of Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " crystal" } ] } ], "subcaption": [], "note": [], "graphics": [ { "print": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599252&type=", "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599258&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599255&type=", "width": "68.86772156", "height": "53.80613708", "fontsize": "" } ] } }, { "name": "p", "data": [ { "name": "text", "data": "室温下测量了Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶体在250~3 000 nm范围内的吸收光谱，结果如" }, { "name": "xref", "data": { "text": "图6", "type": "fig", "rid": "F6", "data": [ { "name": "text", "data": "图6" } ] } }, { "name": "text", "data": "所示。在880~ 1 020 nm范围内，仅有Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "的特征吸收，这与晶体为无色透明的结果一致（如" }, { "name": "xref", "data": { "text": "图1", "type": "fig", "rid": "F1", "data": [ { "name": "text", "data": "图1" } ] } }, { "name": "text", "data": "所示）。根据晶体的吸收系数，采用下式可以计算出晶体的吸收截面" }, { "name": "italic", "data": [ { "name": "text", "data": "σ" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "abs" } ] }, { "name": "text", "data": "：" } ] }, { "name": "dispformula", "data": { "label": [ { "name": "text", "data": "（1）" } ], "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599264&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599262&type=", "width": "12.95400047", "height": "7.28133297", "fontsize": "" } } }, { "name": "text", "data": "，" } ], "id": "DF1" } }, { "name": "p", "data": [ { "name": "text", "data": "其中" }, { "name": "italic", "data": [ { "name": "text", "data": "α" } ] }, { "name": "text", "data": "为吸收系数，" }, { "name": "italic", "data": [ { "name": "text", "data": "N" } ] }, { "name": "text", "data": "为掺杂离子浓度。计算得到的吸收截面值如" }, { "name": "xref", "data": { "text": "图7", "type": "fig", "rid": "F7", "data": [ { "name": "text", "data": "图7" } ] } }, { "name": "text", "data": "所示，最高和次高吸收截面位于985 nm和964 nm处，对应的吸收截面值分别为1.482×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-20" } ] }, { "name": "text", "data": " cm" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "和1.480×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-20" } ] }, { "name": "text", "data": " cm" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "。" } ] }, { "name": "fig", "data": { "id": "F6", "caption": [ { "lang": "zh", "label": [ { "name": "text", "data": "图6" } ], "title": [ { "name": "text", "data": "Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "的吸收光谱" } ] }, { "lang": "en", "label": [ { "name": "text", "data": "Fig. 6" } ], "title": [ { "name": "text", "data": "Absorption spectrum of Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] } ] } ], "subcaption": [], "note": [], "graphics": [ { "print": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599267&type=", "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599273&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599270&type=", "width": "72.18896484", "height": "53.80610657", "fontsize": "" } ] } }, { "name": "fig", "data": { "id": "F7", "caption": [ { "lang": "zh", "label": [ { "name": "text", "data": "图7" } ], "title": [ { "name": "text", "data": "Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "的吸收和发射截面" } ] }, { "lang": "en", "label": [ { "name": "text", "data": "Fig.7" } ], "title": [ { "name": "text", "data": "Absorption and emission cross sections of Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] } ] } ], "subcaption": [], "note": [], "graphics": [ { "print": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599276&type=", "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599282&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599278&type=", "width": "69.94833374", "height": "54.92520142", "fontsize": "" } ] } } ] } ] }, { "name": "sec", "data": [ { "name": "sectitle", "data": { "title": [ { "name": "text", "data": "3　实验结果和讨论" } ], "level": "1", "id": "s3" } }, { "name": "p", "data": [ { "name": "text", "data": "稀土离子在固体中的发光现象发现较早，一类是线状光谱的4f" }, { "name": "italic", "data": [ { "name": "sup", "data": [ { "name": "text", "data": "N" } ] } ] }, { "name": "text", "data": "组态内的能级之间跃迁，即4f-4f跃迁；另一类是带状光谱，它是4f" }, { "name": "italic", "data": [ { "name": "sup", "data": [ { "name": "text", "data": "N" } ] } ] }, { "name": "text", "data": "组态内的能级和其他组态能级之间的跃迁，比如4f" }, { "name": "italic", "data": [ { "name": "sup", "data": [ { "name": "text", "data": "N" } ] } ] }, { "name": "text", "data": "组态和4f" }, { "name": "italic", "data": [ { "name": "sup", "data": [ { "name": "text", "data": "N" } ] } ] }, { "name": "sup", "data": [ { "name": "text", "data": "-1" } ] }, { "name": "text", "data": "5d组态能级之间的跃迁，即4f-5d跃迁。对于自由稀土离子，电偶极作用不能引起4f-4f跃迁，因为4f" }, { "name": "italic", "data": [ { "name": "sup", "data": [ { "name": "text", "data": "N" } ] } ] }, { "name": "text", "data": "组态内各个状态的宇称是相同的，它们之间的电偶极跃迁的矩阵元的值为零，因此，4f" }, { "name": "italic", "data": [ { "name": "sup", "data": [ { "name": "text", "data": "N" } ] } ] }, { "name": "text", "data": "组态内的能级之间跃迁是宇称禁戒的。一般认为由于晶体场奇次项的作用，使与4f" }, { "name": "italic", "data": [ { "name": "sup", "data": [ { "name": "text", "data": "N" } ] } ] }, { "name": "text", "data": "组态状态相反宇称的组态状态混入到4f" }, { "name": "italic", "data": [ { "name": "sup", "data": [ { "name": "text", "data": "N" } ] } ] }, { "name": "text", "data": "组态状态之中，比如4f" }, { "name": "italic", "data": [ { "name": "sup", "data": [ { "name": "text", "data": "N" } ] } ] }, { "name": "sup", "data": [ { "name": "text", "data": "-1" } ] }, { "name": "text", "data": "5d或4f" }, { "name": "italic", "data": [ { "name": "sup", "data": [ { "name": "text", "data": "N" } ] } ] }, { "name": "sup", "data": [ { "name": "text", "data": "-1" } ] }, { "name": "text", "data": "5g组态，这样，在固体和溶液中的稀土离子中原来的4f" }, { "name": "italic", "data": [ { "name": "sup", "data": [ { "name": "text", "data": "N" } ] } ] }, { "name": "text", "data": "组态状态已经不再是一种宇称的状态，而是两种宇称状态的混合态，这些状态之间的电偶极跃迁矩阵元不再为零，出现了线状光谱的4f-4f跃迁。以此为基础，1962年，Judd和Ofelt分别给出了稀土4f组态电子跃迁的强度计算公式，该理论通常称为J-O理论" }, { "name": "sup", "data": [ { "name": "text", "data": "[" }, { "name": "blockXref", "data": { "data": [ { "name": "xref", "data": { "text": "52", "type": "bibr", "rid": "R52", "data": [ { "name": "text", "data": "52" } ] } }, { "name": "text", "data": "-" }, { "name": "xref", "data": { "text": "56", "type": "bibr", "rid": "R56", "data": [ { "name": "text", "data": "56" } ] } } ], "rid": [ "R52", "R53", "R54", "R55", "R56" ], "text": "52-56", "type": "bibr" } }, { "name": "text", "data": "]" } ] }, { "name": "text", "data": "。" } ] }, { "name": "p", "data": [ { "name": "text", "data": "在中间耦合情形下，4" }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599288&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599285&type=", "width": "2.28600001", "height": "3.47133350", "fontsize": "" } } } ] }, { "name": "text", "data": " " }, { "name": "italic", "data": [ { "name": "sup", "data": [ { "name": "text", "data": "n" } ] } ] }, { "name": "text", "data": "稀土离子在两个" }, { "name": "italic", "data": [ { "name": "text", "data": "J" } ] }, { "name": "text", "data": "多重态" }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599294&type=", "big": 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"fontsize": "" } } }, { "name": "text", "data": "+2" }, { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599337&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599334&type=", "width": "3.80999994", "height": "3.72533321", "fontsize": "" } } }, { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599343&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599339&type=", "width": "2.79399991", "height": "3.38666677", "fontsize": "" } } }, { "name": "italic", "data": [ { "name": "sup", "data": [ { "name": "text", "data": "n" } ] } ] }, { "name": "text", "data": "[" }, { "name": "italic", "data": [ { "name": "text", "data": "α'S'L'" } ] }, { "name": "text", "data": "]" }, { "name": "italic", "data": [ { "name": "text", "data": "J" } ] }, { "name": "text", "data": "'" }, { "name": "text", "data": ">" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "=3.72797562×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-26" } ] }, { "name": "text", "data": "<" }, { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599351&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599347&type=", "width": "3.47133350", "height": "3.72533321", "fontsize": "" } } }, { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599359&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599355&type=", "width": "3.55599999", "height": "3.72533321", "fontsize": "" } } }, { "name": "math", "data": { "math": "", "graphicsData": { "small": 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"math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599384&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599381&type=", "width": "1.86266661", "height": "3.38666677", "fontsize": "" } } }, { "name": "italic", "data": [ { "name": "sup", "data": [ { "name": "text", "data": "n" } ] } ] }, { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599390&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599387&type=", "width": "3.55599999", "height": "3.72533321", "fontsize": "" } } }, { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599397&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599394&type=", "width": "8.21266651", 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"italic", "data": [ { "name": "text", "data": "'S'L'" } ] }, { "name": "text", "data": "］" }, { "name": "italic", "data": [ { "name": "text", "data": "J" } ] }, { "name": "text", "data": "'" }, { "name": "text", "data": ">" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "，" } ], "id": "DF3" } }, { "name": "p", "data": [ { "name": "text", "data": "参数" }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599488&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599486&type=", "width": "2.87866688", "height": "2.79399991", "fontsize": "" } } } ] }, { "name": "text", "data": "（具有面积量纲）包含了晶体场强度、两个相反宇称组态的能量差、内部组态的径向积分，包括了静态和振动诱导电偶极子跃迁，它的值可由吸收光谱或发射光谱的实验结果拟合确定。跃迁选择定则为：Δ" }, { "name": "italic", "data": [ { "name": "text", "data": "S" } ] }, { "name": "text", "data": "=0, " }, { "name": 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"fontsize": "" } } } ] }, { "name": "italic", "data": [ { "name": "text", "data": "t" } ] }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599505&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599504&type=", "width": "12.95400047", "height": "3.89466691", "fontsize": "" } } } ] }, { "name": "text", "data": "。" } ] }, { "name": "p", "data": [ { "name": "italic", "data": [ { "name": "text", "data": "S" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "md" } ] }, { "name": "text", "data": "和" }, { "name": "italic", "data": [ { "name": "text", "data": "S" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "ed" } ] }, { "name": "text", "data": "具有面积量纲。对于Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "离子来说，由于实验上仅能观察到一对" }, { "name": "italic", "data": [ { "name": "text", "data": "J" } ] }, { "name": "text", "data": "多重态的跃迁，因而实验上不能直接通过拟合吸收光谱的办法来确定" }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599509&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599507&type=", "width": "3.38666677", "height": "3.89466691", "fontsize": "" } } } ] }, { "name": "text", "data": "，通常需要采用文献[" }, { "name": "xref", "data": { "text": "57", "type": "bibr", "rid": "R57", "data": [ { "name": "text", "data": "57" } ] } }, { "name": "text", "data": "]提出的全谱拟合方法才能确定。" } ] }, { "name": "p", "data": [ { "name": "text", "data": "通常定义无量纲振子跃迁强度" }, { "name": "italic", "data": [ { "name": "text", "data": "f" } ] }, { "name": "text", "data": "为：" } ] }, { "name": "dispformula", "data": { "label": [ { "name": "text", "data": "（4）" } ], "data": [ { "name": "italic", "data": [ { "name": "text", "data": "f" } 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"http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599518&type=", "width": "2.28600001", "height": "3.38666677", "fontsize": "" } } } ] }, { "name": "text", "data": "为与材料有关的校正因子，对折射率为" }, { "name": "italic", "data": [ { "name": "text", "data": "n" } ] }, { "name": "text", "data": "的各项同性介质，电偶极子和磁偶极子" }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599520&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599518&type=", "width": "2.28600001", "height": "3.38666677", "fontsize": "" } } } ] }, { "name": "text", "data": "分别为 " }, { "name": "italic", "data": [ { "name": "text", "data": "n" } ] }, { "name": "text", "data": "（" }, { "name": "italic", "data": [ { "name": "text", "data": "n" } ] }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "+2）/9和" }, { "name": "italic", "data": [ { "name": "text", "data": "n" } ] }, { "name": "sup", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "。" }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599523&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599522&type=", "width": "2.28600001", "height": "3.13266683", "fontsize": "" } } } ] }, { "name": "text", "data": "为跃迁平均波长，对吸收光谱，可取为吸收光谱带的重心波长值。" } ] }, { "name": "p", "data": [ { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599525&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599524&type=", "width": "7.70466709", "height": "3.80999994", "fontsize": "" } } } ] }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599527&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599526&type=", "width": "4.82600021", "height": "3.80999994", "fontsize": "" } } } ] }, { "name": "italic", "data": [ { "name": "text", "data": "bJ" } ] }, { "name": "text", "data": "'" }, { "name": "text", "data": ">" }, { "name": "text", "data": "间的自发辐射概率" }, { "name": "italic", "data": [ { "name": "text", "data": "A" } ] }, { "name": "text", "data": "由下式计算：" } ] }, { "name": "dispformula", "data": { "label": [ { "name": "text", "data": "（5）" } ], "data": [ { "name": "italic", "data": [ { "name": "text", "data": "A" } ] }, { "name": "text", "data": "（" }, { "name": "italic", "data": [ { "name": "text", "data": "aJ" } ] }, { "name": "text", "data": "；" }, { "name": "italic", "data": [ { "name": "text", "data": "bJ" } ] }, { "name": "text", "data": "'）=" }, { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599529&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599528&type=", "width": "2.96333337", "height": "3.38666677", "fontsize": "" } } }, { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599531&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599530&type=", "width": "23.96066666", "height": "8.72066593", "fontsize": "" } } }, { "name": "italic", "data": [ { "name": "text", "data": "S" } ] }, { "name": "text", "data": "（" }, { "name": "italic", "data": [ { "name": "text", "data": "aJ" } ] }, { "name": "text", "data": "；" }, { "name": "italic", "data": [ { "name": "text", "data": "bJ" } ] }, { "name": "text", "data": "'），" } ], "id": "DF5" } }, { "name": "p", "data": [ { "name": "text", "data": "其中，" }, { "name": "italic", "data": [ { "name": "text", "data": "e" } ] }, { "name": "text", "data": "为电荷常数，" }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599533&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599532&type=", "width": "1.94733346", "height": "2.62466669", "fontsize": "" } } } ] }, { "name": "sub", "data": [ { "name": "text", "data": "0" } ] }, { "name": "text", "data": "为真空介电常数。" } ] }, { "name": "p", "data": [ { "name": "text", "data": "实验上，振子强度可由吸收光谱来测定：" } ] }, { "name": "dispformula", "data": { "label": [ { "name": "text", "data": "（6）" } ], "data": [ { "name": "italic", "data": [ { "name": "text", "data": "f " } ] }, { "name": "sup", "data": [ { "name": "text", "data": "exp" } ] }, { "name": "text", "data": "=" }, { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599535&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599534&type=", "width": "24.04533195", "height": "7.61999989", "fontsize": "" } } }, { "name": "text", "data": "=" }, { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599537&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599536&type=", "width": "23.62199974", "height": "7.61999989", "fontsize": "" } } }, { "name": "text", "data": " " }, { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599539&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599538&type=", "width": "28.95599937", "height": "8.12800026", "fontsize": "" } } }, { "name": "text", "data": "，" } ], "id": "DF6" } }, { "name": "p", "data": [ { "name": "text", "data": "其中" }, { "name": "italic", "data": [ { "name": "text", "data": "N" } ] }, { "name": "text", "data": "为单位介质内的稀土离子数，相应的实验谱线强度" }, { "name": "italic", "data": [ { "name": "text", "data": "S" } ] }, { "name": "sup", "data": [ { "name": "text", "data": "exp" } ] }, { "name": "text", "data": "（" }, { "name": "italic", "data": [ { "name": "text", "data": "aJ" } ] }, { "name": "text", "data": ";" }, { "name": "italic", "data": [ { "name": "text", "data": "bJ" } ] }, { "name": "text", "data": "'）为" } ] }, { "name": "p", "data": [ { "name": "italic", "data": [ { "name": "text", "data": "S" } ] }, { "name": "sup", "data": [ { "name": "text", "data": "exp" } ] }, { "name": "text", "data": "（" }, { "name": "italic", "data": [ { "name": "text", "data": "aJ" } ] }, { "name": "text", "data": ";" }, { "name": "italic", "data": [ { "name": "text", "data": "bJ" } ] }, { "name": "text", "data": "'）= " }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599542&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599540&type=", "width": "40.47066879", "height": "8.55133343", "fontsize": "" } } } ] } ] }, { "name": "dispformula", "data": { "label": [ { "name": "text", "data": "（7）" } ], "data": [ { "name": "text", "data": "=" }, { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599544&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599543&type=", "width": "41.65599823", "height": "8.46666718", "fontsize": "" } } }, { "name": "text", "data": "，" } ], "id": "DF7" } }, { "name": "p", "data": [ { "name": "text", "data": "其中" }, { "name": "italic", "data": [ { "name": "text", "data": "，" } ] }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599546&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599545&type=", "width": "2.45533323", "height": "2.62466669", "fontsize": "" } } } ] }, { "name": "text", "data": "为吸收截面，" }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599548&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599547&type=", "width": "7.45066643", "height": "3.47133350", "fontsize": "" } } } ] }, { "name": "text", "data": "为吸收系数，" }, { "name": "italic", "data": [ { "name": "text", "data": "n" } ] }, { "name": "text", "data": "为介质折射率。积分对" }, { "name": "italic", "data": [ { "name": "text", "data": "aJ" } ] }, { "name": "text", "data": "→" }, { "name": "italic", "data": [ { "name": "text", "data": "bJ" } ] }, { "name": "text", "data": "'的吸收带进行。" } ] }, { "name": "p", "data": [ { "name": "text", "data": "如果同一谱线包含了磁偶极子和电偶极子跃迁，则有" } ] }, { "name": "dispformula", "data": { "label": [ { "name": "text", "data": "（8）" } ], "data": [ { "name": "italic", "data": [ { "name": "text", "data": "f" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "ED" } ] }, { "name": "text", "data": "+" }, { "name": "italic", "data": [ { "name": "text", "data": "f" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "MD" } ] }, { "name": "text", "data": "=" }, { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599550&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599549&type=", "width": "24.04533195", "height": "7.61999989", "fontsize": "" } } }, { "name": "text", "data": "，" } ], "id": "DF8" } }, { "name": "p", "data": [ { "name": "text", "data": "因为磁偶极子振子强度" }, { "name": "italic", "data": [ { "name": "text", "data": "f" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "MD" } ] }, { "name": "text", "data": "可以直接计算，故由" }, { "name": "xref", "data": { "text": "公式（8）", "type": "disp-formula", "rid": "DF8", "data": [ { "name": "text", "data": "公式（8）" } ] } }, { "name": "text", "data": "可计算出电偶极子的振子强度" }, { "name": "italic", "data": [ { "name": "text", "data": "f" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "ED" } ] }, { "name": "text", "data": "。" } ] }, { "name": "p", "data": [ { "name": "text", "data": "由于Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "只有" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "7/2" } ] }, { "name": "text", "data": "和" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "5/2" } ] }, { "name": "text", "data": "两个多重态能级，不能通过实验来确定它的3个实验振子强度参数" }, { "name": "italic", "data": [ { "name": "text", "data": "Ω" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "、" }, { "name": "italic", "data": [ { "name": "text", "data": "Ω" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "4" } ] }, { "name": "text", "data": "、" }, { "name": "italic", "data": [ { "name": "text", "data": "Ω" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "6" } ] }, { "name": "text", "data": "。因此，两个能级间的谱线跃迁强度 " }, { "name": "italic", "data": [ { "name": "text", "data": "S（aJ" } ] }, { "name": "text", "data": "; " }, { "name": "italic", "data": [ { "name": "text", "data": "bJ" } ] }, { "name": "text", "data": "'）可由吸收系数计算获得，进而可对材料的其他光谱跃迁参数进行计算。" } ] }, { "name": "p", "data": [ { "name": "text", "data": "如" }, { "name": "xref", "data": { "text": "图3", "type": "fig", "rid": "F3", "data": [ { "name": "text", "data": "图3" } ] } }, { "name": "text", "data": "所示，Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "的特征吸收波长最大值在999 nm，重心吸收波长（即平均吸收波长）" }, { "name": "italic", "data": [ { "name": "text", "data": "λ" } ] }, { "name": "text", "data": "=" }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599552&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599551&type=", "width": "6.68866634", "height": "6.43466663", "fontsize": "" } } } ] }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599561&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599560&type=", "width": "9.05933285", "height": "3.47133350", "fontsize": "" } } } ] }, { "name": "text", "data": "/" }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599556&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599555&type=", "width": "13.97000027", "height": "6.43466663", "fontsize": "" } } } ] }, { "name": "italic", "data": [ { "name": "text", "data": "=" } ] }, { "name": "text", "data": "957 nm，吸收系数对波长的积分" }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599559&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599557&type=", "width": "4.48733330", "height": "6.43466663", "fontsize": "" } } } ] }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599561&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599560&type=", "width": "9.05933285", "height": "3.47133350", "fontsize": "" } } } ] }, { "name": "text", "data": "=913 cm" }, { "name": "sup", "data": [ { "name": "text", "data": "-1" } ] }, { "name": "text", "data": "·nm。其余光谱参数计算所得的结果如表" }, { "name": "xref", "data": { "text": "3", "type": "table", "rid": "T3", "data": [ { "name": "text", "data": "3" } ] } }, { "name": "text", "data": "~" }, { "name": "xref", "data": { "text": "4", "type": "table", "rid": "T4", "data": [ { "name": "text", "data": "4" } ] } }, { "name": "text", "data": "所示。为了便于比较,表中列出了Yb∶YAG" }, { "name": "sup", "data": [ { "name": "text", "data": "[" }, { "name": "xref", "data": { "text": "57", "type": "bibr", "rid": "R57", "data": [ { "name": "text", "data": "57" } ] } }, { "name": "text", "data": "]" } ] }, { "name": "text", "data": "晶体相应的光谱参数。" } ] }, { "name": "table", "data": { "id": "T3", "caption": [ { "lang": "zh", "label": [ { "name": "text", "data": "表3" } ], "title": [ { "name": "text", "data": "Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3 " } ] }, { "name": "text", "data": "和Yb∶YAG晶体Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "的" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "7/2" } ] }, { "name": "text", "data": "→" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "5/2" } ] }, { "name": "text", "data": "跃迁的吸收谱参数计算结果" } ] }, { "lang": "en", "label": [ { "name": "text", "data": "Tab.3" } ], "title": [ { "name": "text", "data": "Computation results of absorption spectrum parameters of the " }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "7/2" } ] }, { "name": "text", "data": "→" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "5/2" } ] }, { "name": "text", "data": " transition of Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " and Yb∶YAG" } ] } ], "note": [], "table": [ { "head": [ [ { "align": "center", "style": "border-top:solid;border-bottom:solid;", "data": [] }, { "align": "center", "style": "border-top:solid;border-bottom:solid;", "data": [ { "name": "text", "data": "吸收振子强度" }, { "name": "italic", "data": [ { "name": "text", "data": "f" } ] } ] }, { "align": "center", "style": "border-top:solid;border-bottom:solid;", "data": [ { "name": "text", "data": "吸收谱线强度" }, { "name": "italic", "data": [ { "name": "text", "data": "S/" } ] }, { "name": "text", "data": "cm" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] } ] }, { "align": "center", "style": "border-top:solid;border-bottom:solid;", "data": [ { "name": "text", "data": "共振吸收跃迁概率" }, { "name": "italic", "data": [ { "name": "text", "data": "A" } ] }, { "name": "text", "data": "/s" }, { "name": "sup", "data": [ { "name": "text", "data": "-1" } ] } ] } ] ], "body": [ [ { "align": "center", "data": [ { "name": "text", "data": "Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "电偶极子（ED）" } ] }, { "align": "center", "data": [ { "name": "text", "data": "9.050×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-7" } ] } ] }, { "align": "center", "data": [ { "name": "text", "data": "6.240×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-20" } ] } ] }, { "align": "center", "data": [ { "name": "text", "data": "588" } ] } ], [ { "align": "center", "data": [ { "name": "text", "data": "Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "磁偶极子（MD）" } ] }, { "align": "center", "data": [ { "name": "text", "data": "1.811×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-7" } ] } ] }, { "align": "center", "data": [ { "name": "text", "data": "1.278×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-20" } ] } ] }, { "align": "center", "data": [ { "name": "text", "data": "117" } ] } ], [ { "align": "center", "data": [ { "name": "text", "data": "Yb∶YAG电偶极子（ED）" } ] }, { "align": "center", "data": [ { "name": "text", "data": "3.58×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-6" } ] } ] }, { "align": "center", "data": [ { "name": "text", "data": "1.45×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-20" } ] } ] }, { "align": "center", "data": [ { "name": "text", "data": "879" } ] } ], [ { "align": "center", "style": "border-bottom:solid;", "data": [ { "name": "text", "data": 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[ { "name": "text", "data": "-7" } ] } ] }, { "align": "center", "style": "border-bottom:solid;", "data": [ { "name": "text", "data": "1.28×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-21" } ] } ] }, { "align": "center", "style": "border-bottom:solid;", "data": [ { "name": "text", "data": "109" } ] }, { "align": "left", "style": "border-bottom:solid;", "data": [] }, { "align": "left", "style": "border-bottom:solid;", "data": [] } ] ], "foot": [] } ], "graphics": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599565&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599564&type=", "width": "161.18469238", "height": "33.16255951", "fontsize": "" } } }, { "name": "p", "data": [ { "name": "text", "data": "由表中数据可以看到，Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "中Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "的" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "5/2" } ] }, { "name": "text", "data": "→" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "7/2" } ] }, { "name": "text", "data": "跃迁包含了磁偶极子和电偶极子跃迁的贡献，但磁偶极子跃迁比电偶极子跃迁小。" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "5/2" } ] }, { "name": "text", "data": "→" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "7/2" } ] }, { "name": "text", "data": "的总跃迁概率" }, { "name": "italic", "data": [ { "name": "text", "data": "A" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "ed" } ] }, { "name": "text", "data": "+" }, { "name": "italic", "data": [ { "name": "text", "data": " A" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "md" } ] }, { "name": "text", "data": "为941 s" }, { "name": "sup", "data": [ { "name": "text", "data": "-1" } ] }, { "name": "text", "data": "。" } ] }, { "name": "p", "data": [ { "name": "text", "data": "Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "有很强的自吸收，实验准确测定其能级寿命比较困难。而通过吸收光谱计算得到的能级寿命1 063 µs和实验测得的能级寿命1 060 µs非常接近，说明通过吸收光谱计算得到其能级寿命是可行的。Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "在GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "中的能级寿命1 063 µs比Yb∶YAG的950 µs长" }, { "name": "sup", "data": [ { "name": "text", "data": "[" }, { "name": "xref", "data": { "text": "58", "type": "bibr", "rid": "R58", "data": [ { "name": "text", "data": "58" } ] } }, { "name": "text", "data": "]" } ] }, { "name": "text", "data": "，更有利于储能，对于调" }, { "name": "italic", "data": [ { "name": "text", "data": "Q" } ] }, { "name": "text", "data": "激光输出更为有利。Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "作为激光基质更优越。" } ] }, { "name": "p", "data": [ { "name": "text", "data": "初态能级" }, { "name": "italic", "data": [ { "name": "text", "data": "I" } ] }, { "name": "text", "data": "和末态能级" }, { "name": "italic", "data": [ { "name": "text", "data": "F" } ] }, { "name": "text", "data": "之间的跃迁概率" }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599567&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599566&type=", "width": "4.31799984", "height": "3.72533321", "fontsize": "" } } } ] }, { "name": "text", "data": "和发射截面" }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599569&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599568&type=", "width": "4.48733330", "height": "3.72533321", "fontsize": "" } } } ] }, { "name": "text", "data": "之间的关系为" }, { "name": "sup", "data": [ { "name": "text", "data": "[" }, { "name": "xref", "data": { "text": "59", "type": "bibr", "rid": "R59", "data": [ { "name": "text", "data": "59" } ] } }, { "name": "text", "data": "]" } ] } ] }, { "name": "dispformula", "data": { "label": [ { "name": "text", "data": "（9）" } ], "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599571&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599570&type=", "width": "40.63999939", "height": "7.87400007", "fontsize": "" } } }, { "name": "text", "data": "，" } ], "id": "DF9" } }, { "name": "p", "data": [ { "name": "text", "data": "其中" }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599573&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599572&type=", "width": "7.61999989", "height": "3.55599999", "fontsize": "" } } } ] }, { "name": "text", "data": "为发射光谱的线性函数，其量纲为长度量纲的倒数。