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dc.contributor.author郭培烜en_US
dc.contributor.authorP. S. Kuoen_US
dc.contributor.author陳 振 芳 老師en_US
dc.contributor.authorJ.F. Chenen_US
dc.date.accessioned2014-12-12T02:23:24Z-
dc.date.available2014-12-12T02:23:24Z-
dc.date.issued1999en_US
dc.identifier.urihttp://140.113.39.130/cdrfb3/record/nctu/#NT880429036en_US
dc.identifier.urihttp://hdl.handle.net/11536/65826-
dc.description.abstract異質GaAsN/GaAs量子井結構,具有較大的Conduction-band offset,可做為1.3μm~1.5μm的發光元件,但因Lattice mismatch,在超過臨界厚度後,會因應力回復造成不相稱差排而產生缺陷。本論文我們以深層能階暫態頻譜、暫態電容的量測、導納頻譜量測、Xray繞射儀與光激光(Photoluminescence,),研究以有機金屬化學氣相沈積法(MOCVD)成長的GaAs0.982N0.018/GaAs 單一量子井結構(Single Quantum Well,SQW)的晶格匹配、載子分佈、不相稱差排的缺陷、缺陷能階與能帶問題。 透過低溫(10K)Photoluminescence的能帶分析,我們發現到因量子侷限效應造成強烈的Blueshift,隨著井厚度的增加,GaAs0.982N0.018的PL光強度遞減,在此溫度下的GaAs對應的能量為1.51eV,並有因長晶時DMHY分解不完全所殘留的碳(Carbon),在10K溫度其所對應的PL能量為1.49eV,對於GaAs而言,C會取代As而形成P-type;X-ray Rocking curve得知此SQW結構井厚度在295A已產生部分晶格鬆弛,造成的晶格不匹配,產生差排,然而當井厚度增大時,因晶格鬆弛造成的差排並沒有顯著提高,推測可能是由於有碳的存在抑制了差排;藉由缺陷量測,我們發現在臨界厚度以內沒有主要載子缺陷,在大於臨厚度則有主要載子的缺陷,在溫度為350K、240K、80K左右,缺陷的活化能分別約為0.51eV、0.44eV~0.48eV、0.16eV。藉由電容電壓的量測,我們得知載子的分布,估算出GaAs0.982N0.018/GaAs此單一量子井結構的Band Offset ΔEc約為0.28eV,ΔEv約為-50meV,為type-II的能帶關係;從光學和電性分析我們得知GaAs0.982N0.018/GaAs單一量子井結構的臨界厚度約在175A到295A之間。zh_TW
dc.description.abstractThe hetrostructure of GaAsN/GaAs quantum well has a relatively large condouction-band offset and is a suitable material for long-wavelength laser diodes(lasing at 1.3~1.5μm or longer wavelengths). However when well thickness increase beyond the critical thickness, lattice relaxation occurrs and the carrier depletion around the quantum well is observed . The photoluminescence reveals a strong blueshift of GaAs0.982N0.018/GaAs quantum emission . The X-ray rocking curve show that the critical thickness of GaAs0.982N0.018/GaAs single quantum well is around 175A~295A . Based on the concerntration profile ,we obtain that the conduction-band offset ΔEc of GaAs0.982N0.018/GaAs single quantum well is around 0.28eV and the ΔEv is around 50meV . The band diagram of GaAs0.982N0.018/GaAs single quantum well is shown to be Type-II . Three deep levels(active energy 0.51、0.44~0.48 and 0.16eV) are observed by DLTS in relaxed samples .en_US
dc.language.isozh_TWen_US
dc.subject量子井結構的電性及光學分析zh_TW
dc.subject晶格鬆弛zh_TW
dc.subject砷化鎵/氮砷化鎵/砷化鎵zh_TW
dc.subject臨界厚度zh_TW
dc.subject深能階暫態頻譜分析zh_TW
dc.subject薄膜雙晶繞射量測zh_TW
dc.subject導納頻譜分析zh_TW
dc.subject晶格錯位zh_TW
dc.subjectElectrical and optical characteristics of GaAs/GaAs0.982N0.018/GaAsen_US
dc.subjecta relatively large condouction-band offseten_US
dc.subjectthe critical thicknessen_US
dc.subjectphotoluminescenceen_US
dc.subjectX-ray rocking curveen_US
dc.subjectDimethylhydrazineen_US
dc.subjectDeep Level Transient Spectroscopeen_US
dc.subjecttype-IIen_US
dc.title砷化鎵/氮砷化鎵/砷化鎵 量子井結構的電性及光學分析zh_TW
dc.titleElectrical and optical characteristics of GaAs/GaAs0.982N0.018/GaAsen_US
dc.typeThesisen_US
dc.contributor.department電子物理系所zh_TW
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