纳米激光器与单光子源调研报告

第一章激光器的小型 第二章单光子 第三章受激辐 第四章调研小 1962年第一代半导体激光pn结，到后来的双异质结，再后来量子阱，量子线，量子FP腔，到分布反馈腔，再到分第一章激光器的小型化17030快就剋想到SPPSPP就是指表面等离子波SurfacePlasmonPolariton这是一种TM电磁场和金些具体数值。其中最薄的结构是90nm的半导体芯区和两边厚度为20nm的SiN370nm比激射波长的685nm,要小。而把腔做的这么小，我们来看看它是怎么样工作44nm。我第二章单光子源数分布角度来看是单粒子的Fock均光子数为M，对于激光而言M平均光子数为（x为量子场）。是45°偏振的单光子通过偏振分束镜，达到半透半反的效果。量子保密通信中第一个密钥分发协议为BB8413550090°的偏振态，同时破坏原状态。同理，Z45°，135°的偏振态，但是得到45°或135°的偏振态，同时破坏原状态。端，Eve为窃听者，协议主要步骤如下。0。时空脉冲的概率趋近于1，其结果造成信噪比大幅恶化。脉冲中有5%为多光子。第三章受激辐射为InAs实验中，将GaAs衬底上做出一个个小的突起（Mesa），每个突起的InAs量子点置于GaAs衬底的突起上。这样的量子点之间的距离可以2.9ps，每个12端口（t2），为t1t2的时间差。I表示探测到的光强度。子的概率降为接近于0。第四章调研小结[1].Herd,R.M.,J.S.DoverandK.A.Arndt,Basiclaserprinciples.Dermatologicclinics,1997.p.355-[2].Fan,T.Y.andR.L.Byer,Diodelaser-pumpedsolid-statelasers.QuantumElectronics,IEEEJournalof,1988.24(6):p.895-912.[3].Garbin,B.,etal.,Incoherentopticaltriggeringofexcitablepulsesinaninjection-lockedsemiconductorlaser.Opticsletters,2014.39(5):p.1254-1257.[4].Ding,K.andC.Z.Ning,Metallicsubwavelength-cavitysemiconductornanolasers.Light:Science&Applications,2012.1(7):p.e20.[5].Ning,C.Z.,Semiconductornanolasers.physicastatussolidi(b),2010.247(4):p.774-[6].Zhang,J.,etal.,SinglePhotonsOn-demandfromLight-holeExcitonsinStrain-EngineeredQuantumDots.Nanoletters,2014.[7].Michler,P.,etal.,Aquantumdotsingle-photonturnstiledevice.Science,2000.290(5500):p.[8].Michler,P.,etal.,Aquantumdotsingle-photonturnstiledevice.Science,2000.290(5500):p.[9].Wei,Y.,etal.,DeterministicandRobustGenerationofSinglePhotonsFromaSingleQuantumDotwith99.5%IndistinguishabilityUsingAdiabaticRapidPassage.Nanoletters,2014.[10].Matsukevich,D.N.,etal.,Deterministicsinglephotonsviaconditionalquantumevolution.Physicalreviewletters,2006.97(1):p.013601.[11].Michler,P.,etal.,Quantumcorrelationamongphotonsfromasinglequantumdotatroomtemperature.Nature,2000.406(6799):p.968-970.[12].Benson,O.,etal.,Regulatedandentangledphotonsfromasinglequantumdot.PhysicalReviewLetters,2000.84(11):p.2513.[13].Moreau,E.,etal.,Single-modesolid-statesinglephotonsourcebasedonisolatedquantumdotsinpillarmicrocavities.AppliedPhysicsLetters,2001.79(18):p.2865-2867.[14].Kurtsiefer,C.,etal.,Stablesolid-statesourceofsinglephotons.PhysicalReviewLetters,2000.85(2):p.290.[15].Santori,C.,etal.,Triggeredsinglephotonsfromaquantumdot.PhysicalReviewLetters,2001.86(8):p.1502.[16].Brunel,C.,etal.,Triggeredsourceofsinglephotonsbasedoncontrolledsinglemoleculefluorescence.PhysicalReviewLetters,1999.83(14):p.2722.McKeeverJ,BocaA,BoozerAD,etal.Deterministicgenerationofsinglephotonsfromoneatomtrappedinacavity[J].Science,2004,303(5666):1992-1994.LukishovaSG,SchmidAW,SupranowitzCM,etal.Dye-dopedcholesteric-liquid-crystalroom-temperaturesingle-photonsource[J].Journalofmodernoptics,2004,51(9-10):1535-1547.LukishovaSG,BissellLJ,MenonVM,etal.Organicphotonicbandgapmicrocavitiesdopedwithsemiconductornanocrystalsforroom-temperatureon-demandsingle-photonsources[J].JournalofModernOptics,2009,56(2-3):167-174.LukishovaSG,SchmidAW,KnoxR,etal.Roomtemperaturesourceofsinglephotonsofdefinitepolarization[J].JournalofModernOptics,2007,54(2-3):417-429.LukishovaSG,KnoxRP,FreivaldP,etal.Sin