Hybridized Course on Condensed Matter Physics

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1 Hybridized Course on Condensed Matter Physics
Tao Xiang September

2 Course Time Table Panorama and basic models of Condensed Matter Theory
Sept 4 to Sept 9 (2 weeks) Tao Xiang Green's Function theory Sept 18 to Oct. 16 (4 weeks) Shao-Jing Qin Theory of quantum phase transition     Oct. 23 to Oct. 30 (2 weeks) Hong-Gang Luo Path integral and mean-field theory   Nov. 6 to Nov. 20 (3 weeks) Yue Yu Theory of mesoscopic phenomena Nov. 27 to Dec. 18 (4 weeks) Zhong-Yi Lu Selected topics: Quantum Hall effect, High-Tc superconductivity, Kondo problem, DFT, DMRG, etc Dec 25 to Jan (4 weeks)

3 What is Condensed Matter Physics?
Old believe: Solid state physics is the physics of dirt. Wolfgang Pauli

4 What is Condensed Matter Physics?
Modern Policy Maker’s definition: >1/3 of physics solid + liquid hard + soft matter: de Gennes structure + transport: the PRL division basis of materials science and engineering P W Anderson 1977诺贝尔物理奖 Father of “Condensed Matter”

5 What is Condensed Matter Physics?
Technicians’ definition: Methodology Simulations 1/3 Theories 1/6 Experiments 1/2

6 What is Condensed Matter Physics?
Functional definition: Applications New Materials New Technology New Fundamental Phenomena

7 What is Condensed Matter Physics?
Specialists’ definition: Universe of Complexities Elementary excitations: quasiparticles, phonon, spin waves, plasmons, excitons, spinons and holons, … Elementary interactions: el-el, el-ph, el-mag, … Elementary structures and phases: charge, spin, orbitals, ions: crystal, glass, liquid … Endless emergent quantum phenomena macroscopic quantum interference, mesoscopic size effects …

8 Relationship with other subjects
Particle Physics Condensed Matter Physics Field Theory Superstring Gravity Cosmology Materials Science Chemistry Information Computer Science Biology 还原论 (Reductionism)：自然界的一切都由其最基本的组成单元和规律所决定 呈展论（Emergence): 客观世界是分层次的，每个层次都有自己的基本规律

9 Reductionism：逐本求源

10 这是“大统一理论”的追求目标，但答案是否定的。
指数墙带来的困惑 由基本的相互作用力就能推出自然界的所有规律吗？ 这是“大统一理论”的追求目标，但答案是否定的。 指数墙问题 实际材料中原子数 N 1023 系统总的自由度数不是每个粒子自由度数相加，而是相乘！ 自由度随粒子数指数增加 Walter Kohn Nobel化学奖

11 Emergence：集体行为不是个体行为的简单相加
More Is Different 由基本粒子构成的巨大的和复杂的的集聚体的行为并不能依据少数粒子的性质作简单外推就能理解。正好相反，在复杂性的每一个层次之中会呈现全新的性质，而要理解这些新行为所需要作的研究，就其基础性而言，与其他研究相比毫不逊色。 Philip W. Anderson 1972

12 More Is Different！ 单元素 双原子 三原子 四原子 1 2 3 4 20
单元素 双原子 三原子 四原子 Si MgB NaCoO La2-xSrxCuO 简单生物 半导体 K超导体 K超导体 高温超导体 大分子

13 More Is Different！ 介观与生物的尺度关系图 米 10-10 10-5 10-9 10-7 10-6 10-8 10-4
单一分子 约 1 纳米 IBM 笔记本电脑750TM 微处理器 7.56 毫米×8.799 毫米 6.35×106液晶體 米 IC 中的铜线宽度 ~ 0.2 微米 紅血球 ~5 微米 DNA 蛋白质 ~ 纳米 细菌 1 m 纳米尺度之记忆元件 1012 位元/cm2 (1Tbit/cm2) 液晶体 线宽度 0.12 微米 藻类 30 微米 10-10 10-5 10-9 10-7 10-6 10-8 10-4 10-3 10-2 Photo credits, bio, L-R GFP: RCSB Protein Data Bank E.Coli: Dennis Kunkel Red Blood Cells: James A. Sullivan, Diatom: Dept of Biology, Indiana University Silicon, L-R CdSe nanocrystal: Andreas Kadavanich, Alivisatos Group, Dept of Chemistry, UC Berkeley Nanotube memory device: Lieber Group, Dept of Chemistry, Harvard University SOI transistor/Cu wiring/PowerPC Microprocessor chip: IBM 半导体纳米粒子 (硒化镉) 5 纳米

