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Introduction to Optical and Optoelectronic Properties of Nanostructures PDF

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“FM” — 2019/2/7 — 15:21 — page 1 — #1 IntroductiontoOpticalandOptoelectronicPropertiesofNanostructures Get to grips with the fundamental optical and optoelectronic properties of nano- structures.Thiscomprehensiveguidemakesawidevarietyofmoderntopicsacces- sible,includingup-to-datematerialontheopticalpropertiesofmonolayercrystals, plasmonics, nanophotonics, ultraviolet quantum well lasers, and wide-bandgap materials and heterostructures. The unified, multidisciplinary approach makes it idealforthoseindisciplinesspanningnanoscience,physics,materialsscience,and optical,electrical,andmechanicalengineering. BuildingonworkfirstpresentedinQuantumHeterostructures(Cambridge1999), this volume draws on years of research and teaching experience. Rigorous cover- age of basic principles makes it an excellent resource for senior undergraduates, and detailed mathematical derivations illuminate concepts for graduate students, researchers, and professional engineers. The examples with solutions included in thetextandend-of-chapterproblemsallowstudentstousethistexttoenhancetheir understanding. VladimirV.MitinisaSUNYDistinguishedProfessorintheDepartmentofElectrical Engineering and in the Department of Physics at the University at Buffalo, State UniversityofNewYork. Viacheslav A. Kochelap is Professor of Theoretical Physics and Head of the The- oretical Physics Department at the Institute of Semiconductor Physics, National AcademyofSciencesofUkraine. MitraDuttaistheViceChancellorforResearchandaUniversityDistinguishedPro- fessor at the University of Illinois at Chicago and also holds appointments in the DepartmentsofElectronicandComputerEngineeringandPhysics. MichaelA.StroscioisaUniversityDistinguishedProfessorandRichardandLoan HillProfessorattheUniversityofIllinoisatChicagoandalsoholdsappointments intheDepartmentsofElectricalandComputerEngineering,Bioengineering,and Physics. “FM” — 2019/2/7 — 15:21 — page iii — #3 Introduction to Optical and Optoelectronic Properties of Nanostructures VLADIMIR V. MITIN UniversityatBuffalo,StateUniversityofNewYork VIACHESLAV A. KOCHELAP LashkaryovInstituteofSemiconductorPhysics,Ukraine MITRA DUTTA UniversityofIllinoisatChicago MICHAEL A. STROSCIO UniversityofIllinoisatChicago “FM” — 2019/2/7 — 15:21 — page iv — #4 UniversityPrintingHouse,CambridgeCB28BS,UnitedKingdom OneLibertyPlaza,20thFloor,NewYork,NY10006,USA 477WilliamstownRoad,PortMelbourne,VIC3207,Australia 314–321,3rdFloor,Plot3,SplendorForum,JasolaDistrictCentre,NewDelhi–110025,India 79AnsonRoad,#06-04/06,Singapore079906 CambridgeUniversityPressispartoftheUniversityofCambridge. ItfurtherstheUniversity’smissionbydisseminatingknowledgeinthepursuitof education,learning,andresearchatthehighestinternationallevelsofexcellence. www.cambridge.org Informationonthistitle:www.cambridge.org/9781108428149 DOI:10.1017/9781108674522 ©CambridgeUniversityPress2019 Thispublicationisincopyright.Subjecttostatutoryexception andtotheprovisionsofrelevantcollectivelicensingagreements, noreproductionofanypartmaytakeplacewithoutthewritten permissionofCambridgeUniversityPress. Firstpublished2019 PrintedintheUnitedKingdombyTJInternationalLtd,PadstowCornwall AcataloguerecordforthispublicationisavailablefromtheBritishLibrary. LibraryofCongressCataloging-in-PublicationData ISBN978-1-108-42814-9Hardback CambridgeUniversityPresshasnoresponsibilityforthepersistenceoraccuracyof URLsforexternalorthird-partyinternetwebsitesreferredtointhispublication anddoesnotguaranteethatanycontentonsuchwebsitesis,orwillremain, accurateorappropriate. “FM” — 2019/2/7 — 15:21 — page v — #5 Contents Preface pageix 1 SomeTrendsinOptoelectronics 1 2 MaterialsforOptoelectronicApplications 9 2.1 Introduction 9 2.2 Semiconductors 9 2.3 CrystalLattices:BondinginCrystals 12 2.4 ElectronEnergyBands 