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Fermi-Luttinger Liquid Michael Pustilnik, Georgia Tech

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1 Fermi-Luttinger Liquid Michael Pustilnik, Georgia Tech
Alex Kamenev in collaboration with Leonid Glazman, U of M Maxim Khodas, U of M Michael Pustilnik, Georgia Tech PRL 96, (2006); arXiv:cond-mat/ arXiv:cond-mat/ RPMBT14, Jul., 2007

2 One-dimensional … M. Chang, et al 1996 Dekker et al 1997
Bockrath, et al 1997 Auslaender et al 2004 I. Bloch 2004

3 Spectral Function

4 d>1: Fermi Liquid Energy relaxation rate: The same for holes
Spectral density: Energy relaxation rate: interaction potential The same for holes

5 d=1 Spectral density: ? ? Energy relaxation rate:

6 Luttinger model Energy relaxation rate: Spectral density:
Dzaloshinskii, Larkin 1973 Spectral density: Energy relaxation rate:

7 Luttinger model (cont)
Haldane, 1983

8

9 1D with non-linear dispersion: Holes

10 1D with non-linear dispersion: Particles
Energy relaxation rate: interaction potential Does not work for integrable models

11 Particles (cont) Fermi head with the Luttinger tail

12 Spectral Edges Shake up or X-ray singularity (cf. Mahan, Nozieres,…)

13 Structure Factor

14 Luttinger approximation
Linear dispersion Exact result within the Luttinger approximation. How does the dispersion curvature and interactions affect the structure factor ?

15 Spectrum curvature + interactions
Fourier components of the interaction potential V

16 AFM spin chain N 200. For this case we have calculated
form factors S. Nagler, et al 2005

17 1D Bose Liquid Bose-Fermi mapping (1D)
Bosons with the strong repulsion = Fermions with the weak attraction – changes sign. Bose-Fermi mapping (1D) 1D hard-core bosons = free fermions (Tonks-Girardeau) Divergence at the upper edge Caux, Calabrese, 2006 Lieb-Liniger model, 1963 Constant-q scan

18 Structure factor: conclusions
Power law singularities at the spectral edges (Lieb modes) with q-dependent exponents. Bosons Fermions

19 Fermi-Luttinger Liquid
Hole’s mass-shell is described by the Luttinger liquid (with momentum-dependent exponent). Particle’s mass-shell is described by the Fermi liquid (with smaller relaxation rate). Spectral edges of the spectral function and the structure factor exhibit power-law singularities.

20 Summary of bosonic exponents
Boson-Fermion mapping Hydrodynamics ?

21 Numerics (preliminary)
Courtesy of J-S. Caux

22 Numerics (preliminary)
Courtesy of J-S. Caux


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