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长春理工大学, 光电子技术研究所,吉林 长春,130022
收稿日期:2006-02-28,
修回日期:2006-10-18,
纸质出版日期:2006-11-20
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姜德龙, 刘庆飞, 李野, 王国政, 高延军, 吴奎, 付申成, 端木庆铎, 田景全. 微通道板离子壁垒膜及其对入射离子的阻止作用[J]. 发光学报, 2006,27(6): 1015-1020
JIANG De-long, LIU Qing-fei, LI Ye, WANG Guo-zheng, GAO Yan-jun, WU Kui, FU Shen-cheng, DUANMU Qing-duo, TIAN Jing-quan. MCP Ion Barrier Film and Its Stopping Function on Incident Ions[J]. Chinese Journal of Luminescence, 2006,27(6): 1015-1020
姜德龙, 刘庆飞, 李野, 王国政, 高延军, 吴奎, 付申成, 端木庆铎, 田景全. 微通道板离子壁垒膜及其对入射离子的阻止作用[J]. 发光学报, 2006,27(6): 1015-1020 DOI:
JIANG De-long, LIU Qing-fei, LI Ye, WANG Guo-zheng, GAO Yan-jun, WU Kui, FU Shen-cheng, DUANMU Qing-duo, TIAN Jing-quan. MCP Ion Barrier Film and Its Stopping Function on Incident Ions[J]. Chinese Journal of Luminescence, 2006,27(6): 1015-1020 DOI:
给出了三代微光像管中微通道板离子壁垒膜对入射正离子阻止作用的描述
引进了核阻止本领、电子阻止本领和平均射程的概念。结合Tomas-Fermi屏蔽势进行了分析讨论和Monte-Carlo模拟计算
给出Al
2
O
3
和SiO
2
薄膜对不同能量垂直入射时的核、电子阻止的定量结果。得出了Al
2
O
3
薄膜阻止本领比SiO
2
阻止本领高的结论。证实了选用Al
2
O
3
离子壁垒膜的科学性和可行性。
The microchannel plate (MCP) ion barrier film's stopping function on incident positive ions in the third generation low-level-light imaging tube was introduced. The concepts of nuclear stopping power
electronic stopping power and average range were also introduced
the micrographs of unfilmed MCP and MCPs filmed with different thicknesses were shown. Using Tomas-Fermi shielding potential
we analyze and discuss this problem and a Monte-Carlo simulation was peromed. Analytical expressions and corresponding nuclear and electronic stopping power curves have been shown. Quantitative results were given
reflecting the stopping function of Al
2
O
3
and SiO
2
films when nucleus and electrons impinge perpendicularly with different energies. Table 1~3 show the corresponding technical data. The conclusion is that the stopping power of Al
2
O
3
film is stronger than that of SiO
2
and the selection of Al
2
O
3
ion barrier film is reasonable and feasible. After the theoretical analysis and experimental simulation
the conclusions are brought forward as follows:The stopping function of ion barrier film on the incident ions can be described by two concepts of nuclear stopping power and electronic stopping power. When the thickness of the films is constant
the range of the ions with the same energy in Al
2
O
3
films is two to three times as short as that in SiO
2
films. It is indicated that the capability of the stopping function of Al
2
O
3
films is higher than that of SiO
2
films. From the calculated results of the stopping function of the films on the ions
it is obviously concluded that the capability of nuclear stopping function on the ions is higher than that of electron
which is in agreement with LSStheory. When 9999 oxygen ions with the energies of 100
300
500 eV are perpendicularly incident to the Al
2
O
3
film with 5 nm thickness
no transmitting ions are observed. While in the same conditions
34 and 629 oxygen ions with the energies of 300 eVand 500 eV
respectively
can pass through the SiO
2
films with 5 nm thickness
i.e
. the maximal transmittance is 6%. In brief
the capability of the stopping function of Al
2
O
3
films is higher than that of SiO
2
films
resulting from that Al
2
O
3
films are high density and the fiber rigidity of Al
2
O
3
films is close to that of corundum; while SiO
2
is atom crystal
and the rigidity of SiO
2
films is equivalent to that of crystal and inferior to that of Al
2
O
3
.
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