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Iron-based Superconductors: Materials, Properties and Mechanisms PDF

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“In February 2008, Dr. Hosono and coworkers broke the striking news that they had found a new superconductor, LaFeAsO F with T = 26 K. This news immediately spread out in 1–x x c the world, and soon after its T was increased to 55 K. This breakthrough rekindled the c edited by superconducting research, which was in a state of dying fire after the discovery of Cu I oxide superconductor in 1988 and MgB in 2001. This book presents a comprehensive R Nan-Lin Wang 2 review on the present status of Fe-pnictide superconductors, including the material, a O Hideo Hosono variety of experimental results (photoemission, neutron scattering, NMR, etc.), theory, and so forth.” N Pengcheng Dai Dr. Jun Akimitsu Aoyama Gakuin University, Japan - B “The timely appearance of the first review volume on iron-based superconductors will greatly promote research on this exciting subject. The authors’ undisputable expertise A guarantees its lasting value.” S Prof. Lu Yu Chinese Academy of Sciences, China E “The balance between early and recent developments establishes this book as an D excellent source of information for both beginners and advanced researchers.” Prof. Elbio Ruben Dagotto S University of Tennessee, USA U Iron-based superconductors, compared with cuprate superconductors, are much more P flexible and have a large variety of parent compounds. From the point of view of fundamental physics, they have properties that are more amenable to band structure E calculations. This allows a quantitative comparison with experiments. In addition, iron- R based superconductors have intrinsic properties favorable for certain applications, such as inertness to impurities, large and isotropic upper critical fields, and strong grain C boundaries. This book reviews the progress made in this fascinating field. The contributors O are leading experts in their fields. The text is a good guide for understanding materials, physical properties, and superconductivity mechanism. Students and beginners will find N it quite useful for familiarizing themselves with the recent progress made in this field. D Nan-Lin Wang is a professor and group leader at the Institute of Physics, Chinese Academy of Sciences, China. He leads a group that explores novel U superconducting and other strongly correlated materials, grows single C crystals, and investigates their electronic properties, particularly with optical spectroscopic techniques. T O MATERIALS, PROPERTIES, AND MECHANISMS Hideo Hosono is a professor at Frontier Research Center and Materials and Structures Laboratory, Tokyo Institute of Technology, Japan. His major concern R IRON-BASED is to create novel electro-active materials, including superconductors based S on his own idea. He is a pioneer of transparent oxide semiconductors. Iron- based superconductors were discovered by his group in 2006–2008. SUPERCONDUCTORS Pengcheng Dai is a professor of physics at the University of Tennessee- Knoxville, USA, and the Institute of Physics, Chinese Academy of Sciences. Wang His interest is to use neutron scattering as a probe to study correlated Hosono electron materials, including high-temperature superconductors. Dai V149 ISBN-13 978-981-4303-22-4 CRC Press Taylor & Francis Group 6000 Broken Sound Parkway NW, Suite 300 Boca Raton, FL 33487-2742 © 2013 by Taylor & Francis Group, LLC CRC Press is an imprint of Taylor & Francis Group, an Informa business No claim to original U.S. Government works Version Date: 20121207 International Standard Book Number-13: 978-9-81430-323-1 (eBook - PDF) This book contains information obtained from authentic and highly regarded sources. Reason- able efforts have been made