18 2.5 SemiconductorHeterostructures 28 2.6 Lattice-MatchedandLattice-MismatchedMaterials 31 2.7 Lattice-Matched and Pseudomorphic Heterostructures, Si/Ge Heterostructures,andLattice-MatchedIII–VHeterostructures 37 2.8 Wide-BandgapMaterialsandHeterostructures 40 2.9 QuantumDots 45 2.10 Two-Dimensional Monolayer Crystals (Graphene, Silicene, Germanene, Tinene, Black Phosphorus, Monochalcogenides, Dichalcogenides,Trichalcogenides,andBoronNitrides) 50 2.11 ClosingRemarkstoChapter2 56 2.12 ControlQuestions 58 3 ElectronsinQuantumStructures 60 3.1 Introduction 60 3.2 QuantumWells 61 3.3 ElectronsinSingle-andFew-MonolayerCrystals 69 3.4 QuantumWires 80 3.5 QuantumDots 84 3.6 CouplingbetweenQuantumWells 90 3.7 Superlattices 98 3.8 ExcitonsinQuantumStructures 104 3.9 Nanostructure-BasedMaterialsAreReconfigurableNanomaterials 114 3.10 ClosingRemarkstoChapter3 122 3.11 ControlQuestions 124 “FM” — 2019/2/7 — 15:21 — page vi — #6 vi Contents 4 Light–SemiconductorMaterialsInteraction 125 4.1 Introduction 125 4.2 ElectromagneticWavesandPhotons 125 4.3 LightInteractionwithMatter:Phototransitions 136 4.4 OpticalPropertiesofBulkSemiconductors 142 4.5 ClosingRemarkstoChapter4 166 4.6 ControlQuestions 166 5 OpticsofQuantumStructures 168 5.1 Introduction 168 5.2 OpticalPropertiesofQuantumStructures 168 5.3 IntrabandTransitionsinQuantumStructures 182 5.4 OpticalPropertiesofTwo-Dimensional(Few-Monolayer)Crystals 193 5.5 TheOpticsofQuantumDots 205 5.6 ClosingRemarkstoChapter5 208 5.7 ControlQuestions 209 6 Electro-OpticsandNonlinearOptics 211 6.1 Introduction 211 6.2 Electro-OpticsinSemiconductors 212 6.3 TerahertzCoherentOscillationsofElectronsinanElectricField 225 6.4 NonlinearOpticsinHeterostructures 228 6.5 PlasmonicsanditsPeculiaritiesinNanostructures 238 6.6 ClosingRemarkstoChapter6 257 6.7 ControlQuestions 258 7 Light-EmittingDevicesBasedonInterbandPhototransitionsin QuantumStructures 260 7.1 Introduction 260 7.2 LightAmplificationinSemiconductors 260 7.3 Light-EmittingDiodesandLasers 279 7.4 BlueandUltravioletLight-EmittingDiodes 297 7.5 QuantumWireandQuantumDotEmittersandLasers 317 7.6 ClosingRemarkstoChapter7 329 7.7 ControlQuestions 330 8 DevicesBasedonIntrabandPhototransitionsinQuantumStructures andSiliconOptoelectronics 331 8.1 Introduction 331 8.2 UnipolarIntersubbandQuantum-CascadeLasers 332 8.3 TerahertzCascadeLasers 336 8.4 PhotodetectorsBasedonIntrabandPhototransitions 340 8.5 SiliconPhotonics 349 “FM” — 2019/2/7 — 15:21 — page vii — #7 Contents vii 8.6 PerspectivesofOptoelectronicDevicesBasedon Two-DimensionalCrystals 353 8.7 AdaptivePhotodetectors 360 8.8 ClosingRemarkstoChapter8 370 8.9 ControlQuestions 370 AppendixABasicStatementsandFormulaeofQuantumPhysics 373 AppendixBTablesofUnits 386 AppendixC ListofPertinentSymbols 389 FurtherReading 391 Index 401 “FM” — 2019/2/7 — 15:21 — page ix — #9 Preface Therearemanymonographsandtextbooksdevotedtonanostructuresandnano- electronics.Itisgenerallyacceptedthatmicrostructurescienceandtechnologydeal withmicrostructureswithsizesdownto0.1micrometer,whilesizesbelow100nm (0.1micrometer)areconsideredinnanoscienceandnanoelectronics.Nanoelectron- ics was and is predominantly driven by applications in processors and memories ofcomputersandtheirfollow-onsystems.Thisiswhytheoverwhelmingmajority oftextbooksdealwiththeprogressinthetechnology,coveringso-calledtop-down technologywhichproducesnanostructuresandnanostructuredeviceswhosecritical dimensionsarereducedtolessthan100nm.Textbookshavedevotedlessattention totheopticalpropertiesandoptoelectronicsofnanostructures,thesubjectofthis book. A new burst of basic research and applications of nanostructures was stimu- latedin2004bya“scotchtape”technologyinwhichasinglelayerofgraphenewas obtainedbypeelingitfromagraphitesurface.Thesimplicityof“scotchtape”tech- nologyandtheveryunusualpropertiesofgrapheneinitiatedinterestinstructures withathicknessofoneatomiclayer.Manymaterialshaveweakbondingbetween the layers, and