忽略自吸收，由Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "的发射光谱" }, { "name": "italic", "data": [ { "name": "text", "data": "I" } ] }, { "name": "text", "data": "（" }, { "name": "italic", "data": [ { "name": "text", "data": "λ" } ] }, { "name": "text", "data": "）计算出线性函数：" } ] }, { "name": "dispformula", "data": { "label": [ { "name": "text", "data": "（10）" } ], "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599575&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599574&type=", "width": "26.92399979", "height": "11.34533310", "fontsize": "" } } }, { "name": "text", "data": "，" } ], "id": "DF10" } }, { "name": "p", "data": [ { "name": "text", "data": "如果该公式中波长按nm计算，则需要乘以10" }, { "name": "sup", "data": [ { "name": "text", "data": "-9" } ] }, { "name": "text", "data": "转换为m" }, { "name": "sup", "data": [ { "name": "text", "data": "-1" } ] }, { "name": "text", "data": "。" } ] }, { "name": "p", "data": [ { "name": "text", "data": "计算出的发射截面如" }, { "name": "xref", "data": { "text": "图7", "type": "fig", "rid": "F7", "data": [ { "name": "text", "data": "图7" } ] } }, { "name": "text", "data": "所示。由吸收截面可知， Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "的吸收截面为0.94×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-20 " } ] }, { "name": "text", "data": "cm" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "，在吸收峰965 nm和985 nm处，吸收截面分别为1.477×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-20" } ] }, { "name": "text", "data": " cm" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "和1.482×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-20" } ] }, { "name": "text", "data": " cm" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "，其中985 nm处的吸收截面最大。在987，999，1 029，1 060 nm，发射截面分别为0.476×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-20" } ] }, { "name": "text", "data": "，0.649×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-20" } ] }, { "name": "text", "data": "，0.268×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-20" } ] }, { "name": "text", "data": "，0.233×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-20" } ] }, { "name": "text", "data": " cm" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "，发射截面最大值位于999 nm处。" } ] }, { "name": "p", "data": [ { "name": "text", "data": "在激光中最重要的是增益截面，其计算公式为" }, { "name": "sup", "data": [ { "name": "text", "data": "[" }, { "name": "xref", "data": { "text": "58", "type": "bibr", "rid": "R58", "data": [ { "name": "text", "data": "58" } ] } }, { "name": "text", "data": "]" } ] }, { "name": "text", "data": "：" } ] }, { "name": "dispformula", "data": { "label": [ { "name": "text", "data": "（11）" } ], "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599577&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599576&type=", "width": "40.72467041", "height": "4.14866638", "fontsize": "" } } }, { "name": "text", "data": "，" } ], "id": "DF11" } }, { "name": "p", "data": [ { "name": "text", "data": "其中" }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599585&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599584&type=", "width": "2.28600001", "height": "3.38666677", "fontsize": "" } } } ] }, { "name": "text", "data": "表示处于激发态的粒子占总粒子数的比例。以" }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599585&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599584&type=", "width": "2.28600001", "height": "3.38666677", "fontsize": "" } } } ] }, { "name": "text", "data": "为0.2，0.5，0.8计算出的增益截面如" }, { "name": "xref", "data": { "text": "图8", "type": "fig", "rid": "F8", "data": [ { "name": "text", "data": "图8" } ] } }, { "name": "text", "data": "所示。可以看到，虽然发射截面在999 nm处最大，但直到" }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599585&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599584&type=", "width": "2.28600001", "height": "3.38666677", "fontsize": "" } } } ] }, { "name": "text", "data": "为0.5时，仍然不太可能实现激光输出，因为只有在波长大于1 007.6 nm时，增益截面才大于0，方可实现激光增益放大。在" }, { "name": "inlineformula", "data": [ { "name": "math", "data": { "math": "", "graphicsData": { "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599585&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599584&type=", "width": "2.28600001", "height": "3.38666677", "fontsize": "" } } } ] }, { "name": "text", "data": "为0.8时，较适合激光输出的波段为1 030 nm和1 060 nm。在强泵浦条件下，当激光上能级的粒子数达到80%时，此时999 nm的增益截面才最大，有望实现该波段的激光输出。与Yb∶CaF" }, { "name": "sub", "data": [ { "name": "text", "data": "2" } ] }, { "name": "sup", "data": [ { "name": "text", "data": "[" }, { "name": "xref", "data": { "text": "58", "type": "bibr", "rid": "R58", "data": [ { "name": "text", "data": "58" } ] } }, { "name": "text", "data": "]" } ] }, { "name": "text", "data": "相比，Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "的最大发射截面为0.649×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-20 " } ] }, { "name": "text", "data": "cm" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "（at 999 nm），比Yb∶CaF" }, { "name": "sub", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "（0.24×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-20 " } ] }, { "name": "text", "data": "cm" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": " at 973 nm）大，有利于激光运转。" } ] }, { "name": "fig", "data": { "id": "F8", "caption": [ { "lang": "zh", "label": [ { "name": "text", "data": "图8" } ], "title": [ { "name": "text", "data": "Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶体在不同布居反转比例" }, { "name": "italic", "data": [ { "name": "text", "data": "β" } ] }, { "name": "text", "data": "下的增益截面" } ] }, { "lang": "en", "label": [ { "name": "text", "data": "Fig. 8" } ], "title": [ { "name": "text", "data": "Gain cross sections of Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " crystal at different population inversion ratios " }, { "name": "italic", "data": [ { "name": "text", "data": "β" } ] } ] } ], "subcaption": [], "note": [], "graphics": [ { "print": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599586&type=", "small": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599588&type=", "big": "http://html.publish.founderss.cn/rc-pub/api/common/picture?pictureId=37599587&type=", "width": "75.76123047", "height": "45.86956787", "fontsize": "" } ] } } ] }, { "name": "sec", "data": [ { "name": "sectitle", "data": { "title": [ { "name": "text", "data": "4　结　　论" } ], "level": "1", "id": "s4" } }, { "name": "p", "data": [ { "name": "text", "data": "本文采用Czochralski法生长了Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "单晶，Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "的有效分凝系数计算为1.04。测量了其吸收光谱。测试范围为250～3 000 nm，测试在室温下进行，在880~1 020 nm 范围内，仅有Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "的特征吸收。计算结果表明，掺杂浓度为7.9133×10" }, { "name": "sup", "data": [ { "name": "text", "data": "20" } ] }, { "name": "text", "data": " cm" }, { "name": "sup", "data": [ { "name": "text", "data": "-3 " } ] }, { "name": "text", "data": "的Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "的电偶极子的吸收、发射振子强度为1.086×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-6" } ] }, { "name": "text", "data": "与7.986×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-6" } ] }, { "name": "text", "data": "，吸收、发射跃迁概率为588 s" }, { "name": "sup", "data": [ { "name": "text", "data": "-1" } ] }, { "name": "text", "data": "与784 s" }, { "name": "sup", "data": [ { "name": "text", "data": "-1" } ] }, { "name": "text", "data": "；磁偶极子的吸收、发射振子强度为1.811×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-7" } ] }, { "name": "text", "data": "与1.599×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-6" } ] }, { "name": "text", "data": "，吸收、发射跃迁概率为117 s" }, { "name": "sup", "data": [ { "name": "text", "data": "-1" } ] }, { "name": "text", "data": "与157 s" }, { "name": "sup", "data": [ { "name": "text", "data": "-1" } ] }, { "name": "text", "data": "；" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "F" }, { "name": "sub", "data": [ { "name": "text", "data": "5/2" } ] }, { "name": "text", "data": "能级寿命计算值1 063 µs，和实验测量的能级寿命1 060 µs接近；Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "最高和次高吸收截面位于985 nm和964 nm处，分别为1.482×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-20" } ] }, { "name": "text", "data": " cm" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "和1.480×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-20" } ] }, { "name": "text", "data": " cm" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "。由吸收光谱计算了跃迁线强、振子强度、跃迁概率和上能级寿命，然后给出了Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "的发射和增益截面。Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "的最高发射截面位于999 nm处，为0.649×10" }, { "name": "sup", "data": [ { "name": "text", "data": "-20" } ] }, { "name": "text", "data": " cm" }, { "name": "sup", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "；增益截面计算表明Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "通常适合输出1 030 nm和1 060 nm波段附近的激光，只有在高粒子数反转情况下才可能实现1 000 nm附近的激光输出。" } ] }, { "name": "p", "data": [ { "name": "text", "data": "E‐mail: lijiahong009@126.com" } ] }, { "name": "p", "data": [ { "name": "text", "data": "E‐mail: zql@aiofm.ac.cn" } ] } ] } ], "footnote": [], "reflist": { "title": [ { "name": "text", "data": "参考文献" } ], "data": [ { "id": "R1", "label": "1", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "HOU W T" }, { "name": "text", "data": "， " }, { "name": "text", "data": "ZHAO H Y" }, { "name": "text", "data": "， " }, { "name": "text", "data": "QIN Z P" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Spectroscopic and continuous-wave laser properties of Er∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " crystal at 2.7 µm" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Opt. Mater. Express" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2020" }, { "name": "text", "data": "， " }, { "name": "text", "data": "10" }, { "name": "text", "data": "（" }, { "name": "text", "data": "11" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "2730" }, { "name": "text", "data": "-" }, { "name": "text", "data": "2737" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1364/ome.405683" } ], "href": "http://dx.doi.org/10.1364/ome.405683" } } ], "title": "Spectroscopic and continuous-wave laser properties of Er∶GdScO3 crystal at 2.7 µm" } ] }, { "id": "R2", "label": "2", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "AMANYAN S N" }, { "name": "text", "data": "， " }, { "name": "text", "data": "ARSEN'EV P A" }, { "name": "text", "data": "， " }, { "name": "text", "data": "BAGDASAROV K S" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Synthesis and examination of GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3 " } ] }, { "name": "text", "data": "single crystals activated by Nd" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "J. Appl. Spectrosc." }, { "name": "text", "data": "， " }, { "name": "text", "data": "1983" }, { "name": "text", "data": "， " }, { "name": "text", "data": "38" }, { "name": "text", "data": "（" }, { "name": "text", "data": "3" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "343" }, { "name": "text", "data": "-" }, { "name": "text", "data": "348" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1007/bf00659891" } ], "href": "http://dx.doi.org/10.1007/bf00659891" } } ], "title": "Synthesis and examination of GdScO3 single crystals activated by Nd3+" } ] }, { "id": "R3", "label": "3", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "LI S M" }, { "name": "text", "data": "， " }, { "name": "text", "data": "FANG Q N" }, { "name": "text", "data": "， " }, { "name": "text", "data": "ZHANG Y H" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "2 μm Ultrabroad spectra and laser operation of Tm∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " crystal" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Opt. Laser Technol." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "143" }, { "name": "text", "data": "： " }, { "name": "text", "data": "107345-1" }, { "name": "text", "data": "-" }, { "name": "text", "data": "6" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1016/j.optlastec.2021.107345" } ], "href": "http://dx.doi.org/10.1016/j.optlastec.2021.107345" } } ], "title": "2 μm Ultrabroad spectra and laser operation of Tm∶GdScO3 crystal" } ] }, { "id": "R4", "label": "4", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "PENG F" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LIU W P" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LUO J Q" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Study of growth， defects and thermal and spectroscopic properties of Dy∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3 " } ] }, { "name": "text", "data": "and Dy， Tb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " as promising 578 nm laser crystals" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "CrystEngComm" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2018" }, { "name": "text", "data": "， " }, { "name": "text", "data": "20" }, { "name": "text", "data": "（" }, { "name": "text", "data": "40" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "6291" }, { "name": "text", "data": "-" }, { "name": "text", "data": "6299" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1039/c8ce01254g" } ], "href": "http://dx.doi.org/10.1039/c8ce01254g" } } ], "title": "Study of growth， defects and thermal and spectroscopic properties of Dy∶GdScO3 and Dy， Tb∶GdScO3 as promising 578 nm laser crystals" } ] }, { "id": "R5", "label": "5", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "YAMAJI A" }, { "name": "text", "data": "， " }, { "name": "text", "data": "KOCHURIKHIN V" }, { "name": "text", "data": "， " }, { "name": "text", "data": "FUJIMOTO Y" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Optical properties and radiation response of Ce" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "-doped GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " crystals" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Phys. Status Solidi （c）" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2012" }, { "name": "text", "data": "， " }, { "name": "text", "data": "9" }, { "name": "text", "data": "（" }, { "name": "text", "data": "12" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "2267" }, { "name": "text", "data": "-" }, { "name": "text", "data": "2270" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1002/pssc.201200333" } ], "href": "http://dx.doi.org/10.1002/pssc.201200333" } } ], "title": "Optical properties and radiation response of Ce3+-doped GdScO3 crystals" } ] }, { "id": "R6", "label": "6", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "P N R S" }, { "name": "text", "data": "， " }, { "name": "text", "data": "PANDA D P" }, { "name": "text", "data": "， " }, { "name": "text", "data": "SUNDARESAN A" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Switchable and nonswitchable polarization in doubly ordered perovskites Na" }, { "name": "italic", "data": [ { "name": "text", "data": "Ln" } ] }, { "name": "text", "data": "CoWO" }, { "name": "sub", "data": [ { "name": "text", "data": "6" } ] }, { "name": "text", "data": " （" }, { "name": "italic", "data": [ { "name": "text", "data": "Ln" } ] }, { "name": "text", "data": " = Er， Tm， Yb， and Lu）" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "J. Phys. Chem. C" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "125" }, { "name": "text", "data": "（" }, { "name": "text", "data": "19" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "10803" }, { "name": "text", "data": "-" }, { "name": "text", "data": "10809" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1021/acs.jpcc.1c02316" } ], "href": "http://dx.doi.org/10.1021/acs.jpcc.1c02316" } } ], "title": "Switchable and nonswitchable polarization in doubly ordered perovskites NaLnCoWO6 （Ln = Er， Tm， Yb， and Lu）" } ] }, { "id": "R7", "label": "7", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "赵亚洁" }, { "name": "text", "data": "， " }, { "name": "text", "data": "盛贵章" }, { "name": "text", "data": "， " }, { "name": "text", "data": "郑捷元" }, { "name": "text", "data": "， " }, { "name": "text", "data": "等" }, { "name": "text", "data": ". " }, { "name": "text", "data": "铜基钙钛矿材料及其研究进展" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "新能源进展" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2022" }, { "name": "text", "data": "， " }, { "name": "text", "data": "10" }, { "name": "text", "data": "（" }, { "name": "text", "data": "3" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "233" }, { "name": "text", "data": "-" }, { "name": "text", "data": "243" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.3969/j.issn.2095-560X.2022.03.007" } ], "href": "http://dx.doi.org/10.3969/j.issn.2095-560X.2022.03.007" } } ], "title": "铜基钙钛矿材料及其研究进展" }, { "lang": "en", "text": [ { "name": "text", "data": "ZHAO Y J" }, { "name": "text", "data": "， " }, { "name": "text", "data": "SHENG G Z" }, { "name": "text", "data": "， " }, { "name": "text", "data": "ZHENG J Y" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Research progress on copper-based perovskite materials" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Adv. New Renew. Energy" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2022" }, { "name": "text", "data": "， " }, { "name": "text", "data": "10" }, { "name": "text", "data": "（" }, { "name": "text", "data": "3" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "233" }, { "name": "text", "data": "-" }, { "name": "text", "data": "243" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.3969/j.issn.2095-560X.2022.03.007" } ], "href": "http://dx.doi.org/10.3969/j.issn.2095-560X.2022.03.007" } } ], "title": "Research progress on copper-based perovskite materials" } ] }, { "id": "R8", "label": "8", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "MANSLEY Z R" }, { "name": "text", "data": "， " }, { "name": "text", "data": "MIZZI C A" }, { "name": "text", "data": "， " }, { "name": "text", "data": "KOIRALA P" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Structure of the （110） " }, { "name": "italic", "data": [ { "name": "text", "data": "Ln" } ] }, { "name": "text", "data": "ScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3 " } ] }, { "name": "text", "data": "（" }, { "name": "italic", "data": [ { "name": "text", "data": "Ln" } ] }, { "name": "text", "data": "=Gd， Tb， Dy） surfaces" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Phys. Rev. Mater." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2020" }, { "name": "text", "data": "， " }, { "name": "text", "data": "4" }, { "name": "text", "data": "（" }, { "name": "text", "data": "4" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "045003-1-6" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1103/physrevmaterials.4.045003" } ], "href": "http://dx.doi.org/10.1103/physrevmaterials.4.045003" } } ], "title": "Structure of the （110） LnScO3 （Ln=Gd， Tb， Dy） surfaces" } ] }, { "id": "R9", "label": "9", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "SHENG J M" }, { "name": "text", "data": "， " }, { "name": "text", "data": "KAN X C" }, { "name": "text", "data": "， " }, { "name": "text", "data": "GE H" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Low temperature magnetism in the rare-earth perovskite GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Chin. Phys. B" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2020" }, { "name": "text", "data": "， " }, { "name": "text", "data": "29" }, { "name": "text", "data": "（" }, { "name": "text", "data": "5" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "057503-1-5" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1088/1674-1056/ab8200" } ], "href": "http://dx.doi.org/10.1088/1674-1056/ab8200" } } ], "title": "Low temperature magnetism in the rare-earth perovskite GdScO3" } ] }, { "id": "R10", "label": "10", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "WANG D H" }, { "name": "text", "data": "， " }, { "name": "text", "data": "HOU W T" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LI N" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Growth， spectroscopic properties and crystal field analysis of Cr" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": " doped GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " crystal" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Opt. Mater. Express" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2019" }, { "name": "text", "data": "， " }, { "name": "text", "data": "9" }, { "name": "text", "data": "（" }, { "name": "text", "data": "11" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "4218" }, { "name": "text", "data": "-" }, { "name": "text", "data": "4227" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1364/ome.9.004218" } ], "href": "http://dx.doi.org/10.1364/ome.9.004218" } } ], "title": "Growth， spectroscopic properties and crystal field analysis of Cr3+ doped GdScO3 crystal" } ] }, { "id": "R11", "label": "11", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "周慧丽" }, { "name": "text", "data": "， " }, { "name": "text", "data": "吴锋" }, { "name": "text", "data": "， " }, { "name": "text", "data": "张志宏" }, { "name": "text", "data": "， " }, { "name": "text", "data": "等" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Lu" }, { "name": "sub", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "O" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "∶Er" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "/Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "荧光材料的上转换发光及其温度传感特性" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "发光学报" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2022" }, { "name": "text", "data": "， " }, { "name": "text", "data": "43" }, { "name": "text", "data": "（" }, { "name": "text", "data": "2" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "192" }, { "name": "text", "data": "-" }, { "name": "text", "data": "200" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/cjl.20210363" } ], "href": "http://dx.doi.org/10.37188/cjl.20210363" } } ], "title": "Lu2O3∶Er3+/Yb3+荧光材料的上转换发光及其温度传感特性" }, { "lang": "en", "text": [ { "name": "text", "data": "ZHOU H L" }, { "name": "text", "data": "， " }, { "name": "text", "data": "WU F" }, { "name": "text", "data": "， " }, { "name": "text", "data": "ZHANG Z H" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Upconversion luminescence and temperature sensing characteristics of Lu" }, { "name": "sub", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "O" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "∶Er" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "/Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": " phosphor" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Chin. J. Lumin." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2022" }, { "name": "text", "data": "， " }, { "name": "text", "data": "43" }, { "name": "text", "data": "（" }, { "name": "text", "data": "2" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "192" }, { "name": "text", "data": "-" }, { "name": "text", "data": "200" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/cjl.20210363" } ], "href": "http://dx.doi.org/10.37188/cjl.20210363" } } ], "title": "Upconversion luminescence and temperature sensing characteristics of Lu2O3∶Er3+/Yb3+ phosphor" } ] }, { "id": "R12", "label": "12", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "张志宏" }, { "name": "text", "data": "， " }, { "name": "text", "data": "周慧丽" }, { "name": "text", "data": "， " }, { "name": "text", "data": "吴锋" }, { "name": "text", "data": "， " }, { "name": "text", "data": "等" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Tm" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "/Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "共掺LuYO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "上转换荧光温度传感特性" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "发光学报" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "42" }, { "name": "text", "data": "（" }, { "name": "text", "data": "12" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "1872" }, { "name": "text", "data": "-" }, { "name": "text", "data": "1881" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/cjl.20210276" } ], "href": "http://dx.doi.org/10.37188/cjl.20210276" } } ], "title": "Tm3+/Yb3+共掺LuYO3上转换荧光温度传感特性" }, { "lang": "en", "text": [ { "name": "text", "data": "ZHANG Z H" }, { "name": "text", "data": "， " }, { "name": "text", "data": "ZHOU H L" }, { "name": "text", "data": "， " }, { "name": "text", "data": "WU F" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Temperature sensing characteristics of up-conversion luminescence in Tm" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "/Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+ " } ] }, { "name": "text", "data": "Co-doped LuYO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " phosphor" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Chin. J. Lumin." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "42" }, { "name": "text", "data": "（" }, { "name": "text", "data": "12" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "1872" }, { "name": "text", "data": "-" }, { "name": "text", "data": "1881" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/cjl.20210276" } ], "href": "http://dx.doi.org/10.37188/cjl.20210276" } } ], "title": "Temperature sensing characteristics of up-conversion luminescence in Tm3+/Yb3+ Co-doped LuYO3 phosphor" } ] }, { "id": "R13", "label": "13", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "JIA J H" }, { "name": "text", "data": "， " }, { "name": "text", "data": "KE Y J" }, { "name": "text", "data": "， " }, { "name": "text", "data": "ZHANG X X" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Giant magnetocaloric effect in the antiferromagnet GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " single crystal" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "J. Alloys Compd." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2019" }, { "name": "text", "data": "， " }, { "name": "text", "data": "803" }, { "name": "text", "data": "： " }, { "name": "text", "data": "992" }, { "name": "text", "data": "-" }, { "name": "text", "data": "997" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1016/j.jallcom.2019.06.361" } ], "href": "http://dx.doi.org/10.1016/j.jallcom.2019.06.361" } } ], "title": "Giant magnetocaloric effect in the antiferromagnet GdScO3 single crystal" } ] }, { "id": "R14", "label": "14", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "YAN W L" }, { "name": "text", "data": "， " }, { "name": "text", "data": "SUN Y J" }, { "name": "text", "data": "， " }, { "name": "text", "data": "WANG Z Y" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Growth and spectroscopic analyses of Yb， Ho∶CaYAlO" }, { "name": "sub", "data": [ { "name": "text", "data": "4" } ] }, { "name": "text", "data": " disordered crystal for ~3 μm mid-infrared laser" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "J. Lumin." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "236" }, { "name": "text", "data": "： " }, { "name": "text", "data": "118067" }, { "name": "text", "data": "." } ], "title": "Growth and spectroscopic analyses of Yb， Ho∶CaYAlO4 disordered crystal for ~3 μm mid-infrared laser" } ] }, { "id": "R15", "label": "15", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "WANG X L" }, { "name": "text", "data": "， " }, { "name": "text", "data": "WANG X J" }, { "name": "text", "data": "， " }, { "name": "text", "data": "DONG J" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Sub-nanosecond， high peak power Yb∶YAG/Cr" }, { "name": "sup", "data": [ { "name": "text", "data": "4+" } ] }, { "name": "text", "data": "∶YAG/YVO" }, { "name": "sub", "data": [ { "name": "text", "data": "4" } ] }, { "name": "text", "data": " passively " }, { "name": "italic", "data": [ { "name": "text", "data": "Q" } ] }, { "name": "text", "data": "-switched Raman micro-laser operating at 1134 nm" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "J. Lumin." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "234" }, { "name": "text", "data": "： " }, { "name": "text", "data": "117955" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1016/j.jlumin.2021.117955" } ], "href": "http://dx.doi.org/10.1016/j.jlumin.2021.117955" } } ], "title": "Sub-nanosecond， high peak power Yb∶YAG/Cr4+∶YAG/YVO4 passively Q-switched Raman micro-laser operating at 1134 nm" } ] }, { "id": "R16", "label": "16", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "LIANG H Z" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LEI W C" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LIU S X" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Color tunable up-conversion luminescence characteristics of Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "-Er" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "-Tm" }, { "name": "sup", "data": [ { "name": "text", "data": "3+ " } ] }, { "name": "text", "data": " tri-doped fluorosilicate glass potentially used in WLED field" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Opt. Mater." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "119" }, { "name": "text", "data": "： " }, { "name": "text", "data": "111320-1" }, { "name": "text", "data": "-" }, { "name": "text", "data": "8" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1016/j.optmat.2021.111320" } ], "href": "http://dx.doi.org/10.1016/j.optmat.2021.111320" } } ], "title": "Color tunable up-conversion luminescence characteristics of Yb3+-Er3+-Tm3+ tri-doped fluorosilicate glass potentially used in WLED field" } ] }, { "id": "R17", "label": "17", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "WANG H" }, { "name": "text", "data": "， " }, { "name": "text", "data": "PANG T" }, { "name": "text", "data": "， " }, { "name": "text", "data": "TIAN Y" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Brightness attenuation mechanisms of Er" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": " self-sensitized upconversion nanocrystals under 1.5 μm pumping" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Appl. Surf. Sci." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "538" }, { "name": "text", "data": "： " }, { "name": "text", "data": "148084-1" }, { "name": "text", "data": "-" }, { "name": "text", "data": "9" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1016/j.apsusc.2020.148084" } ], "href": "http://dx.doi.org/10.1016/j.apsusc.2020.148084" } } ], "title": "Brightness attenuation mechanisms of Er3+ self-sensitized upconversion nanocrystals under 1.5 μm pumping" } ] }, { "id": "R18", "label": "18", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "DAI Y" }, { "name": "text", "data": "， " }, { "name": "text", "data": "ZHANG Z H" }, { "name": "text", "data": "， " }, { "name": "text", "data": "SU L B" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Growth of high-quality Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "-doped Y" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "Al" }, { "name": "sub", "data": [ { "name": "text", "data": "5" } ] }, { "name": "text", "data": "O" }, { "name": "sub", "data": [ { "name": "text", "data": "12" } ] }, { "name": "text", "data": " single crystal fiber by laser heated pedestal growth method" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "J. Inorg. Mater." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "36" }, { "name": "text", "data": "（" }, { "name": "text", "data": "7" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "761" }, { "name": "text", "data": "-" }, { "name": "text", "data": "765" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.15541/jim20200475" } ], "href": "http://dx.doi.org/10.15541/jim20200475" } } ], "title": "Growth of high-quality Yb3+-doped Y3Al5O12 single crystal fiber by laser heated pedestal growth method" } ] }, { "id": "R19", "label": "19", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "邬金闽" }, { "name": "text", "data": "， " }, { "name": "text", "data": "黄得财" }, { "name": "text", "data": "， " }, { "name": "text", "data": "梁思思" }, { "name": "text", "data": "， " }, { "name": "text", "data": "等" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Cr" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "、Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "共掺杂LaSc" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "（BO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "）" }, { "name": "sub", "data": [ { "name": "text", "data": "4" } ] }, { "name": "text", "data": "近红外荧光粉的发光与器件性能" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "发光学报" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "42" }, { "name": "text", "data": "（" }, { "name": "text", "data": "6" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "793" }, { "name": "text", "data": "-" }, { "name": "text", "data": "803" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/CJL.20210066" } ], "href": "http://dx.doi.org/10.37188/CJL.20210066" } } ], "title": "Cr3+、Yb3+共掺杂LaSc3（BO3）4近红外荧光粉的发光与器件性能" }, { "lang": "en", "text": [ { "name": "text", "data": "WU J M" }, { "name": "text", "data": "， " }, { "name": "text", "data": "HUANG D C" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LIANG S S" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Photoluminescence properties and device performance of Cr" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "， Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+ " } ] }, { "name": "text", "data": "co-doped LaSc" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "（BO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "）" }, { "name": "sub", "data": [ { "name": "text", "data": "4" } ] }, { "name": "text", "data": " near infrared phosphors" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Chin. J. Lumin." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "42" }, { "name": "text", "data": "（" }, { "name": "text", "data": "6" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "793" }, { "name": "text", "data": "-" }, { "name": "text", "data": "803" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/CJL.20210066" } ], "href": "http://dx.doi.org/10.37188/CJL.20210066" } } ], "title": "Photoluminescence properties and device performance of Cr3+， Yb3+ co-doped LaSc3（BO3）4 near infrared phosphors" } ] }, { "id": "R20", "label": "20", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "LENGYEL K" }, { "name": "text", "data": "， " }, { "name": "text", "data": "TICHY-RÁCS É" }, { "name": "text", "data": "， " }, { "name": "text", "data": "TIMPMANN K" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Cooperative luminescence of Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": " ion pairs in Li" }, { "name": "sub", "data": [ { "name": "text", "data": "6" } ] }, { "name": "text", "data": "Y（BO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "）" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "∶Yb single crystals" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "J. Lumin." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "230" }, { "name": "text", "data": "： " }, { "name": "text", "data": "117732-1" }, { "name": "text", "data": "-" }, { "name": "text", "data": "9" }, { "name": "text", "data": "." } ], "title": "Cooperative luminescence of Yb3+ ion pairs in Li6Y（BO3）3∶Yb single crystals" } ] }, { "id": "R21", "label": "21", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "PAUL DAVID S" }, { "name": "text", "data": "， " }, { "name": "text", "data": "JAMBUNATHAN V" }, { "name": "text", "data": "， " }, { "name": "text", "data": "YUE F X" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Diode pumped cryogenic Yb∶Lu" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "Al" }, { "name": "sub", "data": [ { "name": "text", "data": "5" } ] }, { "name": "text", "data": "O" }, { "name": "sub", "data": [ { "name": "text", "data": "12" } ] }, { "name": "text", "data": " laser in continuous-wave and pulsed regime" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Opt. Laser Technol." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "135" }, { "name": "text", "data": "： " }, { "name": "text", "data": "106720" }, { "name": "text", "data": "." } ], "title": "Diode pumped cryogenic Yb∶Lu3Al5O12 laser in continuous-wave and pulsed regime" } ] }, { "id": "R22", "label": "22", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "PETROV V A" }, { "name": "text", "data": "， " }, { "name": "text", "data": "PETROV V V" }, { "name": "text", "data": "， " }, { "name": "text", "data": "KUPTSOV G V" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "YAG∶Yb crystal with non-linear doping ions distribution as promising active element for high average power laser systems" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Laser Phys." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "31" }, { "name": "text", "data": "（" }, { "name": "text", "data": "3" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "035003-1-6" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1088/1555-6611/abe235" } ], "href": "http://dx.doi.org/10.1088/1555-6611/abe235" } } ], "title": "YAG∶Yb crystal with non-linear doping ions distribution as promising active element for high average power laser systems" } ] }, { "id": "R23", "label": "23", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "金叶" }, { "name": "text", "data": "， " }, { "name": "text", "data": "李坤" }, { "name": "text", "data": "， " }, { "name": "text", "data": "罗旭" }, { "name": "text", "data": "， " }, { "name": "text", "data": "等" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Sc" }, { "name": "sub", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "（WO" }, { "name": "sub", "data": [ { "name": "text", "data": "4" } ] }, { "name": "text", "data": "）" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "∶Er" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "/Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "的上转换发光及其温度传感特性" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "发光学报" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "42" }, { "name": "text", "data": "（" }, { "name": "text", "data": "1" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "91" }, { "name": "text", "data": "-" }, { "name": "text", "data": "97" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/cjl.20200326" } ], "href": "http://dx.doi.org/10.37188/cjl.20200326" } } ], "title": "Sc2（WO4）3∶Er3+/Yb3+的上转换发光及其温度传感特性" }, { "lang": "en", "text": [ { "name": "text", "data": "JIN Y" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LI K" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LUO X" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Upconversion luminescence and temperature sensing properties for Sc" }, { "name": "sub", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "（WO" }, { "name": "sub", "data": [ { "name": "text", "data": "4" } ] }, { "name": "text", "data": "）" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "∶Er" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "/Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Chin. J. Lumin." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "42" }, { "name": "text", "data": "（" }, { "name": "text", "data": "1" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "91" }, { "name": "text", "data": "-" }, { "name": "text", "data": "97" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/cjl.20200326" } ], "href": "http://dx.doi.org/10.37188/cjl.20200326" } } ], "title": "Upconversion luminescence and temperature sensing properties for Sc2（WO4）3∶Er3+/Yb3+" } ] }, { "id": "R24", "label": "24", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "何旭" }, { "name": "text", "data": "， " }, { "name": "text", "data": "吴亚楠" }, { "name": "text", "data": "， " }, { "name": "text", "data": "蒋越宁" }, { "name": "text", "data": "， " }, { "name": "text", "data": "等" }, { "name": "text", "data": ". " }, { "name": "text", "data": "适用于近红外荧光/核磁双模成像的GdF" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "∶Nd" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "，Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "@NaGdF" }, { "name": "sub", "data": [ { "name": "text", "data": "4" } ] }, { "name": "text", "data": "纳米材料" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "发光学报" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2022" }, { "name": "text", "data": "， " }, { "name": "text", "data": "43" }, { "name": "text", "data": "（" }, { "name": "text", "data": "3" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "350" }, { "name": "text", "data": "-" }, { "name": "text", "data": "358" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/cjl.20210391" } ], "href": "http://dx.doi.org/10.37188/cjl.20210391" } } ], "title": "适用于近红外荧光/核磁双模成像的GdF3∶Nd3+，Yb3+@NaGdF4纳米材料" }, { "lang": "en", "text": [ { "name": "text", "data": "HE X" }, { "name": "text", "data": "， " }, { "name": "text", "data": "WU Y N" }, { "name": "text", "data": "， " }, { "name": "text", "data": "JIANG Y N" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "GdF" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "∶Nd" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "，Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "@NaGdF" }, { "name": "sub", "data": [ { "name": "text", "data": "4" } ] }, { "name": "text", "data": " nanomaterials for near infrared fluorescence and magnetic resonance dual-mode imaging" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Chin. J. Lumin." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2022" }, { "name": "text", "data": "， " }, { "name": "text", "data": "43" }, { "name": "text", "data": "（" }, { "name": "text", "data": "3" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "350" }, { "name": "text", "data": "-" }, { "name": "text", "data": "358" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/cjl.20210391" } ], "href": "http://dx.doi.org/10.37188/cjl.20210391" } } ], "title": "GdF3∶Nd3+，Yb3+@NaGdF4 nanomaterials for near infrared fluorescence and magnetic resonance dual-mode imaging" } ] }, { "id": "R25", "label": "25", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "杨洁" }, { "name": "text", "data": "， " }, { "name": "text", "data": "赵建斌" }, { "name": "text", "data": "， " }, { "name": "text", "data": "刘乂尹" }, { "name": "text", "data": "， " }, { "name": "text", "data": "等" }, { "name": "text", "data": ". " }, { "name": "text", "data": "镱钠共掺氟化钙锶混晶近红外光谱与激光参数" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "发光学报" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2022" }, { "name": "text", "data": "， " }, { "name": "text", "data": "43" }, { "name": "text", "data": "（" }, { "name": "text", "data": "3" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "341" }, { "name": "text", "data": "-" }, { "name": "text", "data": "349" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/cjl.20210358" } ], "href": "http://dx.doi.org/10.37188/cjl.20210358" } } ], "title": "镱钠共掺氟化钙锶混晶近红外光谱与激光参数" }, { "lang": "en", "text": [ { "name": "text", "data": "YANG J" }, { "name": "text", "data": "， " }, { "name": "text", "data": "ZHAO J B" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LIU Y Y" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Near-infrared spectra and laser parameters of Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": " and Na" }, { "name": "sup", "data": [ { "name": "text", "data": "+ " } ] }, { "name": "text", "data": "codoped CaF" }, { "name": "sub", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "-SrF" }, { "name": "sub", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": " crystal" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Chin. J. Lumin." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2022" }, { "name": "text", "data": "， " }, { "name": "text", "data": "43" }, { "name": "text", "data": "（" }, { "name": "text", "data": "3" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "341" }, { "name": "text", "data": "-" }, { "name": "text", "data": "349" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/cjl.20210358" } ], "href": "http://dx.doi.org/10.37188/cjl.20210358" } } ], "title": "Near-infrared spectra and laser parameters of Yb3+ and Na+ codoped CaF2-SrF2 crystal" } ] }, { "id": "R26", "label": "26", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "宁凯杰" }, { "name": "text", "data": "， " }, { "name": "text", "data": "张庆礼" }, { "name": "text", "data": "， " }, { "name": "text", "data": "周鹏宇" }, { "name": "text", "data": "， " }, { "name": "text", "data": "等" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "∶Gd" }, { "name": "sub", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "SiO" }, { "name": "sub", "data": [ { "name": "text", "data": "5" } ] }, { "name": "text", "data": "晶体的结构和光谱性能" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "物理学报" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2012" }, { "name": "text", "data": "， " }, { "name": "text", "data": "61" }, { "name": "text", "data": "（" }, { "name": "text", "data": "12" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "128102-1-8" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.7498/aps.61.128102" } ], "href": "http://dx.doi.org/10.7498/aps.61.128102" } } ], "title": "Yb3+∶Gd2SiO5晶体的结构和光谱性能" }, { "lang": "en", "text": [ { "name": "text", "data": "NING K J" }, { "name": "text", "data": "， " }, { "name": "text", "data": "ZHANG Q L" }, { "name": "text", "data": "， " }, { "name": "text", "data": "ZHOU P Y" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Structure and spectral properties of Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "∶Gd" }, { "name": "sub", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "SiO" }, { "name": "sub", "data": [ { "name": "text", "data": "5" } ] }, { "name": "text", "data": " crystal" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Acta Phys. Sinica" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2012" }, { "name": "text", "data": "， " }, { "name": "text", "data": "61" }, { "name": "text", "data": "（" }, { "name": "text", "data": "12" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "128102-1-8" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.7498/aps.61.128102" } ], "href": "http://dx.doi.org/10.7498/aps.61.128102" } } ], "title": "Structure and spectral properties of Yb3+∶Gd2SiO5 crystal" } ] }, { "id": "R27", "label": "27", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "STEPHEN S K" }, { "name": "text", "data": "， " }, { "name": "text", "data": "VARGHESE T" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Effect of Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": " substitution on the structural and optical properties of Ba" }, { "name": "sub", "data": [ { "name": "text", "data": "1-" } ] }, { "name": "italic", "data": [ { "name": "sub", "data": [ { "name": "text", "data": "x" } ] } ] }, { "name": "text", "data": "Yb" }, { "name": "italic", "data": [ { "name": "sub", "data": [ { "name": "text", "data": "x" } ] } ] }, { "name": "text", "data": "WO" }, { "name": "sub", "data": [ { "name": "text", "data": "4" } ] }, { "name": "text", "data": " nanoparticles-NIR luminescence emissions for optical communication and bioanalyses" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Mater. Charact." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "174" }, { "name": "text", "data": "： " }, { "name": "text", "data": "110985" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1016/j.matchar.2021.110985" } ], "href": "http://dx.doi.org/10.1016/j.matchar.2021.110985" } } ], "title": "Effect of Yb3+ substitution on the structural and optical properties of Ba1-xYbxWO4 nanoparticles-NIR luminescence emissions for optical communication and bioanalyses" } ] }, { "id": "R28", "label": "28", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "WANG W" }, { "name": "text", "data": "， " }, { "name": "text", "data": "JIANG B X" }, { "name": "text", "data": "， " }, { "name": "text", "data": "FENG T" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Broadening emission band of Yb∶LuScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " transparent ceramics for ultrashort pulse laser" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "J. Am. Ceram Soc." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "104" }, { "name": "text", "data": "（" }, { "name": "text", "data": "11" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "6064" }, { "name": "text", "data": "-" }, { "name": "text", "data": "6073" }, { "name": "text", "data": "." } ], "title": "Broadening emission band of Yb∶LuScO3 transparent ceramics for ultrashort pulse laser" } ] }, { "id": "R29", "label": "29", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "LIU Z Y" }, { "name": "text", "data": "， " }, { "name": "text", "data": "TOCI G" }, { "name": "text", "data": "， " }, { "name": "text", "data": "PIRRI A" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Fabrication， microstructures， and optical properties of Yb∶Lu" }, { "name": "sub", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "O" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " laser ceramics from co-precipitated nano-powders" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "J. Adv. Ceram." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2020" }, { "name": "text", "data": "， " }, { "name": "text", "data": "9" }, { "name": "text", "data": "（" }, { "name": "text", "data": "6" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "674" }, { "name": "text", "data": "-" }, { "name": "text", "data": "682" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1007/s40145-020-0403-8" } ], "href": "http://dx.doi.org/10.1007/s40145-020-0403-8" } } ], "title": "Fabrication， microstructures， and optical properties of Yb∶Lu2O3 laser ceramics from co-precipitated nano-powders" } ] }, { "id": "R30", "label": "30", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "SOHARAB M" }, { "name": "text", "data": "， " }, { "name": "text", "data": "BHAUMIK I" }, { "name": "text", "data": "， " }, { "name": "text", "data": "BHATT R" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Investigation of optical and spectroscopic properties of Nd co-doped Yb∶YVO" }, { "name": "sub", "data": [ { "name": "text", "data": "4" } ] }, { "name": "text", "data": " single crystals grown by OFZ method" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "J. Lumin." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "231" }, { "name": "text", "data": "： " }, { "name": "text", "data": "117736" }, { "name": "text", "data": "." } ], "title": "Investigation of optical and spectroscopic properties of Nd co-doped Yb∶YVO4 single crystals grown by OFZ method" } ] }, { "id": "R31", "label": "31", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "MA J" }, { "name": "text", "data": "， " }, { "name": "text", "data": "YANG F" }, { "name": "text", "data": "， " }, { "name": "text", "data": "GAO W L" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Sub-five-optical-cycle pulse generation from a Kerr-lens mode-locked Yb∶CaYAlO" }, { "name": "sub", "data": [ { "name": "text", "data": "4" } ] }, { "name": "text", "data": " laser" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Opt. Lett." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "46" }, { "name": "text", "data": "（" }, { "name": "text", "data": "10" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "2328" }, { "name": "text", "data": "-" }, { "name": "text", "data": "2331" }, { "name": "text", "data": "." } ], "title": "Sub-five-optical-cycle pulse generation from a Kerr-lens mode-locked Yb∶CaYAlO4 laser" } ] }, { "id": "R32", "label": "32", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "DEMIRBAS U" }, { "name": "text", "data": "， " }, { "name": "text", "data": "KELLERT M" }, { "name": "text", "data": "， " }, { "name": "text", "data": "THESINGA J" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Comparative investigation of lasing and amplification performance in cryogenic Yb∶YLF systems" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Appl. Phys. B" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "127" }, { "name": "text", "data": "（" }, { "name": "text", "data": "3" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "46-1-10" }, { "name": "text", "data": "." } ], "title": "Comparative investigation of lasing and amplification performance in cryogenic Yb∶YLF systems" } ] }, { "id": "R33", "label": "33", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "CHEN J X" }, { "name": "text", "data": "， " }, { "name": "text", "data": "DONG L" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LIU F F" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Investigation of Yb∶CaWO" }, { "name": "sub", "data": [ { "name": "text", "data": "4" } ] }, { "name": "text", "data": " as a potential new self-Raman laser crystal" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Cryst‐EngComm" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "23" }, { "name": "text", "data": "（" }, { "name": "text", "data": "2" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "427" }, { "name": "text", "data": "-" }, { "name": "text", "data": "435" }, { "name": "text", "data": "." } ], "title": "Investigation of Yb∶CaWO4 as a potential new self-Raman laser crystal" } ] }, { "id": "R34", "label": "34", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "ZHAO Y Q" }, { "name": "text", "data": "， " }, { "name": "text", "data": "WANG Q G" }, { "name": "text", "data": "， " }, { "name": "text", "data": "MENG L H" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Anisotropy of the thermal and laser output properties in Yb， Nd∶Sc" }, { "name": "sub", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "SiO" }, { "name": "sub", "data": [ { "name": "text", "data": "5" } ] }, { "name": "text", "data": " crystal" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Chin. Opt. Lett." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "19" }, { "name": "text", "data": "（" }, { "name": "text", "data": "4" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "041405-1-5" }, { "name": "text", "data": "." } ], "title": "Anisotropy of the thermal and laser output properties in Yb， Nd∶Sc2SiO5 crystal" } ] }, { "id": "R35", "label": "35", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "VOLOKITINA A" }, { "name": "text", "data": "， " }, { "name": "text", "data": "DAVID S P" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LOIKO P" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Monoclinic zinc monotungstate Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "， Li" }, { "name": "sup", "data": [ { "name": "text", "data": "+" } ] }, { "name": "text", "data": "∶ZnWO" }, { "name": "sub", "data": [ { "name": "text", "data": "4" } ] }, { "name": "text", "data": "∶ Part Ⅱ. Polarized spectroscopy and laser operation" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "J. Lumin." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "231" }, { "name": "text", "data": "： " }, { "name": "text", "data": "117811" }, { "name": "text", "data": "." } ], "title": "Monoclinic zinc monotungstate Yb3+， Li+∶ZnWO4∶ Part Ⅱ. Polarized spectroscopy and laser operation" } ] }, { "id": "R36", "label": "36", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "JIANG B B" }, { "name": "text", "data": "， " }, { "name": "text", "data": "ZHENG L H" }, { "name": "text", "data": "， " }, { "name": "text", "data": "JIANG D P" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Growth and optical properties of ytterbium and rare earth ions codoped CaF" }, { "name": "sub", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "-SrF" }, { "name": "sub", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": " eutectic solid-solution （" }, { "name": "italic", "data": [ { "name": "text", "data": "RE" } ] }, { "name": "text", "data": " = Y" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "， Gd" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "， La" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "）" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "J. Rare Earths" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "39" }, { "name": "text", "data": "（" }, { "name": "text", "data": "4" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "390" }, { "name": "text", "data": "-" }, { "name": "text", "data": "397" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1016/j.jre.2020.08.001" } ], "href": "http://dx.doi.org/10.1016/j.jre.2020.08.001" } } ], "title": "Growth and optical properties of ytterbium and rare earth ions codoped CaF2-SrF2 eutectic solid-solution （RE = Y3+， Gd3+， La3+）" } ] }, { "id": "R37", "label": "37", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "BASYROVA L" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LOIKO P" }, { "name": "text", "data": "， " }, { "name": "text", "data": "MAKSIMOV R" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Comparative study of Yb∶Lu" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "Al" }, { "name": "sub", "data": [ { "name": "text", "data": "5" } ] }, { "name": "text", "data": "O" }, { "name": "sub", "data": [ { "name": "text", "data": "12" } ] }, { "name": "text", "data": " and Yb∶Lu" }, { "name": "sub", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "O" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " laser ceramics produced from laser-ablated nanopowders" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Ceram. Int." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "47" }, { "name": "text", "data": "（" }, { "name": "text", "data": "5" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "6633" }, { "name": "text", "data": "-" }, { "name": "text", "data": "6642" }, { "name": "text", "data": "." } ], "title": "Comparative study of Yb∶Lu3Al5O12 and Yb∶Lu2O3 laser ceramics produced from laser-ablated nanopowders" } ] }, { "id": "R38", "label": "38", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "李加红" }, { "name": "text", "data": "， " }, { "name": "text", "data": "孙贵花" }, { "name": "text", "data": "， " }, { "name": "text", "data": "张庆礼" }, { "name": "text", "data": "， " }, { "name": "text", "data": "等" }, { "name": "text", "data": ". " }, { "name": "text", "data": "退火气氛对GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "和Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶体的结构和光谱性质的影响" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "物理学报" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2022" }, { "name": "text", "data": "， " }, { "name": "text", "data": "71" }, { "name": "text", "data": "（" }, { "name": "text", "data": "16" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "164206-1-7" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.7498/aps.71.20220196" } ], "href": "http://dx.doi.org/10.7498/aps.71.20220196" } } ], "title": "退火气氛对GdScO3和Yb∶GdScO3晶体的结构和光谱性质的影响" }, { "lang": "en", "text": [ { "name": "text", "data": "LI J H" }, { "name": "text", "data": "， " }, { "name": "text", "data": "SUN G H" }, { "name": "text", "data": "， " }, { "name": "text", "data": "ZHANG Q L" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Effect of annealing atmosphere on the structure and spectral properties of GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " and Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " crystals" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Acta Phys. Sinica" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2022" }, { "name": "text", "data": "， " }, { "name": "text", "data": "71" }, { "name": "text", "data": "（" }, { "name": "text", "data": "16" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "164206-1-7" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.7498/aps.71.20220196" } ], "href": "http://dx.doi.org/10.7498/aps.71.20220196" } } ], "title": "Effect of annealing atmosphere on the structure and spectral properties of GdScO3 and Yb∶GdScO3 crystals" } ] }, { "id": "R39", "label": "39", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "WANG A Y" }, { "name": "text", "data": "， " }, { "name": "text", "data": "ZHANG J" }, { "name": "text", "data": "， " }, { "name": "text", "data": "YE S" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Optimized growth and laser application of Yb∶LuAG single-crystal fibers by micro-pulling-down technique" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Crystals" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "11" }, { "name": "text", "data": "（" }, { "name": "text", "data": "2" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "78-1-10" }, { "name": "text", "data": "." } ], "title": "Optimized growth and laser application of Yb∶LuAG single-crystal fibers by micro-pulling-down technique" } ] }, { "id": "R40", "label": "40", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "PAN Y X" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LIN H" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LIU J" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Fabrication and spectral properties of Yb， Ho∶Y" }, { "name": "sub", "data": [ { "name": "text", "data": "2" } ] }, { "name": "text", "data": "O" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " transparent ceramics" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Opt. Mater." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "112" }, { "name": "text", "data": "： " }, { "name": "text", "data": "110479-1" }, { "name": "text", "data": "-" }, { "name": "text", "data": "6" }, { "name": "text", "data": "." } ], "title": "Fabrication and spectral properties of Yb， Ho∶Y2O3 transparent ceramics" } ] }, { "id": "R41", "label": "41", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "ZENG H J" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LIN H F" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LIN Z L" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Diode-pumped sub-50-fs Kerr-lens mode-locked Yb∶GdYCOB laser" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Opt. Express" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "29" }, { "name": "text", "data": "（" }, { "name": "text", "data": "9" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "13496" }, { "name": "text", "data": "-" }, { "name": "text", "data": "13503" }, { "name": "text", "data": "." } ], "title": "Diode-pumped sub-50-fs Kerr-lens mode-locked Yb∶GdYCOB laser" } ] }, { "id": "R42", "label": "42", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "ÁLVAREZ-PÉREZ J O" }, { "name": "text", "data": "， " }, { "name": "text", "data": "CANO-TORRES J M" }, { "name": "text", "data": "， " }, { "name": "text", "data": "RUIZ A" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "A roadmap for laser optimization of Yb∶Ca" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "（NbGa）" }, { "name": "sub", "data": [ { "name": "text", "data": "5" } ] }, { "name": "text", "data": "O" }, { "name": "sub", "data": [ { "name": "text", "data": "12" } ] }, { "name": "text", "data": "-CNGG-type single crystal garnets" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "J. Mater. Chem. C" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "9" }, { "name": "text", "data": "（" }, { "name": "text", "data": "13" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "4628" }, { "name": "text", "data": "-" }, { "name": "text", "data": "4642" }, { "name": "text", "data": "." } ], "title": "A roadmap for laser optimization of Yb∶Ca3（NbGa）5O12-CNGG-type single crystal garnets" } ] }, { "id": "R43", "label": "43", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "相国涛" }, { "name": "text", "data": "， " }, { "name": "text", "data": "杨梦琳" }, { "name": "text", "data": "， " }, { "name": "text", "data": "刘臻" }, { "name": "text", "data": "， " }, { "name": "text", "data": "等" }, { "name": "text", "data": ". " }, { "name": "text", "data": "NaScF" }, { "name": "sub", "data": [ { "name": "text", "data": "4" } ] }, { "name": "text", "data": "∶Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "/Er" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "纳米颗粒荧光温敏特性" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "发光学报" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2022" }, { "name": "text", "data": "， " }, { "name": "text", "data": "43" }, { "name": "text", "data": "（" }, { "name": "text", "data": "5" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "684" }, { "name": "text", "data": "-" }, { "name": "text", "data": "690" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/cjl.20220064" } ], "href": "http://dx.doi.org/10.37188/cjl.20220064" } } ], "title": "NaScF4∶Yb3+/Er3+纳米颗粒荧光温敏特性" }, { "lang": "en", "text": [ { "name": "text", "data": "XIANG G T" }, { "name": "text", "data": "， " }, { "name": "text", "data": "YANG M L" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LIU Z" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Temperature sensing properties in NaScF" }, { "name": "sub", "data": [ { "name": "text", "data": "4" } ] }, { "name": "text", "data": "∶Yb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "/Er" }, { "name": "sup", "data": [ { "name": "text", "data": "3+ " } ] }, { "name": "text", "data": "nanoparticles" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Chin. J. Lumin." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2022" }, { "name": "text", "data": "， " }, { "name": "text", "data": "43" }, { "name": "text", "data": "（" }, { "name": "text", "data": "5" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "684" }, { "name": "text", "data": "-" }, { "name": "text", "data": "690" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/cjl.20220064" } ], "href": "http://dx.doi.org/10.37188/cjl.20220064" } } ], "title": "Temperature sensing properties in NaScF4∶Yb3+/Er3+ nanoparticles" } ] }, { "id": "R44", "label": "44", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "刘翠翠" }, { "name": "text", "data": "， " }, { "name": "text", "data": "林楠" }, { "name": "text", "data": "， " }, { "name": "text", "data": "马骁宇" }, { "name": "text", "data": "， " }, { "name": "text", "data": "等" }, { "name": "text", "data": ". " }, { "name": "text", "data": "带有非吸收窗口的高性能InGaAs/AlGaAs量子阱激光二极管" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "发光学报" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2022" }, { "name": "text", "data": "， " }, { "name": "text", "data": "43" }, { "name": "text", "data": "（" }, { "name": "text", "data": "1" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "110" }, { "name": "text", "data": "-" }, { "name": "text", "data": "118" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/cjl.20210306" } ], "href": "http://dx.doi.org/10.37188/cjl.20210306" } } ], "title": "带有非吸收窗口的高性能InGaAs/AlGaAs量子阱激光二极管" }, { "lang": "en", "text": [ { "name": "text", "data": "LIU C C" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LIN N" }, { "name": "text", "data": "， " }, { "name": "text", "data": "MA X Y" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "High performance InGaAs/AlGaAs quantum well semiconductor laser diode with non-absorption window" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Chin. J. Lumin." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2022" }, { "name": "text", "data": "， " }, { "name": "text", "data": "43" }, { "name": "text", "data": "（" }, { "name": "text", "data": "1" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "110" }, { "name": "text", "data": "-" }, { "name": "text", "data": "118" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/cjl.20210306" } ], "href": "http://dx.doi.org/10.37188/cjl.20210306" } } ], "title": "High performance InGaAs/AlGaAs quantum well semiconductor laser diode with non-absorption window" } ] }, { "id": "R45", "label": "45", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "ZHANG Y H" }, { "name": "text", "data": "， " }, { "name": "text", "data": "LI S M" }, { "name": "text", "data": "， " }, { "name": "text", "data": "DU X" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " crystal for efficient ultrashort pulse lasers" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Opt. Lett." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "46" }, { "name": "text", "data": "（" }, { "name": "text", "data": "15" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "3641" }, { "name": "text", "data": "-" }, { "name": "text", "data": "3644" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1364/ol.431243" } ], "href": "http://dx.doi.org/10.1364/ol.431243" } } ], "title": "Yb∶GdScO3 crystal for efficient ultrashort pulse lasers" } ] }, { "id": "R46", "label": "46", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "GUPTA S K" }, { "name": "text", "data": "， " }, { "name": "text", "data": "GROVER V" }, { "name": "text", "data": "， " }, { "name": "text", "data": "SHUKLA R" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Exploring pure and " }, { "name": "italic", "data": [ { "name": "text", "data": "RE" } ] }, { "name": "text", "data": " co-doped （Eu" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "， Tb" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": " and Dy" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "） gadolinium scandate： luminescence behaviour and dynamics of energy transfer" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Chem. Eng. J." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2016" }, { "name": "text", "data": "， " }, { "name": "text", "data": "283" }, { "name": "text", "data": "： " }, { "name": "text", "data": "114" }, { "name": "text", "data": "-" }, { "name": "text", "data": "126" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1016/j.cej.2015.07.043" } ], "href": "http://dx.doi.org/10.1016/j.cej.2015.07.043" } } ], "title": "Exploring pure and RE co-doped （Eu3+， Tb3+ and Dy3+） gadolinium scandate： luminescence behaviour and dynamics of energy transfer" } ] }, { "id": "R47", "label": "47", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "CHENEBUAH E T" }, { "name": "text", "data": "， " }, { "name": "text", "data": "NGANBE M" }, { "name": "text", "data": "， " }, { "name": "text", "data": "TCHAGANG A B" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Comparative analysis of machine learning approaches on the prediction of the electronic properties of perovskites： a case study of " }, { "name": "italic", "data": [ { "name": "text", "data": "ABX" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " and " }, { "name": "italic", "data": [ { "name": "text", "data": "A" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "2" } ] }, { "name": "italic", "data": [ { "name": "text", "data": "BB′X" } ] }, { "name": "sub", "data": [ { "name": "text", "data": "6" } ] }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Mater. Today Commun." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "27" }, { "name": "text", "data": "： " }, { "name": "text", "data": "102462" }, { "name": "text", "data": "." } ], "title": "Comparative analysis of machine learning approaches on the prediction of the electronic properties of perovskites： a case study of ABX3 and A2BB′X6" } ] }, { "id": "R48", "label": "48", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "RIETVELD H M" }, { "name": "text", "data": ". " }, { "name": "text", "data": "A profile refinement method for nuclear and magnetic structures" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "J. Appl. Cryst." }, { "name": "text", "data": "， " }, { "name": "text", "data": "1969" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2" }, { "name": "text", "data": "（" }, { "name": "text", "data": "2" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "65" }, { "name": "text", "data": "-" }, { "name": "text", "data": "71" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1107/s0021889869006558" } ], "href": "http://dx.doi.org/10.1107/s0021889869006558" } } ], "title": "A profile refinement method for nuclear and magnetic structures" } ] }, { "id": "R49", "label": "49", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "RIETVELD H M" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Line profiles of neutron powder-diffraction peaks for structure refinement" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Acta Cryst." }, { "name": "text", "data": "， " }, { "name": "text", "data": "1967" }, { "name": "text", "data": "， " }, { "name": "text", "data": "22" }, { "name": "text", "data": "（" }, { "name": "text", "data": "1" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "151" }, { "name": "text", "data": "-" }, { "name": "text", "data": "152" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1107/s0365110x67000234" } ], "href": "http://dx.doi.org/10.1107/s0365110x67000234" } } ], "title": "Line profiles of neutron powder-diffraction peaks for structure refinement" } ] }, { "id": "R50", "label": "50", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "柳欢" }, { "name": "text", "data": "， " }, { "name": "text", "data": "高薪羽" }, { "name": "text", "data": "， " }, { "name": "text", "data": "白杰" }, { "name": "text", "data": "， " }, { "name": "text", "data": "等" }, { "name": "text", "data": ". " }, { "name": "text", "data": "钙钛矿氧化物ABO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "的结构调控与电催化性能研究进展" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "应用化工" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "50" }, { "name": "text", "data": "（" }, { "name": "text", "data": "12" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "3498" }, { "name": "text", "data": "-" }, { "name": "text", "data": "3503" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.3969/j.issn.1671-3206.2021.12.056" } ], "href": "http://dx.doi.org/10.3969/j.issn.1671-3206.2021.12.056" } } ], "title": "钙钛矿氧化物ABO3的结构调控与电催化性能研究进展" }, { "lang": "en", "text": [ { "name": "text", "data": "LIU H" }, { "name": "text", "data": "， " }, { "name": "text", "data": "GAO X Y" }, { "name": "text", "data": "， " }, { "name": "text", "data": "BAI J" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Advances in structural regulation and electrocatalytic properties of ABO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " perovskite oxides" }, { "name": "text", "data": " ［J］ " }, { "name": "text", "data": "Appl. Chem. Ind." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "50" }, { "name": "text", "data": "（" }, { "name": "text", "data": "12" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "3498" }, { "name": "text", "data": "-" }, { "name": "text", "data": "3503" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.3969/j.issn.1671-3206.2021.12.056" } ], "href": "http://dx.doi.org/10.3969/j.issn.1671-3206.2021.12.056" } } ], "title": "Advances in structural regulation and electrocatalytic properties of ABO3 perovskite oxides" } ] }, { "id": "R51", "label": "51", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "杨洁" }, { "name": "text", "data": "， " }, { "name": "text", "data": "皮明雨" }, { "name": "text", "data": "， " }, { "name": "text", "data": "张丁可" }, { "name": "text", "data": "， " }, { "name": "text", "data": "等" }, { "name": "text", "data": ". " }, { "name": "text", "data": "低维钙钛矿光电探测器研究进展" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "发光学报" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "42" }, { "name": "text", "data": "（" }, { "name": "text", "data": "6" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "755" }, { "name": "text", "data": "-" }, { "name": "text", "data": "773" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/CJL.20210033" } ], "href": "http://dx.doi.org/10.37188/CJL.20210033" } } ], "title": "低维钙钛矿光电探测器研究进展" }, { "lang": "en", "text": [ { "name": "text", "data": "YANG J" }, { "name": "text", "data": "， " }, { "name": "text", "data": "PI M Y" }, { "name": "text", "data": "， " }, { "name": "text", "data": "ZHANG D K" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Recent progress on low-dimensional perovskite photodetectors" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Chin. J. Lumin." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "42" }, { "name": "text", "data": "（" }, { "name": "text", "data": "6" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "755" }, { "name": "text", "data": "-" }, { "name": "text", "data": "773" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/CJL.20210033" } ], "href": "http://dx.doi.org/10.37188/CJL.20210033" } } ], "title": "Recent progress on low-dimensional perovskite photodetectors" } ] }, { "id": "R52", "label": "52", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "周港杰" }, { "name": "text", "data": "， " }, { "name": "text", "data": "胡艺萱" }, { "name": "text", "data": "， " }, { "name": "text", "data": "谭林玲" }, { "name": "text", "data": "， " }, { "name": "text", "data": "等" }, { "name": "text", "data": ". " }, { "name": "text", "data": "碲掺杂钙⁃铝⁃锗酸盐玻璃宽带近红外发光及其调控机理" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "发光学报" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2022" }, { "name": "text", "data": "， " }, { "name": "text", "data": "43" }, { "name": "text", "data": "（" }, { "name": "text", "data": "1" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "51" }, { "name": "text", "data": "-" }, { "name": "text", "data": "57" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/cjl.20210337" } ], "href": "http://dx.doi.org/10.37188/cjl.20210337" } } ], "title": "碲掺杂钙⁃铝⁃锗酸盐玻璃宽带近红外发光及其调控机理" }, { "lang": "en", "text": [ { "name": "text", "data": "ZHOU G J" }, { "name": "text", "data": "， " }, { "name": "text", "data": "HU Y X" }, { "name": "text", "data": "， " }, { "name": "text", "data": "TAN L L" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Broadband near-infrared luminescence and regulation mechanism of tellurium-doped calcium-aluminum-germanate glass" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Chin. J. Lumin." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2022" }, { "name": "text", "data": "， " }, { "name": "text", "data": "43" }, { "name": "text", "data": "（" }, { "name": "text", "data": "1" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "51" }, { "name": "text", "data": "-" }, { "name": "text", "data": "57" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/cjl.20210337" } ], "href": "http://dx.doi.org/10.37188/cjl.20210337" } } ], "title": "Broadband near-infrared luminescence and regulation mechanism of tellurium-doped calcium-aluminum-germanate glass" } ] }, { "id": "R53", "label": "53", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "杨立群" }, { "name": "text", "data": "， " }, { "name": "text", "data": "马晓辉" }, { "name": "text", "data": "， " }, { "name": "text", "data": "郑士建" }, { "name": "text", "data": "， " }, { "name": "text", "data": "等" }, { "name": "text", "data": ". " }, { "name": "text", "data": "柔性钙钛矿太阳能电池中电极材料和电荷传输材料的研究进展" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "发光学报" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2020" }, { "name": "text", "data": "， " }, { "name": "text", "data": "41" }, { "name": "text", "data": "（" }, { "name": "text", "data": "10" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "1175" }, { "name": "text", "data": "-" }, { "name": "text", "data": "1194" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/CJL.20200192" } ], "href": "http://dx.doi.org/10.37188/CJL.20200192" } } ], "title": "柔性钙钛矿太阳能电池中电极材料和电荷传输材料的研究进展" }, { "lang": "en", "text": [ { "name": "text", "data": "YANG L Q" }, { "name": "text", "data": "， " }, { "name": "text", "data": "MA X H" }, { "name": "text", "data": "， " }, { "name": "text", "data": "ZHENG S J" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Research progress on electrode materials and charge transport materials in flexible perovskite solar cells" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Chin. J. Lumin." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2020" }, { "name": "text", "data": "， " }, { "name": "text", "data": "41" }, { "name": "text", "data": "（" }, { "name": "text", "data": "10" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "1175" }, { "name": "text", "data": "-" }, { "name": "text", "data": "1194" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/CJL.20200192" } ], "href": "http://dx.doi.org/10.37188/CJL.20200192" } } ], "title": "Research progress on electrode materials and charge transport materials in flexible perovskite solar cells" } ] }, { "id": "R54", "label": "54", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "胡强" }, { "name": "text", "data": "， " }, { "name": "text", "data": "白雪" }, { "name": "text", "data": "， " }, { "name": "text", "data": "宋宏伟" }, { "name": "text", "data": "， " }, { "name": "text", "data": "等" }, { "name": "text", "data": ". " }, { "name": "text", "data": "稀土离子掺杂钙钛矿纳米晶的光学性质和应用" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "发光学报" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2022" }, { "name": "text", "data": "， " }, { "name": "text", "data": "43" }, { "name": "text", "data": "（" }, { "name": "text", "data": "1" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "8" }, { "name": "text", "data": "-" }, { "name": "text", "data": "25" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/CJL.20210330" } ], "href": "http://dx.doi.org/10.37188/CJL.20210330" } } ], "title": "稀土离子掺杂钙钛矿纳米晶的光学性质和应用" }, { "lang": "en", "text": [ { "name": "text", "data": "HU Q" }, { "name": "text", "data": "， " }, { "name": "text", "data": "BAI X" }, { "name": "text", "data": "， " }, { "name": "text", "data": "SONG H W" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Rare earth ion doped perovskite nanocrystals" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Chin. J. Lumin." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2022" }, { "name": "text", "data": "， " }, { "name": "text", "data": "43" }, { "name": "text", "data": "（" }, { "name": "text", "data": "1" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "8" }, { "name": "text", "data": "-" }, { "name": "text", "data": "25" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/CJL.20210330" } ], "href": "http://dx.doi.org/10.37188/CJL.20210330" } } ], "title": "Rare earth ion doped perovskite nanocrystals" } ] }, { "id": "R55", "label": "55", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "时秋峰" }, { "name": "text", "data": "， " }, { "name": "text", "data": "王磊" }, { "name": "text", "data": "， " }, { "name": "text", "data": "郭海洁" }, { "name": "text", "data": "， " }, { "name": "text", "data": "等" }, { "name": "text", "data": ". " }, { "name": "text", "data": "真空紫外光及X射线激发下Pr" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": "掺杂Ba" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "La（PO" }, { "name": "sub", "data": [ { "name": "text", "data": "4" } ] }, { "name": "text", "data": "）" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "发光性质" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "发光学报" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "42" }, { "name": "text", "data": "（" }, { "name": "text", "data": "11" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "1756" }, { "name": "text", "data": "-" }, { "name": "text", "data": "1762" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/CJL.20210281" } ], "href": "http://dx.doi.org/10.37188/CJL.20210281" } } ], "title": "真空紫外光及X射线激发下Pr3+掺杂Ba3La（PO4）3发光性质" }, { "lang": "en", "text": [ { "name": "text", "data": "SHI Q F" }, { "name": "text", "data": "， " }, { "name": "text", "data": "WANG L" }, { "name": "text", "data": "， " }, { "name": "text", "data": "GUO H J" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Luminescence properties of Pr" }, { "name": "sup", "data": [ { "name": "text", "data": "3+" } ] }, { "name": "text", "data": " doped in Ba" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "La（PO" }, { "name": "sub", "data": [ { "name": "text", "data": "4" } ] }, { "name": "text", "data": "）" }, { "name": "sub", "data": [ { "name": "text", "data": "3 " } ] }, { "name": "text", "data": "with vacuum ultraviolet and X-ray excitation" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Chin. J. Lumin." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2021" }, { "name": "text", "data": "， " }, { "name": "text", "data": "42" }, { "name": "text", "data": "（" }, { "name": "text", "data": "11" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "1756" }, { "name": "text", "data": "-" }, { "name": "text", "data": "1762" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.37188/CJL.20210281" } ], "href": "http://dx.doi.org/10.37188/CJL.20210281" } } ], "title": "Luminescence properties of Pr3+ doped in Ba3La（PO4）3 with vacuum ultraviolet and X-ray excitation" } ] }, { "id": "R56", "label": "56", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "张思远" }, { "name": "text", "data": ". " }, { "name": "text", "data": "稀土离子的光谱学" }, { "name": "text", "data": " ［M］. " }, { "name": "text", "data": "北京" }, { "name": "text", "data": "： " }, { "name": "text", "data": "科学出版社" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2008" }, { "name": "text", "data": "." } ], "title": "稀土离子的光谱学" }, { "lang": "en", "text": [ { "name": "text", "data": "ZHANG S Y" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Spectroscopy of Rare Earth Ions" }, { "name": "text", "data": " ［M］. " }, { "name": "text", "data": "Beijing" }, { "name": "text", "data": "： " }, { "name": "text", "data": "Science Press" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2008" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" } ], "title": "Spectroscopy of Rare Earth Ions" } ] }, { "id": "R57", "label": "57", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "张庆礼" }, { "name": "text", "data": "， " }, { "name": "text", "data": "肖敬忠" }, { "name": "text", "data": "， " }, { "name": "text", "data": "孙敦陆" }, { "name": "text", "data": "， " }, { "name": "text", "data": "等" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Yb∶YAG的晶体生长和光谱参数计算" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "光谱学与光谱学分析" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2004" }, { "name": "text", "data": "， " }, { "name": "text", "data": "24" }, { "name": "text", "data": "（" }, { "name": "text", "data": "10" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "1157" }, { "name": "text", "data": "-" }, { "name": "text", "data": "1160" }, { "name": "text", "data": "." } ], "title": "Yb∶YAG的晶体生长和光谱参数计算" }, { "lang": "en", "text": [ { "name": "text", "data": "ZHANG Q L" }, { "name": "text", "data": "， " }, { "name": "text", "data": "XIAO J Z" }, { "name": "text", "data": "， " }, { "name": "text", "data": "SUN D L" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Crystal growth and spectral parameter computation of Yb∶YAG" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Spectrosc. Spectral Anal." }, { "name": "text", "data": "， " }, { "name": "text", "data": "2004" }, { "name": "text", "data": "， " }, { "name": "text", "data": "24" }, { "name": "text", "data": "（" }, { "name": "text", "data": "10" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "1157" }, { "name": "text", "data": "-" }, { "name": "text", "data": "1160" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" } ], "title": "Crystal growth and spectral parameter computation of Yb∶YAG" } ] }, { "id": "R58", "label": "58", "citation": [ { "lang": "zh", "text": [ { "name": "text", "data": "徐军" }, { "name": "text", "data": "， " }, { "name": "text", "data": "徐晓东" }, { "name": "text", "data": "， " }, { "name": "text", "data": "苏良碧" }, { "name": "text", "data": ". " }, { "name": "text", "data": "掺镱激光晶体材料" }, { "name": "text", "data": " ［M］. " }, { "name": "text", "data": "上海" }, { "name": "text", "data": "： " }, { "name": "text", "data": "上海科学普及出版社" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2005" }, { "name": "text", "data": "." } ], "title": "掺镱激光晶体材料" }, { "lang": "en", "text": [ { "name": "text", "data": "XU J" }, { "name": "text", "data": "， " }, { "name": "text", "data": "XU X D" }, { "name": "text", "data": "， " }, { "name": "text", "data": "SU L B" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Ytterbium‐doped Laser Crystal Materials" }, { "name": "text", "data": " ［M］. " }, { "name": "text", "data": "Shanghai" }, { "name": "text", "data": "： " }, { "name": "text", "data": "Shanghai Science Popularization Press" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2005" }, { "name": "text", "data": ". " }, { "name": "text", "data": "（in Chinese）" } ], "title": "Ytterbium‐doped Laser Crystal Materials" } ] }, { "id": "R59", "label": "59", "citation": [ { "lang": "en", "text": [ { "name": "text", "data": "ZHANG Q L" }, { "name": "text", "data": "， " }, { "name": "text", "data": "SUN G" }, { "name": "text", "data": "， " }, { "name": "text", "data": "GAO J Y" }, { "name": "text", "data": "， " }, { "name": "text", "data": "et al" }, { "name": "text", "data": ". " }, { "name": "text", "data": "Profile function properties & optical transition formulae" }, { "name": "text", "data": " ［J］. " }, { "name": "text", "data": "Chin. Phys. B" }, { "name": "text", "data": "， " }, { "name": "text", "data": "2017" }, { "name": "text", "data": "， " }, { "name": "text", "data": "26" }, { "name": "text", "data": "（" }, { "name": "text", "data": "7" }, { "name": "text", "data": "）： " }, { "name": "text", "data": "077803-1-5" }, { "name": "text", "data": ". " }, { "name": "text", "data": " doi: " }, { "name": "extlink", "data": { "text": [ { "name": "text", "data": "10.1088/1674-1056/26/7/077803" } ], "href": "http://dx.doi.org/10.1088/1674-1056/26/7/077803" } } ], "title": "Profile function properties & optical transition formulae" } ] } ] }, "response": [], "contributions": [], "acknowledgements": [], "conflict": [], "supportedby": [], "articlemeta": { "doi": "10.37188/CJL.20220249", "clc": [ [ { "name": "text", "data": "O482.31" } ] ], "dc": [ { "name": "text", "data": "A" } ], "publisherid": "1000-7032（2022）11-1779-10", "citeme": [ { "data": [ { "name": "text", "data": "李加红,张庆礼,孙贵花等.Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": "晶体光谱参数计算[J].发光学报,2022,43(11):1779-1788." } ], "text": "李加红,张庆礼,孙贵花等.Yb∶GdScO3晶体光谱参数计算[J].发光学报,2022,43(11):1779-1788." }, { "data": [ { "name": "text", "data": "LI Jia-hong,ZHANG Qing-li,SUN Gui-hua,et al.Spectral Parameter Computation of Yb∶GdScO" }, { "name": "sub", "data": [ { "name": "text", "data": "3" } ] }, { "name": "text", "data": " Crystal[J].Chinese Journal of Luminescence,2022,43(11):1779-1788." } ], "text": "LI Jia-hong,ZHANG Qing-li,SUN Gui-hua,et al.Spectral Parameter Computation of Yb∶GdScO3 Crystal[J].Chinese Journal of Luminescence,2022,43(11):1779-1788." } ], "fundinggroup": [ { "lang": "zh", "text": [ { "name": "text", "data": "安徽省先进激光技术实验室开放项目（AHL 20220 ZR04）；国家自然科学基金（51802307）；安徽省重大科技专项（202203a05020002）资助项目" } ] }, { "lang": "en", "text": [ { "name": "text", "data": "Supported by The Open Project of Advanced Laser Technology Laboratory of Anhui Province（AHL 20220 ZR04）； National Natural Science Foundation of China（51802307）； Major Special Project of Science and Technology of Anhui Province（202203a05020002）" } ] } ], "history": { "received": "2022-06-24", "revised": "2022-07-03", "ppub": "2022-11-05", "opub": "2022-12-08" } }, "appendix": [], "type": "research-article", "ethics": [], "supplementary": [], "journalTitle": "发光学报", "issue": "11", "volume": "43", "originalSource": [] }