14 More is different! 层出不穷的新奇量子现象 能量 10-6 10-4 10-2 100 102 104 温度(K)
原子BEC 重费米子超导 激子BEC 高温超导 半导体 3He超流 量子霍耳效应 庞磁阻 金属

15 Role of theory in this field
To develop useful models for experimental systems To reveal mechanisms for observed phenomena To develop accurate methods to predict properties To establish a systematic world view of condensed matter (and the universe)

16 Two Milestones of the 1st Half 20th Century
Crystal Dynamics 1848: 空间点阵学说(Bravais) 1889: 空间群理论(Federov 和 Schvenflies) 1907: 独立振子的量子理论(Einstein) 1912: 连续介质中的弹性波的量子理论(Debye) Band Theory 1900: 金属电导和热传导的经典自由电子理论(Drude) 1924: 基于Fermi统计的自由电子理论(Pauli 和 Sommerfield) 1907: 铁磁性相变的分子场理论(Weiss) 金属导电的能带理论(Bloch)

17 Standard Picture of Metel and Insulator
EF Metals Insulators and Semiconductors First semiconductor transistor

18 Main Stream of Modern Condensed Matter Theory
Understanding of collective motions of electrons Main Actors: electrons (charge + spin) Key Concept: Symmetry breaking Achievements Landau Fermi Liquid Theory Landau Theory of Continuous Phase Transition BCS Theory of Superconductivity Anderson Theory of Localization Theory of Quantum Hall Effects ……

19 Main Stream of Modern Condensed Matter Theory
Driving force: Challenging problems raised in emergent quantum phenomena Theoretical frameworks Single-electron approximation: Band theory, Landau Fermi Liquid Correlated electrons: Unified theory is still absent Development of theoretical methods Analytical: path integral, Green’s function, mean-field theory … Numerical: density functional, Monte Carlo, DMRG, DMFT …

20 Challenging Problems 能量 10-6 10-4 10-2 100 102 104 温度(K)
Superconductivity: cuprates, heavy fermions, … Quantum Hall Effects: integer, fractional, graphene, … Superfluid and supersolid: 4He, 3He Bose-Einstein condensation: excitons, cold atoms (Anti)-ferromagnetism and Mott transition Kondo effects Anderson localization Quantum criticality …… More to come

21 T = 273K 100°C 水沸腾成蒸汽 0°C 水冻结成冰 为什么1023个水分子，单个水分子结构不变、相互作用不变，会“集体地” 、“不约而同地”从一个相“变”到另一个相？

22 经典粒子的合作行为: 统计力学描述 Complex assemblies of atoms and molecules require a STATISTICAL description 分子间的作用力为范德瓦耳斯力 1873 范德瓦耳斯

23 全同粒子的关联现象：量子统计 Satyan N. Bose Albert Einstein Enrico Fermi Paul A.M. Dirac 玻色统计： 每个状态可容纳任意多个粒子 费米统计： 每个状态最多可容纳一个粒子

24 Fermi Statistics：Foundation of Chemistry
Bosons have no Chemical Bonds Fermions can form Chemical Bonds “With a heavy heart, I have been converted to the idea that Fermi-Dirac, not Einstein-Bose is the correct statistics” (for electrons) Pauli, letter to Schrodinger, Dec 1926

25 T ~ 101 K Superconductivity
1911 Onnes discovered the phenomenon of superconductivity 1957 BCS established the microscopic theory of superconductivity H. Kamerlingh Onnes John Bardeen Leon N. Cooper J. Robert Schrieffer (1913) (1972)

