How might a Fermi surface die?

Slides:



Advertisements
Similar presentations
Anderson localization: from single particle to many body problems.
Advertisements

Trapped ultracold atoms: Bosons Bose-Einstein condensation of a dilute bosonic gas Probe of superfluidity: vortices.
Inhomogeneous Superconductivity in the Heavy Fermion CeRhIn 5 Tuson Park Department of Physics, Sungkyunkwan University, Suwon , South Korea IOP.
Iron pnictides: correlated multiorbital systems Belén Valenzuela Instituto de Ciencia de Materiales de Madrid (ICMM-CSIC) ATOMS 2014, Bariloche Maria José.
Theory of the pairbreaking superconductor-metal transition in nanowires Talk online: sachdev.physics.harvard.edu Talk online: sachdev.physics.harvard.edu.
Quantum Critical Behavior of Disordered Itinerant Ferromagnets D. Belitz – University of Oregon, USA T.R. Kirkpatrick – University of Maryland, USA M.T.
High T c Superconductors & QED 3 theory of the cuprates Tami Pereg-Barnea
D-wave superconductivity induced by short-range antiferromagnetic correlations in the Kondo lattice systems Guang-Ming Zhang Dept. of Physics, Tsinghua.
Subir Sachdev arXiv: Subir Sachdev arXiv: Loss of Neel order in insulators and superconductors Ribhu Kaul Max Metlitski Cenke Xu.
Domain walls at the SDW endpoint of (TMTSF) 2 PF 6 under pressure C.Pasquier, Laboratoire de Physique des Solides, Orsay S. Brazovskii LPTMS, Orsay Acknowledgments:
Quantum Criticality. Condensed Matter Physics (Lee) Complexity causes new physics Range for CMP.
Strongly Correlated Electron Systems a Dynamical Mean Field Perspective:Points for Discussion G. Kotliar Physics Department and Center for Materials Theory.
Quasiparticle anomalies near ferromagnetic instability A. A. Katanin A. P. Kampf V. Yu. Irkhin Stuttgart-Augsburg-Ekaterinburg 2004.
Universality in ultra-cold fermionic atom gases. with S. Diehl, H.Gies, J.Pawlowski S. Diehl, H.Gies, J.Pawlowski.
A new scenario for the metal- Mott insulator transition in 2D Why 2D is so special ? S. Sorella Coll. F. Becca, M. Capello, S. Yunoki Sherbrook 8 July.
THE STATE UNIVERSITY OF NEW JERSEY RUTGERS Studies of Antiferromagnetic Spin Fluctuations in Heavy Fermion Systems. G. Kotliar Rutgers University. Collaborators:
Mott –Hubbard Transition & Thermodynamic Properties in Nanoscale Clusters. Armen Kocharian (California State University, Northridge, CA) Gayanath Fernando.
Magnetic quantum criticality Transparencies online at Subir Sachdev.
A1- What is the pairing mechanism leading to / responsible for high T c superconductivity ? A2- What is the pairing mechanism in the cuprates ? What would.
From Kondo and Spin Glasses to Heavy Fermions, Hidden Order and Quantum Phase Transitions A Series of Ten Lectures at XVI Training Course on Strongly Correlated.
Heavy Fermions Student: Leland Harriger Professor: Elbio Dagotto Class: Solid State II, UTK Date: April 23, 2009.
Fluctuation conductivity of thin films and nanowires near a parallel-
Lecture schedule October 3 – 7, 2011  #1 Kondo effect  #2 Spin glasses  #3 Giant magnetoresistance  #4 Magnetoelectrics and multiferroics  #5 High.
Huiqiu Yuan Department of Physics, Zhejiang University, CHINA Field-induced Fermi surface reconstruction near the magnetic quantum critical point in CeRhIn.
B. Valenzuela Instituto de Ciencia de Materiales de Madrid (ICMM-CSIC)
Fermionic quantum criticality and the fractal nodal surface Jan Zaanen & Frank Krüger.
Dung-Hai Lee U.C. Berkeley Quantum state that never condenses Condense = develop some kind of order.
Switching of Magnetic Ordering in CeRhIn 5 under Hydrostatic Pressure Kitaoka Laboratory Kazuhiro Nishimoto N. Aso et al., Phys. Rev. B 78, (2009).
Introduction to even-denominator FQHE: composite fermions Tejas Deshpande Journal club: 11 November, 2014.
2013 Hangzhou Workshop on Quantum Matter, April 22, 2013
会社名など E. Bauer et al, Phys. Rev. Lett (2004) M. Yogi et al. Phys. Rev. Lett. 93, (2004) Kitaoka Laboratory Takuya Fujii Unconventional.
Self-generated instability of a ferromagnetic quantum-critical point
Zheng-Yu Weng IAS, Tsinghua University
Wigner-Mott scaling of transport near the two-dimensional metal-insulator transition Milos Radonjic, D. Tanaskovic, V. Dobrosavljevic, K. Haule, G. Kotliar.
Superconductivity and non-Fermi-liquid behavior of Ce 2 PdIn 8 V. H. Tran et al., PHYSICAL REVIEW B 83, (2011) Kitaoka Lab. M1 Ryuji Michizoe.
Non-Fermi Liquid Behavior in Weak Itinerant Ferromagnet MnSi Nirmal Ghimire April 20, 2010 In Class Presentation Solid State Physics II Instructor: Elbio.
Raman Scattering As a Probe of Unconventional Electron Dynamics in the Cuprates Raman Scattering As a Probe of Unconventional Electron Dynamics in the.
Kondo Physics, Heavy Fermion Materials and Kondo Insulators
Optical lattice emulator Strongly correlated systems: from electronic materials to ultracold atoms.
Qimiao Si Rice University KIAS, Oct 29, 2005 Heavy fermion metals: Global phase diagram, local quantum criticality, and experiments.
Mott Transition and Superconductivity in Two-dimensional
Quantum Criticality in Magnetic Single-Electron Transistors T p Physics of non-Fermi-liquid Metals Qimiao Si, Rice University, DMR Quantum criticality.
Lecture schedule October 3 – 7, 2011
Superconductivity and magnetism in iron-based superconductor
The quest to discover the self-organizing principles that govern collective behavior in matter is a new frontier, A New Frontier ELEMENTS BINARYTERTIARY.
Low-temperature properties of the t 2g 1 Mott insulators of the t 2g 1 Mott insulators Interatomic exchange-coupling constants by 2nd-order perturbation.
Deconfined quantum criticality T. Senthil (MIT) P. Ghaemi,P. Nikolic, M. Levin (MIT) M. Hermele (UCSB) O. Motrunich (KITP), A. Vishwanath (MIT) L. Balents,
Chapter 7 in the textbook Introduction and Survey Current density:
Lattice gauge theory treatment of Dirac semimetals at strong coupling Yasufumi Araki 1,2 1 Institute for Materials Research, Tohoku Univ. 2 Frontier Research.
 = -1 Perfect diamagnetism (Shielding of magnetic field) (Meissner effect) Dynamic variational principle and the phase diagram of high-temperature superconductors.
Qimiao Si Rice University
DISORDER AND INTERACTION: GROUND STATE PROPERTIES of the DISORDERED HUBBARD MODEL In collaboration with : Prof. Michele Fabrizio and Dr. Federico Becca.
Review on quantum criticality in metals and beyond
Some open questions from this conference/workshop
Ginzburg Landau phenomenological Theory
Phase diagram of FeSe by nematic ultrafast dynamics
Spin-Orbit Coupling Effects in Bilayer and Optical Lattice Systems
Toward a Holographic Model of d-wave Superconductors
Essential of Ultra Strong Magnetic field and Activity For Magnetars
Condensed Matter Physics and Materials Science: David M
Nathan Finney Michael Gammon Newell Jensen
Search of a Quantum Critical Point in High Tc Superconductors
Interplay between disorder and interactions
Quantum phase transitions and the Luttinger theorem.
Killing the Fermi surface: Some ideas on the strange metal, Fermi arcs and other phenomena T. Senthil (MIT) TS, ``Critical fermi surfaces and non-fermi.
On the cosmic scale: Stars density  Interstellar Space  temperature
Spectroscopy of ultracold bosons by periodic lattice modulations
Quantum phase transitions out of the heavy Fermi liquid
Chengfu Mu, Peking University
Phases of Mott-Hubbard Bilayers Ref: Ribeiro et al, cond-mat/
Presentation transcript:

How might a Fermi surface die? T. Senthil

Electrons in metals

Modern solid state physics

A common phase diagram Non Fermi Liquid T Phase A Phase B Tuning parameter

Example 1: High temperature superconducting materials Pseudo gap AF Mott insulator Non-fermi liquid metal Fermi liquid

Example 2: Magnetic ordering in certain rare earth alloys CePd2Si2, CeCu6-xAux, YbRh2Si2,…… Metal Non –fermi liquid

Representative data on YbRh2Si2 Custers et al, Nature, 2003 Trovarelli et al, PRL 2000 B(T) T-dependence of resistivity at critical point: ρ(T) ~ T for three decades in temperature! Fermi liquid Magnetic metal Non fermi liquid

Origin of non-fermi liquid physics? T Tuning parameter Phase A Phase B Non Fermi Liquid

So possibly……….

Recent clue from experiments

Killing a Fermi surface

Geometry of Fermi surface of CeRhIn5 Example: Evolution of Fermi surface across the magnetic phase transition in CeRhIn5 H. Shishido, R. Settai, H. Harima, & Y. Onuki, JPSJ 74, 1103 (2005)

A simple theoretical example

Evolution from metal to insulator

Possible experimental realization of a second order Mott transition

Another example: High temperature superconducting materials Pseudo gap AF Mott insulator Non-fermi liquid metal Fermi liquid

Basic question for theory How can an entire Fermi surface disappear continuously?

Even more basic: What is the Fermi surface?

How might the Fermi surface die?

Electronic structure at criticality: ``Critical Fermi surface”

Why a critical Fermi surface?

Evolution of single particle gap

Why a critical Fermi surface? Evolution of momentum distribution

Killing a Fermi surface

Some obvious consequences/questions

Scaling phenomenology at a quantum critical point with a critical Fermi surface?

Critical Fermi surface: scaling for single particle physics

New possibility: angle dependent exponents

Leaving the critical point

Implications of angle dependent exponents

Finite T crossovers

Summary A Fermi surface may die through a second order phase transition -at the critical point the Landau quasiparticle is destroyed but the Fermi surface is preserved ( the `critical Fermi surface’) => non-fermi liquid Presence of critical fermi surface will change the scaling phenomenology associated with universal critical singularities. Concrete model calculations with a critical Fermi surface exist Future – many challenges Tests of scaling in experiments Calculational framework?