monolayers or bilayers can easily be produced with “scotch tape” technology.Inspiteofthefactthatthe“scotchtape”technologyisnotapplicable forindustrialproduction,itisconvenientandinexpensiveforwideuseinresearch. Thesemonolayerstructuresdemonstratedinterestingelectrical,optical,andopto- electronicproperties.Todaydifferentmethodsoffabricationofgraphenehavebeen developed, including epitaxial technologies. A number of other one-atom-thick material structures have been discovered and studied. These monolayer materials constitute a new class of two-dimensional crystals which complements conven- tional two-dimensional heterostructures. Industrially applicable technologies for thesestructuresarecurrentlyunderactivedevelopment. Modern educational programs need to address the rapidly evolving facets of nanoscience and nanotechnology. A new generation of researchers, technologists, andengineershastobetrainedintheemergingnano-disciplines.Withthepurpose ofcontributingtoeducationinthenano-fields,wepresentthistextbookproviding aunifyingframeworkforthebasicideasneededtounderstandrecentdevelopments underlyingtheopticalandoptoelectronicpropertiesofnanostructures.Thisbook grew out of the authors’ research and teaching experience in these subjects. We havefoundthatmanyoftheideasandachievementscanbeexplainedinarelatively “FM” — 2019/2/7 — 15:21 — page x — #10 x Preface simplesetting.Wehavedesignedthistextbookprimarilyforseniorundergraduate students and first-year graduate students, who will have been trained in different fields,includingnanoscience,physicsandopticalengineering,materialsscienceand engineering,andmechanicalengineering.Toreachsuchabroadaudience,materials arepresentedinsuchawaythataninstructorcanchoosethelevelofpresentation dependingonthebackgroundsofthestudents.Weincludedetailsofderivationsand themathematicaljustificationofconceptsinsomesections.Thesedetailedsections may be omitted in an undergraduate curriculum. The book contains some solved examplesinthetextandcontrolquestionsforstudentself-evaluationattheendof eachchapter. Althoughthisbookhasbeenwrittenbasicallyforthestudent,thematerialpre- sentedinChapters4–8shouldbeusefulforawideaudienceofresearchersworking ondifferentsubjectswithinthemultidisciplinaryareaofnanoscience.Thecoreof this textbook is in Chapters 4–8 but, in order to make the book self-contained, we give in Chapters 1–3 the relevant background material on nanostructures and their electronic properties. Appendix A discusses the Schrödinger wave equation forparticlesandcontainsmajorrelationsandequationsfromquantummechanics. AppendixBincludestablesofunitsaswellasmajorphysicalconstants. In Chapter 1, we present in concise form the main subject of the book, namely the recent and diverse trends in nanotechnologies; novel concepts of nanodevices arealsoreviewedbriefly.Thesetrendsmakeitclearwhyunderstandingthefunda- mentalsoftheopticsandoptoelectronicsofnanostructuresisofgreatimportance. Chapters 2 and 3 have been written for students who have not taken courses in nanoelectronics. InChapter2,wepresentanoverviewofthebasicmaterialsthatareexploitedin nanoelectronics.Weintroducethemajorpropertiesofsemiconductorsandmateri- alsthatdemonstrategreatpotentialforapplicationinnanoelectronicsandoptoelec- tronics. Special attention is paid to carbon nanotubes, graphene, transition-metal dichalcogenidesandothersingle-atomic-layermaterials. In Chapter 3, we discuss the basic physical concepts related to the behavior of particlesinthenanoworld.Keepinginmindthediversevariantsofnanostructures, we analyze a number of particular examples which highlight important quantum properties of particles in heterostructures. Recently, substantial efforts in research have been made in the area of reconfigurable materials. The last section in Chap- ter 3 briefly describes three examples of reconfigurable materials based on nanos- tructures, namely on graphene, quantum wells, and quantum dots. Many of the examples