Study of photoluminescence in GaN thin film
碩士 === 國立清華大學 === 光電工程研究所 === 94 === We excite GaN compound semiconductor by using the Ti: sapphire pulse laser as the pumping source so that we could observe the nonlinear absorption phenomenon, and hence the band structure of GaN. The wavelength of the Ti: sapphire pulse laser is 800 nm, unit peak...
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ndltd-TW-094NTHU51240052015-10-13T11:15:49Z http://ndltd.ncl.edu.tw/handle/39446512865094138968 Study of photoluminescence in GaN thin film 氮化鎵薄膜之光致螢光現象研究 林士航 碩士 國立清華大學 光電工程研究所 94 We excite GaN compound semiconductor by using the Ti: sapphire pulse laser as the pumping source so that we could observe the nonlinear absorption phenomenon, and hence the band structure of GaN. The wavelength of the Ti: sapphire pulse laser is 800 nm, unit peak power could be 81.25 KW. After chirped-pulse amplification, its wavelength is still 800nm, but unit peak power could reach 4.62 GW. First we use He-Cd laser (325nm) to excite n-GaN sample with variable pump power and temperature. The photoluminescence we got correspond to the band-edge structure of GaN. The PL spectrum of GaN should has the dependence of polarization of E-filed in theory, but we couldn’t observe that phenomenon. It maybe due to Si-doped induced merge of band structure. For comparing, we also do experiment of unintentially-doped GaN, and with these data we could try to understand the mechanism of the carrier recombination in these two sample, both are dominated by donor-bound excitons. Alternatively, we use the pulse laser to excite GaN sample and thus have a PL spectrum looks like the linear excited one, but with a thinner spectrum width. Besides, using pulse-laser excitation, we could extract the power dependence (cubic) between the intensity of pumping laser and PL signal, and it shows that the photoluminescence is due to the 3-photon absorption of GaN. 齊正中 2005 學位論文 ; thesis 58 zh-TW |
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碩士 === 國立清華大學 === 光電工程研究所 === 94 === We excite GaN compound semiconductor by using the Ti: sapphire pulse laser as the pumping source so that we could observe the nonlinear absorption phenomenon, and hence the band structure of GaN. The wavelength of the Ti: sapphire pulse laser is 800 nm, unit peak power could be 81.25 KW. After chirped-pulse amplification, its wavelength is still 800nm, but unit peak power could reach 4.62 GW.
First we use He-Cd laser (325nm) to excite n-GaN sample with variable pump power and temperature. The photoluminescence we got correspond to the band-edge structure of GaN. The PL spectrum of GaN should has the dependence of polarization of E-filed in theory, but we couldn’t observe that phenomenon. It maybe due to Si-doped induced merge of band structure. For comparing, we also do experiment of unintentially-doped GaN, and with these data we could try to understand the mechanism of the carrier recombination in these two sample, both are dominated by donor-bound excitons. Alternatively, we use the pulse laser to excite GaN sample and thus have a PL spectrum looks like the linear excited one, but with a thinner spectrum width. Besides, using pulse-laser excitation, we could extract the power dependence (cubic) between the intensity of pumping laser and PL signal, and it shows that the photoluminescence is due to the 3-photon absorption of GaN.
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author2 |
齊正中 |
author_facet |
齊正中 林士航 |
author |
林士航 |
spellingShingle |
林士航 Study of photoluminescence in GaN thin film |
author_sort |
林士航 |
title |
Study of photoluminescence in GaN thin film |
title_short |
Study of photoluminescence in GaN thin film |
title_full |
Study of photoluminescence in GaN thin film |
title_fullStr |
Study of photoluminescence in GaN thin film |
title_full_unstemmed |
Study of photoluminescence in GaN thin film |
title_sort |
study of photoluminescence in gan thin film |
publishDate |
2005 |
url |
http://ndltd.ncl.edu.tw/handle/39446512865094138968 |
work_keys_str_mv |
AT línshìháng studyofphotoluminescenceinganthinfilm AT línshìháng dànhuàjiābáomózhīguāngzhìyíngguāngxiànxiàngyánjiū |
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