to publish reliable data and information, but the author and publisher cannot assume responsibility for the validity of all materials or the consequences of their use. The authors and publishers have attempted to trace the copyright holders of all material reproduced in this publication and apologize to copyright holders if permission to publish in this form has not been obtained. If any copyright material has not been acknowledged please write and let us know so we may rectify in any future reprint. Except as permitted under U.S. Copyright Law, no part of this book may be reprinted, reproduced, transmitted, or utilized in any form by any electronic, mechanical, or other means, now known or hereafter invented, including photocopying, microfilming, and recording, or in any information storage or retrieval system, without written permission from the publishers. For permission to photocopy or use material electronically from this work, please access www. copyright.com (http://www.copyright.com/) or contact the Copyright Clearance Center, Inc. (CCC), 222 Rosewood Drive, Danvers, MA 01923, 978-750-8400. CCC is a not-for-profit organiza- tion that provides licenses and registration for a variety of users. For organizations that have been granted a photocopy license by the CCC, a separate system of payment has been arranged. Trademark Notice: Product or corporate names may be trademarks or registered trademarks, and are used only for identification and explanation without intent to infringe. Visit the Taylor & Francis Web site at http://www.taylorandfrancis.com and the CRC Press Web site at http://www.crcpress.com October10,2012 9:37 PSPBook-9inx6in 00-Wang–prelims Contents Preface xiii 1 Iron-BasedSuperconductors:DiscoveryandProgress inMaterials 1 HideoHosono 1.1 Introduction 1 1.2 SmallHistoryonDiscoveryandProgressinParent Materials 3 1.3 CrystalStructureofParentMaterials 6 1.3.1 1111-TypeMaterials(LnFePnO,Ln: Lanthanide) 6 1.3.2 122-TypeMaterials(AeFe Pn ,Ae:Alkaline 2 2 EarthorEu) 9 1.3.3 111-TypeMaterials(AFePn,A:AlkaliMetal) 10 1.3.4 11-TypeMaterials(Fe1+xSe) 10 1.3.5 Homologous-TypeMaterials: (Fe2As2)(Aen+1MmOy) 10 1.4 ParentMaterialandSuperconductivity 11 1.4.1 DopingEffect 11 1.4.1.1 The1111-type 12 1.4.1.2 The122-type 15 1.4.2 LocalStructureandT 20 c 1.5 UniqueCharacteristicsofFeSCs 23 1.5.1 Multi-BandNatureofFe3d 23 1.5.2 ParentMaterial:AntiferromagneticMetal 24 1.5.3 ImpurityRobustT 25 c 1.5.4 LargeCriticalFieldandSmallAnisotropy 25 1.5.5 AdvantageousGrainBoundaryNature 26 October10,2012 9:37 PSPBook-9inx6in 00-Wang–prelims vi Contents 1.6 SingleCrystal 27 1.6.1 Growthof1111-TypeCrystals 27 1.6.2 Growthofthe122-TypeCrystals 29 1.6.3 CharacteristicsofaSingleCrystal 30 1.7 ThinFilm 32 1.7.1 1111-TypeCompounds 32 1.7.2 122-TypeCompounds 35 1.7.3 11-TypeCompounds 38 1.8 SummaryandRelevantNewSuperconductors 40 2 SynthesisandPhysicalPropertiesoftheNew PotassiumIronSelenideSuperconductorK Fe Se 53 0.80 1.76 2 R.Hu,E.D.Mun,D.H.Ryan,K.Cho,H.Kim,H.Hodovanets, W.E.Straszheim,M.A.Tanatar,R.Prozorov, W.N.Rowan-Weetaluktuk,J.M.Cadogan, M.M.Altarawneh,C.H.Mielke,V.S.Zapf,S.L.Bud’ko, andP.C.Canfield 2.1 Introduction 54 2.2 ExperimentalMethods 55 2.3 CrystalGrowthandStoichiometry 57 2.4 PhysicalPropertiesofSingleCrystalsofK0.80Fe1.76Se2 59 2.4.1 TransportandThermodynamicProperties 59 2.4.2 LondonPenetrationDepthand Magneto-OpticalImaging 64 2.4.3 AnisotropicH (T) 66 c2 2.4.4 57FeMo¨ssbauerSpectroscopy 71 2.4.5 PhaseSeparationandPossible SuperconductingAerogel 79 2.5 Summary 80 3 Angle-ResolvedPhotoemissionSpectroscopyofIron Pnictides 89 TakafumiSato,PierreRichard,KosukeNakayama, TakashiTakahashi,andHongDing 3.1 Introduction 90 3.1.1 PrincipleofARPES 91 3.2 ExperimentalResults 93 3.2.1 FermiSurfaceandPairingSymmetry 93 3.2.1.1 Hole-dopedsystem 93 3.2.1.2 Electron-dopedsystem 104 October10,2012 