凝聚态物理前沿讲座_方忠_Quantum Simulation in the F.ppt

《凝聚态物理前沿讲座_方忠_Quantum Simulation in the F.ppt》由会员分享，可在线阅读，更多相关《凝聚态物理前沿讲座_方忠_Quantum Simulation in the F.ppt（60页珍藏版）》请在淘文阁 - 分享文档赚钱的网站上搜索。

1、4/12/2023方方 忠忠中国科学院物理研究所，理论室中国科学院物理研究所，理论室 Quantum Simulation in the Field ofSpintronics and OrbitronicsAcknowledgement:Y.G.Yao,K.Terakura N.Nagaosa Y.Tokura凝聚态物理前沿讲座凝聚态物理前沿讲座4/12/2023 Contents 1.Quantum simulations based on DFT (1)Simple introduction to first-principles calculations (2)Our method,c

2、ode,and computer facilities 2.Dissipationless quantum current for spintronics (1)Anomalous Hall Effect (2)Spin Hall Current (3)Anomalous Nernst Effect 3.Orbiton and Orbitronics (1)Phase diagram of La1-xSrxMnO3 (2)Orbital-dependent phase control in Ca2-xSrxRuO4 (3)Magnetism in double perovskites 4.Su

3、rface of transition-metal oxides4/12/2023Quantum Simulation based on DFTAtoms+electronsElectronsMany-bodyElectronsSingle-particleDensityFunctionalAdiabatic ApproximationHohenberg-KohnKohn-ShamHellmann-FeynmanForce and StressMDSCF4/12/2023Self-consistent Solver for KS problemSCFLDAGGALDA+U4/12/2023LD

4、A+U method4/12/2023Pseudopotential SchemeNormal-conservingPseudopotentialUltra-SoftPseudopotential4/12/2023Virtual Crystal Approxmation(VCA)For virtual atomsSolve Schrodinger equationIonic unscreened potential4/12/2023How to solve the single particle problem Real Space (no FFT)Finite element Finite

5、difference Multi-grid Adaptive Wavelet Reciprocal Space (with FFT)LACO LMTO FLAPW PAW Plane-wave Greens function Pseudopotential,ASA,4/12/2023Other Problems in Simulations1.Exchange-correlation functional2.Strongly-correlated systems3.Force calculation&Molecular dynamics4.Magnetic,optical&electronic

6、 properties5.Excited States6.Non-equilibrium&Time-dependent process7.Order(N)method&Large scale8.Catalysis,Chemical reaction,Bio-systems9.4/12/20231.First-principles calculations based on DFT2.Plane-wave basis3.Ultra-soft Pseudo-potential4.LDA,GGA,LDA+U,etc5.Virtual crystal approximation(VCA)6.Real

7、space RMM for larger systems7.Full parallelization by MPI8.SGI,IBM-SP,Alpha,Cray,VPP,PC-ClusterOur Method4/12/2023 STATE Code:(Simulational Tool for Atom Technology)Main Contributors:Z.Fang,Y.Morikawa,T.Ikeda,H.Sawadaand other JRCAT membersFor details:Z.Fang,et.al,J.Phys:Cond.Matt.,14,3001(2001).(re

8、view article)100,000 lines,Accuracy 1meV/Atom,200 atoms.Widely used in Japan,Taiwan,Korea,Denmark,etc.4/12/2023IBM SP690,64 CPUs,128G,1T-disk4/12/2023Three Characters of Electron Charge Spin Orbitalwell known “hot”topic newExtensively used being used will be usedI,V,Charge currentCharge excitation s

9、pin wave orbitonCharge current spin current movement anisotropy functionality .4/12/2023SpintronicsThe electron has both charge and spin.Mostly only the charge property is used.Energy scale for the charge interaction is high,1eV,energy scale for the spin interaction is low,10-100 meV.Much lower powe

10、r consumption for spin-based device.Spin-based electronics also promises a greater integration between the logic and storage devices4/12/2023Problems for Spintronic devices spin injection into semiconductor Ohmic injection from ferromagnet Low efficiency(Difficulty):Ferromagnetic metal:conductivity

