Bosonizing one-dimensional cold atomic gases
By M. Cazalilla. 2003
312 citations recorded by the source corpus.
We present results for the long-distance asymptotics of correlation functions of mesoscopic one-dimensional systems with periodic and open (Dirichlet) boundary conditions, as well as at finite temperature in the thermodynamic limit. The results are obtained using Haldane's harmonic-fluid approach (also known as 'bosonization'), and are valid for both bosons and fermions, in weakly and strongly interacting regimes. The harmonic-fluid approach and the method of computing the correlation functions using conformal transformations are explained in great detail. As an application relevant to one-dimensional systems of cold atomic gases, we consider the model of bosons interacting with a zero-range potential. The Luttinger-liquid parameters are obtained from the exact solution by solving the Bethe-ansatz equations in finite-size systems. The range of applicability of the approach is discussed, and the prefactor of the one-body density matrix of bosons is fixed by finding an appropriate parametrization of the weak-coupling result. The formula thus obtained is shown to be accurate, when compared with recent diffusion Monte Carlo calculations, within less than 10%. The experimental implications of these results for Bragg scattering experiments at low and high momenta are also discussed.
Subfields: Atomic and Molecular Physics, and Optics, Condensed Matter Physics
View Paper: https://www.semanticscholar.org/paper/485f6907c1af062b36aedf381486e70bad8a9e73
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In Atomic and Molecular Physics, and Optics
In Condensed Matter Physics
Citations in the corpus
- Probing quantum and thermal noise in an interacting many-body system (2007, methodology): “The effective approach to the Lieb-Liniger model, capturing the long-distance behavior of all correlation functions is known as the Luttinger liquid formalism [35, 36, 37].”
- One dimensional bosons: From condensed matter systems to ultracold gases (2011, methodology): “In addition, on the lattice it is also possible to show (see e.g. the appendix in Cazalilla (2004a)) the equivalence of the Jordan-Wigner approximation and Girardeau’s Bose-Fermi mapping, which applies to the many-body wavefunctions of both models and is reviewed in Sec.”
- Phase space representation of quantum dynamics (2009, background): “(Cazalilla, 2004; De Grandi et al., 2008), where large K corresponds to weak interactions 41 spectrum of the SG model is quite rich.”
- Tonks–Girardeau gas of ultracold atoms in an optical lattice (2004, background): “At finite temperatures a new momentum scale sets i”
- Many-Body Physics with Ultracold Gases (2007, methodology): “Indeed, the Bose-Hubbard model in one dimension at n 1 describes a Luttinger liquid with K = 1 + 4πn/γL + . . ., where γL = U/J is the effective coupling parameter on a lattice (Cazalilla, 2004).”
- One-dimensional quantum liquids: Beyond the Luttinger liquid paradigm (2011, background): “For example, for spinless fermions at ρ|x±vt| 1, one has (Cazalilla, 2004)〈 Ψ†(0, 0)Ψ(x, t) 〉 LL ∼ (136)∑ n ρei(2n+1)kF x 2i(−1)n Cn (iρ(vt+ x) + 0) µL (iρ(vt− x) + 0)µR , where Cn are “nonuniversal” prefactors, and µR(L) = (2n+ 1) 2K/4± (2n+ 1)/2 + 1/4K ≥ 0.”