9:37 PSPBook-9inx6in 00-Wang–prelims Contents vii 3.2.2 Many-BodyInteractions 108 3.2.3 ParentCompound 112 3.3 ConcludingRemarksandSummary 115 4 QuantumOscillationsinIronPnictide Superconductors 125 SuchitraE.Sebastian 4.1 QuantumOscillations 126 4.1.1 AngularDependence 128 4.1.1.1 Fermisurfacegeometry 128 4.1.1.2 Spinsplitting 128 4.2 MagneticFieldDependence 129 4.3 TemperatureDependence 130 4.4 IronPnictideSuperconductors 131 4.5 QuantumOscillationsinAntiferromagneticParent IronPnictides 131 4.5.1 FermiSurfaceGeometry:Nonmagneticand AntiferromagneticBandStructureCalculations 134 4.5.2 ExperimentalComparisonwithBandStructure 137 4.5.3 DiracNodes 141 4.6 QuantumOscillationsinOverdopedParamagnetic IronPnictides 142 4.6.1 Quasi-NestingofHoleandElectronCylinders 144 4.7 CupratesandIronPnictides:ElectronicStructure Comparison 146 4.7.1 EnhancementinLindhardFunctionin PnictidesandCuprates 147 4.7.2 QuantumCriticalPointunderSuperconducting Dome 149 4.8 Conclusion 152 5 OpticalInvestigationonIron-BasedSuperconductors 161 Nan-LinWangandZhi-GuoChen 5.1 Introduction 161 5.2 IntroductionAboutOpticalPropertiesofSolids 164 5.2.1 OpticalConstants 164 5.2.2 InterbandandIntrabandExcitations 166 5.2.3 DrudeModelandDrude-LorentzModel 168 5.2.4 ExtendedDrudeModel 170 October10,2012 9:37 PSPBook-9inx6in 00-Wang–prelims viii Contents 5.2.5 SumRules 172 5.2.6 OpticalResponseofBrokenSymmetryStates ofMetals 174 5.3 OpticalStudiesontheParentCompounds 176 5.3.1 SpinDensityWaveGapinFeAs-Based Compounds 177 5.3.2 AbsenceofSDWGapinFeTe1+x 182 5.3.3 FullyLocalizedFe3dElectronsinK0.8Fe1.6Se2 184 5.4 Multi-Componentsvs.ExtendedDrudeModel AnalysisofOpticalConductivity 186 5.5 ElectronCorrelationsinthe Fe-Pnictides/Chalcogenides 192 5.5.1 KineticEnergyReductionbyElectron Correlations 192 5.5.2 EffectofHund’sCoupling 196 5.6 AnisotropicChargeDynamics 201 5.6.1 c-AxisOpticalPropertiesinParent Compounds 201 5.6.2 AnisotropicOpticalPropertieswithin ab-Plane 204 5.6.3 c-AxisOpticalPropertiesofSuperconducting Compounds 209 5.7 OpticalPropertiesofIron-BasedSuperconductors BelowT 214 c 5.7.1 ProbingtheSuperconductingEnergyGaps 214 5.7.2 JosephsonCouplingPlasmoninKxFe2−ySe2 223 5.7.3 Superconductivity-InducedSpectralWeight Transfer 226 5.7.4 CoherentPeakBelowT ProbedbyTHz c Spectroscopy 230 6 AntiferromagneticSpinFluctuationsintheFe-Based Superconductors 243 ShiliangLiandPengchengDai 6.1 Introduction 244 6.2 AntiferromagnetisminParentCompounds 246 6.2.1 Long-RangeAntiferromagneticOrder 246 6.2.2 SpinWaves 249 6.2.3 DestructionofAntiferromagneticOrder 253 October10,2012 9:37 PSPBook-9inx6in 00-Wang–prelims Contents ix 6.3 MagneticExcitationsintheSuperconductingState 256 6.3.1 MagneticResonance 257 6.3.2 FieldEffectonMagneticResonance 261 6.3.3 Field-InducedMagnetization 264 6.4 MagneticExcitationsintheNormalState 264 6.4.1 In-PlaneAnisotropyinthe“122”System 264 6.4.2 IncommensurateMagneticExcitationsinthe “11”System 265 6.5 Conclusion 268 7 ReviewofNMRStudiesonIron-Based Superconductors 275 KenjiIshidaandYusukeNakai 7.1 Introduction 275 7.2 NMRBasics 276 7.2.1 NMRHamiltonian 276 7.2.2 KnightShiftandNuclearSpin-Lattice RelaxationRateinMetals 278 7.2.3 KnightShiftandNuclearSpin-Lattice RelaxationRateintheSuperconductingState 281 7.3 NMRExperimentalResultsonIron-Based Superconductors 287 7.3.1 LaFeAs(O1−xFx)andLaFeAsO1−δwith“1111” Structure 287 7.3.1.1 LaFeAsO:parentcompound 288 7.3.1.2 NormalstateofLaFeAs(O1−xFx)and LaFeAsO1−δ 291 7.3.1.3 Superconductingstateof LaFeAs(O1−xFx)andLaFeAsO1−δ 299 7.3.2 NMRStudyin“122”System 305 7.3.2.1 BaFe As 307 2 2 7.3.2.2 NMRinthenormalstateof BaFe2(As1−xPx)2 313 7.3.2.3 NMRinthenormalstateof Ba(Fe1−xCox)2As2 319 7.3.2.4 NMRinthenormalstateof (Ba1−xKx)Fe2As2 323 7.3.2.5 NMRresultsonthesuperconducting stateof“122”compounds 325

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