analyzed can serve as the simplest underlying models of nanostructures thatareexploitedinlaterchapters. For supplemental information on the fundamentals presented in Chapters 2 and 3, students can refer to the following recent books: Quantum Mechanics for Nanostructures, V. Mitin, D. Sementsov, and N. Vagidov, Cambridge University Press,2010,IntroductiontoNanoelectronics:Nanotechnology,Engineering,Science, and Applications, V. Mitin, V. Kochelap, and M. Stroscio, Cambridge University “FM” — 2019/2/7 — 15:21 — page xi — #11 Preface xi Press, 2008, and Quantum Heterostructures: Microelectronics and Optoelectronics, V.Mitin,V.Kochelap,andM.Stroscio,CambridgeUniversityPress,1999. Chapter4coversthepropertiesoflightandlight–semiconductorinteractions.We start with a brief review of the basic concepts of electromagnetic fields. We define the classical characteristics of electromagnetic fields, such as the energy, intensity, anddensityofstates,andweintroducetheconceptofthequantaofthesefields–the photons.Byanalyzingelectromagneticfieldsinfreespaceandinopticalresonators, weshowthatresonatorsdrasticallychangethestructureandthebehaviorofelec- tromagnetic fields. Next we study the interaction of light with matter and define three principal optical processes: spontaneous emission, stimulated emission, and stimulatedabsorption.Wereviewtheopticalpropertiesofbulksemiconductorsand define the major optical characteristics of semiconductors, with specific emphasis ontheIII–Vcompounds. Chapter 5 emphasizes that the electrodynamics of heterostructures differs from thatofbulkmaterials.Thespatialnonuniformitycausesspecificcharacteristicsof the interaction of light with matter, including light propagation, absorption, etc. We introduce several parameters which characterize the interaction of light with matterfordifferentcasesoflightpropagation.Theparametersforlightabsorption are calculated for type-I heterostructure quantum wells. The optical properties of monolayermaterialsarediscussed.Variousfactorsaffectingtheopticalproperties of low-dimensional electrons, such as the broadening of spectra due to intraband scatteringprocesses,excitoniceffects,etc.,areanalyzedinthischapter. Chapter 6 discusses the influence of an external electric field on the refractive index and the absorption coefficient, i.e., the effect of the electric field on the propagation of light through a material or on the reflection of the light, which is known as the electro-optical effect. We study the electro-optical effect for quan- tumheterostructuresincludingquantumwells,double-andmultiple-quantum-well structures, and superlattices. We consider the quantum-confined Stark effect, the Burstein–Moss effect, and the effect of destroying excitons in gated heterostruc- tures. We show that electro-optical effects have great potential for optoelectronic applications using the electric field to control light and for realizing the tunable generation of microwave emission. We consider nonlinear optical effects in quan- tum heterostructures that occur at high intensities of light. Also in Chapter 6 we present a new emerging branch of the subject – plasmonics for optoelectronics. We discuss subwavelength light phenomena, which involve surface plasmons and plasmonexcitationinlow-dimensionalelectrongases. Chapters7and8aredevotedtotheapplicationsofnanostructures.Weanalyze theeffectofopticalconfinement.Ourdiscussionfocusesonheterostructureswhich facilitatethesimultaneousformationofopticalmodesandtherealizationoflaser oscillations which convert electric power into laser emission. A variety of differ- ent laser designs are analyzed, such as: quantum well and quantum wire lasers, includingdevicesoperatingintheterahertz(THz),infrared,visible,andultraviolet spectralregions;thequantumcascadelaser;andsingle-monolayerphotodetectors and emitters. In particular, we consider ultraviolet-emitting devices based on the

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