26 Meissiner Effect：Anderson-Higgs Mechanism
规范场（磁场）与自发破缺的Goldstone粒子耦合，可以获得质量(能隙)，导致磁场在表面的快速衰减 伦敦方程

27 Landau-Ginzberg Theory and Quantized Magnetic Flux Vortices
Alexei A Abrikosov 2003 Nobel Prize Vortices of NbSe2

28 T ~ 102 K ：High-Tc superconductors
Bednorz & Muller 1986 One of the most challenging problems left last century 朱经武 赵忠贤 UBC Hg2Ba2Ca2Cu3Ox YBa2Cu3O7 fake La2-xBaxCuO4 Hg

29 赝能隙：高温超导反常现象之根源 kb 费米面不封闭，存在能隙 ka 低能熵缺失，状态数不守恒 赝能隙现象：
正常相中出现的类似于超导能隙的现象 超导电子配对好像在相变之前就存在，但没有形成宏观相干 低能熵缺失，状态数不守恒

30 高温超导体c轴电阻的反常 c (z) a,b (x,y) 平面内电阻随温度降低而降低，典型的金属行为

31 Superfluid T ~ 4 K 1938 Kapitsa discovered the superfluidity of 4He --- first realization of Bose-Einstein Condensation 1940s Landau formulated the theory of 4He superfluidity Pyotr L. Kapitsa (1978) Lev Landau 1941 (1962)

32 Fermion Superfluid T ~ 10-3 K
Early 1970s 3He superfluidity was discovered 1996, 2003 Nobel prizes 自旋－轨道自发对称破缺 David M. Lee Douglas D. Osheroff Robert C.Richardson Anthony Leggett

33 Supersolid: intrinsic? Unsolved issue
Moses H W Chan 2004 Penn State Univ

34 Integer Quantum Hall Effect
Quantum Hall Effect: novel Quantum state Integer Quantum Hall Effect 1985 Nobel Prize

35 Daniel C. Tsui Horst L. Störmer Robert Laughlin 1998 Nobel Prize
Fractional Quantum Hall Effect T ~ 10-2 K Laughlin wave-function Fractional charge and fractional statistics Abelian and non-Abelian Daniel C. Tsui Horst L. Störmer Robert Laughlin Nobel Prize

36 Microwave induced “zero-resistance state” --- a novel non-equilibrium transport state
RG Mani, JH Smet, K von Klitzing, et al., Nature 420, 646 (2002); MA Zudov, RR Du, et al., PRL 90, (2003).

37 Kondo Effect: key for understanding many correlated effects
Kondo resonance 磁性杂质与金属电子相互作用在费米面上产生一个杂质共振态

38 Kondo peak is observed, but it is not-symmetric!
Experimental observation of Kondo Effect Au(111) Co No features Fano resonance tip Kondo peak is observed, but it is not-symmetric! V. Madhavan et al., Science 280, 567 (1998)

39 Fano Resonance U. Fano 1961 non-symmetric resonance led by the interference between a discrete level and a continuum Absorption spectrum Discrete channel Continuum channel q: asymmetry factor

40 Two Kinds of Interference Channels
HG Luo, T Xiang, XQ Wang, ZB Su, L Yu, PRL 92 (2004) Kondo共振态与导电电子的干涉 Kondo共振态与展宽的杂质能级的自干涉

41 Comparison with Experimental Data

42 Bose-Einstein Condensation of diluted cold atoms
A technical breakthrough, stimulate the unification of quantum optics and condensed matter physics 2001 Nobel Prize

43 T = 0K ：Quantum Phase Transition
Quantum-critical g gc 基态性质作为控制参数g的函数有奇异性，临界点是物质的新态，没有元激发！ 强关联量子系统不同基态（呈展态）间的竟争 临界涨落控制整个量子临界区的动力学行为

44 Quantum Criticality in High-Tc Cuprates
Is the non-Fermi liquid behavior discovered in high-Tc a quantum critical phenomenon? d-wave superconducting AF

45 Mott Transition Standard Model:
Odd number of electrons: metal Even number of electrons: insulator But many materials (eg La2CuO4) that are expected to be metals are actually insulators Is the Mott transition really intrinsic, not a result of the ordering of other parameters (eg AFM)? What is the equation describing the Mott Transition? Is there any order parameter?