11、mismatch spin polarization is almost lost at interface.Ferromagnetic semiconductor (e.g.Ga1-xMnxAs):Curie temperature much lower than room temp.Ferromagnetic tunnel junction.spin detection by ferromagnet spin transport in semiconductor spin relaxation timeOptical pump and probe4/12/2023Only two know

12、n examples of dissipationless transport in solids!Supercurrent in a superconductor is dissipationless,since London equation related J to A,not to E!Vector potential=odd under T,charge current=odd under T.In the QHE,the Hall conductivity is proportional to the magnetic field B,which is odd under T.La

13、ughlin argument:all states below the fermi energy contribute to the Hall conductance.Streda formula,TKNN formula relates the Hall conductance to the 1st Chern number.4/12/2023New dissipationless transport in solidsdue to spin-orbital coupling!Anomalous Hall Effect(charge current):1 T.Jungwirth,et.al

14、.,PRL,88,207208(2002);2 Z.Fang,et.al,SCIENCE,302,92(2003)3 Y.G.Yao,et.al,PRL,92,37204(2004);4 W.L.Lee,et.al,SCIENCE,303,1647(2003)Conventional:xy =R0H +4RSM Intrinsic Mechanism:xyxy(M)Thus Jx=xyEy is T invariant J is odd,E is even,M is odd Dissipationless spin Hall current:1 S.Murakami,et.al,SCIENCE

15、,301,1348(2003);2 J.E.Hirsch,et.al.,PRL,83,1834(1999)3 J.Sinova,et.al,PRL,92,126603(2004)4 S.Q.Shen,et.al.,cond-mat/040305.5 Y.Xiong&X.C.Xie,cond-mat/0403083.Spin current is even under T4/12/2023BjHFMjAHEConventional HallAnomalous HallEESpinjSHEESpin Hall4/12/2023Merit of AHE and SHE 1.It works beca

16、use of spin-orbital coupling,which is active even at room T.2.It is entirely topological(dissipationless).4/12/2023 Spin-Orbital Coupling Berry Phase Magnetic Monopoles in Momentum SpaceAnomalous Hall current and Spin Hall current (Both are dissipationless)Intrinsic Mechanism4/12/2023Effective Hamil

17、tonian for adiabatic transportEquation of motion(Dirac monopole)Drift velocityTopological termNontrivial spin dynamics comes from the Dirac monopole at the center of k space,witheg=l:Adiabatic transport=potential V does not cause inter-band transitions only retain the intra-band matrix elements 4/12

18、/2023Full Quantum Calculations Based on Kubo FormularAnomalous Hall conductivitywithSpin Hall conductivityJys4/12/2023Conserved Spin Current(S.Murakami,et.al.,cond-mat/0310005)Conserved spinwhich satisfydefine current i,n,m =band index,=kramers doublets index4/12/2023Z.Fang,et.al.,SCIENCE 302,92(200

19、3)反常反常HallHall效应与动量空间中的磁单极效应与动量空间中的磁单极4/12/2023Calculated Gauge Flux for kz=0 in SrRuO3bz(kz=0)GMMMMZ.Fang,et.al,SCIENCE,302,92(2003)4/12/2023SrRuO34/12/2023SrRuO34/12/2023Calculated Spin Hall Current in GaAs4/12/2023Calculated Spin Current for GaAs and SnTe4/12/2023One Example for Half-MetalMnAs4/1

20、2/2023Fully spin polarized anomalous Hall current in MnAsSpin conductivityAHE conductivity4/12/2023Anomalous Nernst EffectBVFMVConventionalAnomalous4/12/2023Inverse Anomalous Nernst Effect:Cooling and refrigeratorFMHeat current jQExHeat current:Eq.of motion:4/12/2023egt2g3z2-r2x2-y2xyyzzxOrbitronics

21、4/12/2023Orbital Degrees of Freedom(ODF)EnergyDown spinUp spinEFO-2pO-2pt2gt2gegeg2-fold(ODF)3-fold“Half-metal”4/12/2023Various OrderingsFMA-typeC-typeG-typeLatticeSpinChargeOrbitalSC,TMR,CMR,M-I Transition,Anomalous Hall Effect,Magneto-optical,Ferroelectricity,Piezoelectricity,etc 4/12/2023Experime

