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Non-Fermi Liquid (NFL) phases of 2d itinerant electrons

Non-Fermi Liquid (NFL) phases of 2d itinerant electrons. Symposium on Theoretical and Mathematical Physics, Euler Institute, St. Petersburg, July 11, 2011. MPA Fisher with Hongchen Jiang, Matt Block, Ryan Mishmash, Donna Sheng, Lesik Motrunich (in progress).

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Non-Fermi Liquid (NFL) phases of 2d itinerant electrons

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  1. Non-Fermi Liquid (NFL) phases of 2d itinerant electrons Symposium on Theoretical and Mathematical Physics, Euler Institute, St. Petersburg, July 11, 2011 MPA Fisher with Hongchen Jiang, Matt Block, Ryan Mishmash, Donna Sheng, Lesik Motrunich (in progress) Goal: Construct and Analyze non-Fermi liquid phases of strongly interacting 2d itinerant electrons • “Parton” construction for NFL (Gutzwiller wf’s) • Ex of a NFL: “D-wave Metal” • Hamiltonian and energetics (DMRG) for “D-wave Metal”?

  2. What is a “Non-Fermi-liquid metal”? First: What is a Fermi Liquid Metal

  3. 2D Free Fermi Gas Momentum Distribution Function: Volume of Fermi sea set by particle density 1 k kF 2D Fermi Liquid Metal Luttingers Thm: Volume inside Fermi surface still set by total density of fermions 1 ky Z < 1 kx k kF

  4. 2D Non-Fermi Liquid Metal • Various possibilities: • A singular “Fermi surface” that satisfies Luttinger’s theorem but without a jump discontinuity in momentum distribution function 2) A singular Fermi surface that violates Luttinger’s theorem (eg. volume “x” rather than “1-x”) 3) A singular “Fermi surface” with ``arc” kF k 4.) Other….

  5. Wavefunction(s) for NFL metals?

  6. Wavefunction for 2D Free Fermi gas Free Fermion determinant: (eg with 2D circular Fermi surface) ky kx Real space “nodal structure” Define a ``relative single particle function” Nodal lines: Ultraviolet and infrared “locking”

  7. Wavefunction for interacting Fermi liquid? Retain sign (nodal) structure of free fermions, modify amplitude, eg to keep particles apart. Common form: Multiply free fermion wf by a Jastrow factor, with u(r) a variational function For Spinful Electrons: Gutzwiller Projection Slater determinant Project out doubly occupied sites

  8. Parton approach to NFL wavefunctions Decompose electron: spinless charge e boson, s=1/2 neutral fermionic spinon Mean Field Theory Treat “Spinons” and Bosons as Independent: Wavefunctions (enlarged Hilbert space - twice as many particles) “Fix-up” Mean Field Theory “Glue” together Fermion and Boson “partons” Project back into physical Hilbert space

  9. Fermi and Non-Fermi Liquids via partons? Spinons in a filled Fermi sea Fermi Liquid: Bosons into Bose condensate Non-Fermi Liquid: Bosons into uncondensed fluid - a “Bose metal” NFL Metal: Product of Fermi sea and uncondensed “Bose-Metal”

  10. But what is a “Bose-Metal”? First - A conventional interacting superfluid: Boson Green’s function Off-diagonal long-ranged order nk Momentum distribution function Z<1 k

  11. 2D Bose-Metal • A stable T=0 liquid phase of bosons that is not a superfluid • Real space Green’s function has oscillatory power law decay (not a Bose condensate) • Singularities in momentum distribution function • Singular momentum on a “Bose surface” ky k kB kx Angular dependent anomalous dimension

  12. Parton Construction for a Bose-metal: (all Fermionic decomposition of the electron) Gutzwiller wavefunction: Wf for D-wave Bose-Metal (DBM) DBM: Product of 2 Fermi sea determinants, elongated in the x or y directions - + + - Dxy relative 2-particle correlations

  13. Bose Surfaces in D-wave Bose-Metal Mean Field Green’s functions factorize: Momentum distribution function: Two singular lines in momentum space, Bose surfaces:

  14. “D-Wave Metal” Itinerant NFL phase of 2d electrons? All fermionic Parton construction Wavefunction; Product of determinants Filled Fermi sea Can use Variational Monte Carlo to extract equal time correlation functions from wf But what about energetics???

  15. Hamiltonians with Bose-metalor NFL metal ground states??

  16. First: Hamiltonian for D-wave Bose-Metal? (Strong coupling limit of parton gauge theory) “Ring exchange” Phase diagram: K/J and density of bosons ?? 0 K/J (K/J)c Superfluid DBM ?? J-K Model has a sign problem - completely intractable

  17. Ladders to the Rescue Transverse y-components of momentum become quantized Put Bose superfluid on n-leg ladder Put D-wave Bose metal on n-leg ladder ky ky kx kx Many gapless 1d modes, one for each “Bose” point Single gapless 1d mode Signature of 2d Bose surface present on ladders Expectation: Signature of Bose surface in Bose-Metal on n-leg ladders

  18. Boson ring model on the 2-Leg Ladder • Exact Diag. • Variational Monte Carlo • DMRG E. Gull, D. Sheng, S. Trebst, O. Motrunich and MPAF, PRB 78, 54520 (2008) K • Correlation Functions: • Momentum Distribution function • Density-density structure factor Ladder descendant of 2D Bose-metal??

