納米激光器與單光子源調(diào)研報(bào)告

第一章激光器的小型 第二章單光子 第三章受激輻 第四章調(diào)研小 1962年第一代半導(dǎo)體激光pn結(jié)，到后來(lái)的雙異質(zhì)結(jié)，再后來(lái)量子阱，量子線，量子FP腔，到分布反饋腔，再到分第一章激光器的小型化17030快就剋想到SPPSPP就是指表面等離子波SurfacePlasmonPolariton這是一種TM電磁場(chǎng)和金些具體數(shù)值。其中最薄的結(jié)構(gòu)是90nm的半導(dǎo)體芯區(qū)和兩邊厚度為20nm的SiN370nm比激射波長(zhǎng)的685nm,要小。而把腔做的這么小，我們來(lái)看看它是怎么樣工作44nm。我第二章單光子源數(shù)分布角度來(lái)看是單粒子的Fock均光子數(shù)為M，對(duì)于激光而言M平均光子數(shù)為（x為量子場(chǎng)）。是45°偏振的單光子通過(guò)偏振分束鏡，達(dá)到半透半反的效果。量子保密通信中第一個(gè)密鑰分發(fā)協(xié)議為BB8413550090°的偏振態(tài)，同時(shí)破壞原狀態(tài)。同理，Z45°，135°的偏振態(tài)，但是得到45°或135°的偏振態(tài)，同時(shí)破壞原狀態(tài)。端，Eve為竊聽者，協(xié)議主要步驟如下。0。時(shí)空脈沖的概率趨近于1，其結(jié)果造成信噪比大幅惡化。脈沖中有5%為多光子。第三章受激輻射為InAs實(shí)驗(yàn)中，將GaAs襯底上做出一個(gè)個(gè)小的突起（Mesa），每個(gè)突起的InAs量子點(diǎn)置于GaAs襯底的突起上。這樣的量子點(diǎn)之間的距離可以2.9ps，每個(gè)12端口（t2），為t1t2的時(shí)間差。I表示探測(cè)到的光強(qiáng)度。子的概率降為接近于0。第四章調(diào)研小結(jié)[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