22、ntalTheoreticalSCIENCE 288,462(2000).J.Phys.Soc.Jap.68,3790(1999).Phase Diagram of Tetragonal La1-xSrxMnO3(Controlling of Orbital and Spin Orderings)Z.Fang&K.Terakura,PRL 84,3169(2000).4/12/2023FMA-AFC-AFG-AFOrbital and Spin OrderingsPhysics:Spin Orbital Lattice Double exchange Super-exchange Compre

23、ssion Less conductivity4/12/2023Electric-Field-induced Orbital SwitchingK.Hatsuda,APL 83,3329(2003).4/12/2023LatticeSpinChargeOrbitalElectronic Structures of Ca2-xSrxRuO4EnergyDown spinUp spinEFO-2pO-2pt2gt2gegeg3-fold4/12/2023Ca2-xSrxRuO4:Isovalent substitution Rotation Rotation Rotation +Tilting T

24、ilting +CompressionAF MottInsulatorNearlyFM MetalS.Nakatsuji,et al.,PRLO.Friedt,et al.,PRB4/12/2023Issues:(1)How to understand the complicated phase diagram.(2)Whats the rule of orbital.4/12/2023Effects of Structure DistortionsZ.Fang&K.Terakura,PRB64,R20509(2001)Rotationxy orbitalVHSFMTiltingyz,zxne

25、stingAF4/12/2023Occupations and MagnetizationsZ.Fang et al.PRB(2004).4/12/2023Orbital Phase Diagram of Ca2-xSrxRuO4CaSrDoping x0.0 0.2 0.5 2.0EEfxyyz,zxEEfxyyz,zxEEfxyyz,zxxyxy ferro-orbital orderingAF,S=1 from yz,zxFM,S=1/2 from xyItinerant yz,zx with small SNM stateWith VHS from xy1.J.H.Jung,Z.Fan

26、g,et.al.,PRL 91,056403(2003).2.Z.Fang,et.al.,PRB 69,045116(2004).4/12/2023110RuO6 八面体在表面的旋转八面体在表面的旋转Sr2RuO4的表面电子结构的表面电子结构LEEDSTM1.R.Matzdorf,Z.Fang,et.al.,SCIENCE 289,746(2000).2.Z.Fang,et.al.,PRB 64,R20509(2001)4/12/2023PDOS of various doping x4/12/2023Exp.XASCalculated XAS90K300K4/12/2023Optical c

27、onductivityExperimentsCalculationsJ.H.Jung,Z.Fang,et al.PRL(2003).4/12/2023FeFeMSr2FeMO6(M=Mo,W,Re)8 1.Why Tc is so high for M=Mo,Re?2.Why M=W case is AF insulator?4/12/2023EFd statesd statesMajority spinMinority spinMo d stateor other p statesFMZ.Fang,et.al.,PRB 63,R180407(2001)EFd statesd statesMa

28、jority spinMinority spinMo d statesor other p statesAFNew Mechanism for Sr2FeMO6 and(Ga1-xMnx)As4/12/2023Fe(t2g)SpinEF M(t2g)(M=Mo,Re)Fe(t2g)Electronic Structure of Sr2FeMoO64/12/2023Surface of SrTiO3 with Oxygen Vacancy Important substrate Surface gas sensitivity Ferroelectricity Catalytically acti

29、ve4/12/2023STMSTST.Kubo,et.al.,PRL 86,1801(2001)H.Tanaka,et.al.,Jpn.J.Appl.Phys.32,1405(1993)4/12/20234/12/2023StructureChargeMagnetizationSrOTiO2Sr Ti OLDA+USurface of SrTiO3 with oxygen vacancy (Spin polarized surface)Z.Fang,et.al.,Surf.Sci.Lett.470,L75(2001)4/12/20234/12/2023SrO termination(GGA)T

30、iO2 termination(GGA)262626TiO2 termination(LDA+U)5 x 5 STM of SrTiO3 surface4/12/2023100100001001SurfaceCentral（La,Sr)O terminationMnO2 terminationMnOrbital polarization on the surfaces of La1-xSrxMnO3Z.Fang,et.al.,J.Phys.Soc.Jpn.70,3356(2001).4/12/2023 SummaryQuantum Simulation Charge Spin Orbital(Electronics)(Spintronics)(Orbitronics)Problems:1.Efficient method for cross-correlated systems 2.Towards large scale(surface&interface)3.Accurate method for many-body systems