# From the moving piston to the dynamical Casimir effect: explorations with shaken condensates

## TL;DR

This paper explores how ultracold atom systems with moving boundaries can simulate the dynamical Casimir effect, revealing new quantum phenomena like vacuum squeezing and multimode entanglement through theoretical models.

## Contribution

It introduces a theoretical framework for studying dynamical Casimir effects in ultracold atom setups using the Luttinger liquid model, highlighting novel quantum effects.

## Key findings

- Demonstrated phase dynamics analysis using Moore's formalism.
- Identified classical excitation and nonlinear mode generation.
- Found strong parametric multimode squeezing.

## Abstract

Recent experimental realizations of uniform confining potentials for ultracold atoms make it possible to create quantum acoustic resonators and explore nonequilibrium dynamics of quantum field theories. These systems offer a promising new platform for studying the dynamical Casimir effect, since they allow to achieve relativistic, i.e. near sonic, velocities of the boundaries. In comparison to previously studied optical and classical hydrodynamic systems ultracold atoms allow to realize a broader class of dynamical experiments combining both classical driving and vacuum squeezing. In this paper we discuss theoretically two types of experiments with interacting one dimensional condensates with moving boundaries. Our analysis is based on the Luttinger liquid model which utilizes the emergent conformal symmetry of the low energy sector of the Lieb-Liniger model. The first system we consider is a variable length interferometer with two Y-junctions connected back to back. We demonstrate that dynamics of the relative phase between the two arms of the interferometer can be analyzed using the formalism developed by Moore in the problem of electromagnetic vacuum squeezing in a cavity with moving mirrors. The second system we discuss is a single condensate in a box potential with periodically moving walls. This system exhibits classical excitation of the mode resonant with the drive as well as nonlinear generation of off-resonant modes. In addition we find strong parametric multimode squeezing between modes whose energy difference matches integer multiples of the drive frequency.