发光学报
髮光學報
발광학보
CHINESE JOURNAL OF LUMINESCENCE
2007年
3期
407-411
,共5页
王玥%施卫%苑进社%贺训军%胡辉%姬广举
王玥%施衛%苑進社%賀訓軍%鬍輝%姬廣舉
왕모%시위%원진사%하훈군%호휘%희엄거
InGaN/GaN%单量子阱%光致发光%透射光谱%反射光谱
InGaN/GaN%單量子阱%光緻髮光%透射光譜%反射光譜
InGaN/GaN%단양자정%광치발광%투사광보%반사광보
InGaN/GaN%single quantum well%photoluminescence%transmission spectra%reflection spectra
研究了用金属有机物气相外延(MOVPE)法在蓝宝石衬底上生长的In组分浓度保持不变的InGaN/GaN单量子阱结构在室温下的发光特性和光吸收特性.实验结果表明,在InGaN厚度<3 nm时,随着样品InGaN势阱层宽度的增加(1 nm),光致发光(PL)谱的发光峰值波长出现明显的红移33 nm现象,而且发光强度下降8%,谱线半峰全宽(FWHM)展宽,通过对样品的透射、反射光谱研究发现,量子阱层窄(1.5 nm)的样品在波长接近红外区时出现无吸收的现象,即R+T达到了100%,而在阱层较宽的样品中没有发现这一现象, 对引起这些现象的原因进行了讨论.这些结果有助于开发和优化三族氮化物半导体光电器件的进一步研究工作.
研究瞭用金屬有機物氣相外延(MOVPE)法在藍寶石襯底上生長的In組分濃度保持不變的InGaN/GaN單量子阱結構在室溫下的髮光特性和光吸收特性.實驗結果錶明,在InGaN厚度<3 nm時,隨著樣品InGaN勢阱層寬度的增加(1 nm),光緻髮光(PL)譜的髮光峰值波長齣現明顯的紅移33 nm現象,而且髮光彊度下降8%,譜線半峰全寬(FWHM)展寬,通過對樣品的透射、反射光譜研究髮現,量子阱層窄(1.5 nm)的樣品在波長接近紅外區時齣現無吸收的現象,即R+T達到瞭100%,而在阱層較寬的樣品中沒有髮現這一現象, 對引起這些現象的原因進行瞭討論.這些結果有助于開髮和優化三族氮化物半導體光電器件的進一步研究工作.
연구료용금속유궤물기상외연(MOVPE)법재람보석츤저상생장적In조분농도보지불변적InGaN/GaN단양자정결구재실온하적발광특성화광흡수특성.실험결과표명,재InGaN후도<3 nm시,수착양품InGaN세정층관도적증가(1 nm),광치발광(PL)보적발광봉치파장출현명현적홍이33 nm현상,이차발광강도하강8%,보선반봉전관(FWHM)전관,통과대양품적투사、반사광보연구발현,양자정층착(1.5 nm)적양품재파장접근홍외구시출현무흡수적현상,즉R+T체도료100%,이재정층교관적양품중몰유발현저일현상, 대인기저사현상적원인진행료토론.저사결과유조우개발화우화삼족담화물반도체광전기건적진일보연구공작.
Gallium nitride and its ternary alloys have been attracting much attention because of their unique physical and chemical properties and their great potentialities for semiconductor industrial applications, such as light emitting diodes(LEDs), laser diodes(LDs) operating from green to ultraviolet(UV), UV-detectors and microwave power devices. The primary object of this study is to investigate the influence of different thickness of Fixed-Indium-Content InGaN layer on the shift of the photoluminescence(PL) spectra and optical absorption of the whole system structure. Photoluminescence(PL) and absorption properties of the Fixed-Indium-Content InGaN/GaN heterojunction single quantum well (SQW) structures have been investigated using photoluminescence spectrum and ultraviolet-vi-sible spectrophotometer at room temperature, respectively. The films were grown by metal-organic vapor phase epitaxy (MOVPE), using GaN buffer layer on sapphire substrates. The width of InGaN layer (<3 nm) in the SQW was varied while keeping other growth parameters fixed. Sample A has an InGaN active layer of thickness 1.5 nm, and Sample B has an InGaN active layer of thickness 2.5 nm. Two samples were capped with a 25 nm GaN layer. PL measurements show that the PL peak position (432 nm in Sample A and 465 nm in Sample B) was redshifted by 33 nm, the intensity was reduced about 8%, and the full width at half maximum (FWHM) of PL spectrum increases with increasing (1 nm) of the potential well layer width. The spectra of transmission and reflection show that transmission T is very high there can be only few reflection R as no absorption R+T exceeds 100% in the near infrared ranges for the sample with InGaN layer of thickness 1.5 nm. The reasons of these results are discussed. The significance of these studies is multifold and these results provide further information of importance toward the design optimization of optoelectronic devices employing the Ⅲ-nitrides.