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宁波大学光电子材料研究所,浙江 宁波,315211
收稿日期:2000-11-07,
修回日期:2001-04-11,
纸质出版日期:2001-08-30
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夏海平, 章践立, 陈红兵, 张新民, 王金浩, 聂秋华. 含偶氮分子的ormocer固体薄膜制备及二阶光学非线性[J]. 发光学报, 2001,22(3): 276-279
XIA Hai-ping, ZHANG Jian-li, CHEN Hong-bing, ZHANG Xin-min, WANG Jin-hao, NIE Qiu-hua. Fabrication of Ormocer Films Containing Azo dye Molecules and Their Optical Second Order Nonlinearities[J]. Chinese Journal of Luminescence, 2001,22(3): 276-279
夏海平, 章践立, 陈红兵, 张新民, 王金浩, 聂秋华. 含偶氮分子的ormocer固体薄膜制备及二阶光学非线性[J]. 发光学报, 2001,22(3): 276-279 DOI:
XIA Hai-ping, ZHANG Jian-li, CHEN Hong-bing, ZHANG Xin-min, WANG Jin-hao, NIE Qiu-hua. Fabrication of Ormocer Films Containing Azo dye Molecules and Their Optical Second Order Nonlinearities[J]. Chinese Journal of Luminescence, 2001,22(3): 276-279 DOI:
利用溶胶凝胶(solgel)低温合成非晶态技术
以γ氨基丙基三乙氧基硅烷(3-aminopropyltriethox ysilane
KH550)与γ缩水甘油醚基丙基三甲氧基硅烷(3-glycidoxy-propltrimethoxysilane
KH560)为先驱体
把Disperse Orange3(DO3)偶氮分子以3wt%浓度掺杂到上述溶胶与ormocer(organic modified ceramic)体系中。在ITO片上制备成厚度为4μm的DO3/90KH560-10KH550薄膜。经高温电晕极化后
用二次谐波发生装置
测量出薄膜材料的二次谐波强度
并计算出经极化后薄膜材料的p→p的二阶有效极化系数d
eff
=0.11pm/V。极化24小时后
其SHG强度基本保持不变
大约为刚极化后的80%大小。我们认为这主要是由于介质中KH550的引入
其中-NH
2
基团与DO3中的-NH
2
之间形成了氢键的作用
以及由氢键引起的介质材料进一步致密化作用
使得DO3分子不易发生弛豫作用
而保持极化后的分子状态。
Using 3-aminopropyltriethoxy-silane(KH550) and 3-glycidoxypropltrimethoxy-silane(KH560) as precursors
Disperse Orange 3 (DO3) was doped into above sol and ormocer in 3wt% concentration
and the sol-gel derived films with 4μm thickness coated on ITO film were fabricated. Corona poling was performed by applying a high voltage of + 5kV to a needle electrode. After corona poling of the film at 185° for 4 hours
about 1/5 of DO3 molecules remained in solid state film
estimating from their spectra
and the concentration of DO3 molecule in poled film was estimated about 1.6×10
19
cm
-3
. Second harmonic generation (SHG) was used to probe the size and stability of the orientational order of the poled films. The second harmonic intensity of the films was measured using p (parallel polarized) excitation and p detection
and compared with that generated by a
y
-cut quartz crystal. No Maker fringe pattern for the film was observed
we could assume that the coherence length was much larger than the film thickness. The SHG intensity increases with increasing angle and reaches to maximum at θ=52°. The effective second order nonlinear coefficient
d
eff
and d
33
were estimated about 0.11pm/V and 0.14pm/V
respectively
and the intensity of SHG decreased slightly and remained ~80% of the initial value even after poling 500 hours. It is thought that for a combination of DO3 and organic inorganic gel the pore shrinkage and high baking temperature stabilize the nonlinearity in particular. Furthermore
due to leading KH550 (containing-NH
2
group) into sol-gel derived matrix
it is expected that the hydrogen bonds between DO3 and KH550 in matrix are formed and the more density of matrix is reached
which can keep the oriented DO3 stable.
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