Fluctuations of squeezing fields beyond the Tomonaga--Luttinger liquid paradigm

TL;DR

This paper introduces a squeezed-field path-integral approach to analyze one-dimensional quantum systems beyond the traditional Tomonaga--Luttinger liquid model, revealing new fluctuation effects and side-band excitations.

Contribution

It develops a nonlinear Lagrangian framework incorporating squeezing field fluctuations, extending the TLL paradigm to include interaction-induced corrections and additional excitation branches.

Findings

Emergence of a side-band branch due to squeezing field fluctuations

Renormalization of phase velocities and spectral weights by squeezing modes

Temperature-dependent nonlinear dispersion relations

Abstract

The concept of Tomonaga--Luttinger liquids (TLL) on the basis of the free-boson models is ubiquitous in theoretical descriptions of low-energy properties in one-dimensional quantum systems. In this work, we develop a squeezed-field path-integral description for gapless one-dimensional systems beyond the free-boson picture of the TLL paradigm. In the squeezed-field description, the parameter of the Bogoliubov transformation for the TL Hamiltonian becomes a dynamical squeezing field, and its fluctuations give rise to corrections to the free-boson results. We derive an effective nonlinear Lagrangian describing the dispersion relation of the squeezing field, and interactions between the excitations of the TLL and the squeezing modes. Using the effective Lagrangian, we analyze the imaginary-time correlation function of a vertex operator in the non-interacting limit. We show that a side-band branch emerges due to the fluctuation of the squeezing field, in addition to the standard branch of the free-boson model of the TLL paradigm. Furthermore, we perturbatively analyze the spectral function of the density fluctuations for an ultracold Bose gas in one dimension. We evaluate the renormalized values of the phase velocities and spectral weights of the TLL and side-band branches due to the interaction between the TLL and the squeezing modes. At zero temperature, the renormalized dispersion relations are linear in the momentum, but at nonzero temperatures, these acquire a nonlinear dependence on the momentum due to the thermal population of the excitation branches.