  19. Phase Diagram for 2-leg ladder Phases: Superfluid – “Bose condensate” D-Wave Bose Metal - DBL s-wave Pair-Boson “condensate” D-wave Bose-Metal occupies large region of phase diagram

  20. Superfluid versus D-wave Bose-Metal D-wave Bose-Metal; Singular “Bose points” at Superfluid - “condensed” at zero momentum

  21. Variational Wf for D-wave Bose-metal on 2-leg ladder In DBM: Bonding/Antibonding occupied For d1 Fermion Just Bonding occupied For d2 Fermion Variational parameter: Fermi wavevectors in d1 bands

  22. DBM: How good is ladder variational wavefunction? Gauge mean field theory predicts singularities in momentum distribution function at: Both DMRG and det1 x det2 Wavefunction show singular cusps only at (Ampere’s law) d2 d1

  23. Hamiltonian for D-wave Metal? Strong coupling limit of parton gauge theory t-K “Ring” Hamiltonian(no double occupancy constraint) 2 2 1 1 Electron singlet pair “rotation” term 4 3 4 3

  24. Phase diagram of electron t-K Hamiltonian? (Density and K/t) Severe sign problem - intractable Once again: Analyze t-K electron ring Hamiltonian on 2-leg ladder

  25. Possible to identify a NFL on a 2-leg ladder? Interacting Fermions in 1d: A Luttinger liquid Luttinger liquid exponent: Momentum distribution function has (dominant) singularity at k=kF satisfying Luttinger sum rule kF k Interacting Fermions on 2-leg ladder: 2-bands Luttinger “volume” sum rule still satisfied: kx kx Searching for a “non-Luttinger liquid” (ie. a Luttinger-liquid violating Luttinger’s sum rule)

  26. Electron t-K model on 2-leg ladder Two dimensionless parameters: K/t and density n (n=1/3 henceforth) No double occupancy Hongchen Jiang, Matt Block, Ryan Mishmash, Donna Sheng, Lesik Motrunich and MPAF (in progress) ED DMRG VMC Bosonization of Quasi-1d U(1) gauge theory

  27. Ground State energy: DMRG

  28. K/t <0.7 Luttinger Liquid Satisfies Luttinger’s Theorem: the volume enclosed by the “Fermi surface” yields the particle density. (16 particles, singlet, 8 up and 8 down) A canonical (single band) Luttinger liquid

  29. 0.7< K/t <1.25 : Spin Polarized Non-interacting spin polarized Fermi sea is exact ground state here. Luttinger theorem satisfied

  30. K/t>1.25: Non-LL Phase

  31. K/t > 1.25: Non-LL Phase Non-monotonic momentum distribution function; No sign of Luttingers volume

  32. Non-Luttinger-Liquid phase for K>1.25? Electron momentum distribution function: Singular features, but at momenta which do not satisfy Luttinger’s volume theorem Can we understand in terms of D-wave Metal on 2-leg ladder?? Employ parton construction, gauge theory and VMC

  33. The d-wave Metal on 2 Legs Gauge theory: Projects down to physical Hilbert space Number of 1d modes = (number in MFT) – (gauge constraints) = (2+1+2)-(2) = 3 Central charge c=3, strongly entangled

  34. Electron momentum distribution function Mean Field Theory: electron momentum distribution, convolution of partons Gauge theory - certain wavevectors enhanced Illustrate with Boson ring model (MFT) Very sharp peaks in the exact boson momentum distribution function! (from DMRG)

  35. Momentum distribution function in the d-wave metal? ? (Free spinon sea)

  36. Convolution: c = b f 1 0 0 0 0

  37. K/t>1.25: Non-LL Phase

  38. Density-density structure factor: DMRG

  39. The d-wave Metal on 2 Legs In , enhanced singularities are predicted by the gauge theory at various wavevectors.

  40. Evolution of Peak Locations

  41. Evolution of Peak Locations

  42. DMRG Phase diagram varying transverse electron hopping, tperp

  43. Variational Monte Carlo (VMC) D-wave Metal: Product of Slater determinants Variational Parameters: Distribution of dx partons between bonding/anti-bonding bands (f-spinons and dy partons only in bonding band) 2 parameters to tune the Luttinger exponents (Luttinger liquid phase: Jastrow factor multiplying filled Fermi sea)

  44. Ground State energy: DMRG vs VMC

  45. Evolution of VMC States

  46. Evolution of VMC States

  47. Evolution of VMC States

  48. Evolution of VMC States

  49. Evolution of VMC States

  50. Evolution of VMC States

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