Download presentation
Published byStephanie Freeman Modified over 8 years ago
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
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
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.