k . p finite difference method for semiconductor heterostructures
碩士 === 國立中山大學 === 物理研究所 === 84 === We have developed a six-band k.p finite difference method (KPFD) to calculate the electronic band structures of InAs-GaSb super- lattices and AlSb-GaSb-InAs-GaSb-AlSb quantum wells. The simple theoretical...
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ndltd-TW-084NSYSU1980112015-10-13T14:34:58Z http://ndltd.ncl.edu.tw/handle/44948476903637042063 k . p finite difference method for semiconductor heterostructures k.p有限差分法對半導體異質結構能帶計算的應用 Chau, Zih-Ming 趙志明 碩士 國立中山大學 物理研究所 84 We have developed a six-band k.p finite difference method (KPFD) to calculate the electronic band structures of InAs-GaSb super- lattices and AlSb-GaSb-InAs-GaSb-AlSb quantum wells. The simple theoretical method combines the virtues of the envelope- function (k.p) and bond-orbital model. All interaction parameters involved are directly related to parameters for describing bulk bands near the zone center in the bond-orbital model or k.p model. The method can reproduce fairly accurate bulk band structure near the center of the two-dimensional Brillouin zone when we properly choose the interaction parameters and the dis- tance between two adjacent pseudo- layers. For intrinsic InAs-GaSb superlattices, we don't find truly semimetallic band structure. At low temperature(∼4.2k), the critical InAs thickness for a zero-gap semiconductor result is approximately 120 A. The evolution of the InAs-GaSb band structure with increasing periodicity is calculated and found to be in excellent agreement with previous NBO (nearest neighbor bond-orbital model) results. In AlSb-GaSb-InAs-GaSb- AlSb quantum wells, we shall demonstrate that the semiconductor- semimetal transition does exist in this hole-electron-hole quantum wells systems. Chiang, Jih-Chen 蔣志純 1996 學位論文 ; thesis 36 zh-TW |
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zh-TW |
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碩士 === 國立中山大學 === 物理研究所 === 84 === We have developed a six-band k.p finite difference method
(KPFD) to calculate the electronic band structures of InAs-GaSb
super- lattices and AlSb-GaSb-InAs-GaSb-AlSb quantum wells. The
simple theoretical method combines the virtues of the envelope-
function (k.p) and bond-orbital model. All interaction
parameters involved are directly related to parameters for
describing bulk bands near the zone center in the bond-orbital
model or k.p model. The method can reproduce fairly accurate
bulk band structure near the center of the two-dimensional
Brillouin zone when we properly choose the interaction
parameters and the dis- tance between two adjacent pseudo-
layers. For intrinsic InAs-GaSb superlattices, we don't find
truly semimetallic band structure. At low temperature(∼4.2k),
the critical InAs thickness for a zero-gap semiconductor result
is approximately 120 A. The evolution of the InAs-GaSb band
structure with increasing periodicity is calculated and found
to be in excellent agreement with previous NBO (nearest
neighbor bond-orbital model) results. In AlSb-GaSb-InAs-GaSb-
AlSb quantum wells, we shall demonstrate that the semiconductor-
semimetal transition does exist in this hole-electron-hole
quantum wells systems.
|
author2 |
Chiang, Jih-Chen |
author_facet |
Chiang, Jih-Chen Chau, Zih-Ming 趙志明 |
author |
Chau, Zih-Ming 趙志明 |
spellingShingle |
Chau, Zih-Ming 趙志明 k . p finite difference method for semiconductor heterostructures |
author_sort |
Chau, Zih-Ming |
title |
k . p finite difference method for semiconductor heterostructures |
title_short |
k . p finite difference method for semiconductor heterostructures |
title_full |
k . p finite difference method for semiconductor heterostructures |
title_fullStr |
k . p finite difference method for semiconductor heterostructures |
title_full_unstemmed |
k . p finite difference method for semiconductor heterostructures |
title_sort |
k . p finite difference method for semiconductor heterostructures |
publishDate |
1996 |
url |
http://ndltd.ncl.edu.tw/handle/44948476903637042063 |
work_keys_str_mv |
AT chauzihming kpfinitedifferencemethodforsemiconductorheterostructures AT zhàozhìmíng kpfinitedifferencemethodforsemiconductorheterostructures AT chauzihming kpyǒuxiànchàfēnfǎduìbàndǎotǐyìzhìjiégòunéngdàijìsuàndeyīngyòng AT zhàozhìmíng kpyǒuxiànchàfēnfǎduìbàndǎotǐyìzhìjiégòunéngdàijìsuàndeyīngyòng |
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