46 Optical Lattice Mott绝缘态： t << U 库仑排斥U大于粒子的动能 t 超流凝聚态：t >>U
Tools of Quantum Optics Problems of Condensed Matter

47 T ~ 10-6 K Accurately controlled Quantum Phase Transition
--- Superfluid-Insulator Transition

48 New concepts and new methods are desired!
Why Challenging Emergent quantum phenomena are mainly caused by the collective motions of electrons, correlations among electrons are important In nearly 99% case, we can only solve rigorously a problem of Harmonic Oscillators Perturbation is the only tool we have to attack a many-body problem. But the correlated effect is non-perturbative! New concepts and new methods are desired!

49 How to face the challenge
Capture key physics from experimental observations: physical intuition Theoretical modeling: power of theoretical analysis “First principle” calculations: determine basic parameters

50 Theoretical Methods Analytical: perturbation from a right starting point Green’s Functions (Shao-Jing Qin) Path Integral and Mean Field Theory (Yue Yu) Equations of Motion (truncation approach) Numerical: object oriented Density Functional Theory (single-particle) Quantum Monte Carlo (minus sign problem) Density Matrix Renormalization Group Dynamical Mean-Field Theory ( D)

51 Density Functional Theory
First principle: no input parameters Basis of materials design Good only for weakly coupled systems: in real calculations, LDA or other approximations has to be taken Correlated effects cannot be correctly and fully treated 指数墙问题幽灵不散！ 面对纷繁呈展的世界，物理学家始终在做着还原的梦: 从最基本的量子力学原理和电子间的库仑相互作用出发，计算和分析各种呈展量子现象 Walter Kohn

52 fermions P(x) can be negative
Quantum Monte Carlo Random sampling (integration) Detailed balance P(x)r(x  x’) = P(x’)r(x’  x) Metropolis algorithm: If P(x’) > P(x) accept move If P(x’) < P(x) accept with probability r(x  x’) = P(x’) / P(x) Minus Sign Problem: fermions P(x) can be negative

53 克服指数墙的约束：密度矩阵重正化群 数值重正化群的基本出发点：
Kenneth K. Wilson 1982 Nobel 物理奖 数值重正化群的基本出发点： 在研究低能物理性质时，高能量状态的贡献很小，因此我们可以用有限个基矢来近似表达一个无限大自由度(或Hilbert空间)的状态 重正化群与标度不变性 数值重正化群 核心问题： 如何判别哪个基矢重要，哪个不重要

54 密度矩阵重正化群（DMRG） 系统 如何确定每个自由度对目标状态贡献的大小？ 子系统 子系统 物理实验：外加一个扰动，测系统的反应
物理实验：外加一个扰动，测系统的反应　 　　　　　例如：加电流，测电压，确定电阻　R = V / I DMRG实验: 无外界扰动，用系统的一部分作为探针（约化密度矩阵）去探测另一部分所处的状态

55 密度矩阵重正化群（DMRG） 研究一维多体量子体系最精确的方法 能精确计算各种基态、热力学和动力学量 1D S=1 Heisenberg模型
基态能量 能隙 粒子数 量子蒙特卡罗 (5) 严格对角化 (2) (2) DMRG (4) (2)  近年来的新进展：多体含时Schordinger方程的求解 有望突破的方向：高维量子系统和量子化学计算，与量子 Monte Carlo方法的结合

56 Dynamical Mean Field Theory
Reduce the quantum many body problem to a one site or a cluster of sites, in a medium of non interacting electrons obeying a self consistency condition. Instead of using functionals of the density, use more sensitive functionals of the one electron spectral function. Perspective: Combine with LDA

57 Dynamical Mean Field Theory
Freeze the spatial fluctuation, consider only the local quantum fluctuation Map a lattice model onto a quantum impurity model of electrons in a medium of non-interacting electrons obeying a self consistency condition Instead of using functionals of the density, use more sensitive functionals of the one electron spectral function. Perspective: Combine with LDA

58 Dynamical Mean Field Theory
Hubbard model Single-site action Self-consistent equation