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As Contributors: | Isabelle Bouchoule |

Arxiv Link: | https://arxiv.org/abs/1806.08759v2 |

Date submitted: | 2018-07-04 |

Submitted by: | Bouchoule, Isabelle |

Submitted to: | SciPost Physics |

Domain(s): | Theoretical |

Subject area: | Quantum Physics |

We present a general analysis of the cooling produced by losses on condensates or quasi-condensates. We study how the occupations of the collective phonon modes evolve in time, assuming that the loss process is slow enough so that each mode adiabatically follows the decrease of the mean density. The theory is valid for any loss process whose rate is proportional to the $j$th power of the density, but otherwise spatially uniform. We cover both homogeneous gases and systems confined in a smooth potential. For a low-dimensional gas, we can take into account the modified equation of state due to the broadening of the cloud width along the tightly confined directions, which occurs for large interactions. We find that at large times, the temperature decreases proportionally to the energy scale $mc^2$, where $m$ is the mass of the particles and $c$ the sound velocity. We compute the asymptotic ratio of these two quantities for different limiting cases: a homogeneous gas in any dimension and a one-dimensional gas in a harmonic trap.

Has been resubmitted

Resubmission 1806.08759v4 (25 October 2018)

Resubmission 1806.08759v3 (18 September 2018)

- Report 2 submitted on 2018-10-22 13:54 by
*Anonymous* - Report 1 submitted on 2018-09-26 09:00 by
*Anonymous*

Submission 1806.08759v2 (4 July 2018)

1- Significant extension and generalization of previous theoretical models, which enables the interpretation of recent experiments studying cooling through losses in cold atomic gases.

2- Comprehensive, timely and relevant.

3- Clear explanation of all steps of the derivation.

None (see below for minor questions)

The authors present a general formalism for the cooling of quantum gases through uniform particle loss. While often associated with heating it is shown that under certain conditions few-particle loss processes can also lead to cooling. The study is motivated by a series of recent experiments, e.g. in the groups of Schmiedmayer and Bouchoule. As such, it is timely and relevant.

The present work is particularly interesting because the existing formalism to describe such cooling is significantly extended to cover general N-body losses, as well as arbitrary dimensions and realistic trapping potentials. For example, the cooling of a 1D gas through 3-body losses has recently been studied in an experiment by some of the authors for the first time. The results show good agreement with the theoretical predictions outlined in the present study. It will be very interesting to check experimentally if the predictions also hold in 3D situations, where evaporation (i.e. cooling through selective removal of particles with above average energy) will compete with the mechanism studied here (uniform loss of particles).

The study is well written and clearly explains all assumptions and steps of the derivation, as well as some limits of the theory. In particular, it nicely describes the inherent competition between the cooling of the low energy modes and their heating through shot noise.

A few minor questions:

1- Footnote 1: It is not quite clear to me what exactly the remark on Ito / Stratonovich formalisms refers to here? Could the authors briefly elaborate to make this clearer for the general reader?

2- Is there a simple way to estimate for which experimental parameters one would expect the assumption of Poissonian, uncorrelated shot noise to hold for the loss process?

3- In realistic experiments there will often be different loss processes present at once (e.g. three-body loss from interatomic collisions due high atomic densities, and one-body loss from background gas collisions), each with their own asymptotic temperature. What would one expect to see in these cases?

4- Is there a deeper meaning / interpretation behind the asymptotic temperature? Particularly Fig. 1b seems to suggest that the cooling exhibits some universal properties?

5- It would be nice to discuss if the gases become more degenerate during the cooling process. Can new regimes be reached, e.g. for 1D Bose gases?

## Author Isabelle Bouchoule on 2018-09-10

(in reply to Report 1 on 2018-07-26)We thank the referee for her/his careful reading of the manuscript

and we are glad to hear that she/he appreciates the presented work.

We answer below to her/his comments and questions:

1. In the stochastic equation for $N$ (Eq. 1), the variance of the random

variable $d\xi$ depends on $N$ (see Eq. 2). For a differential equation

for $N$ of the form $dN = -A(N)dt + d\xi$ with an $N$-dependent stochastic

term (namely $\langle d\xi(t)d\xi(t') \rangle = f(N) \delta(t-t')$), one

should specify whether the stochastic equation is written in the Stratonovich

or in the Ito formalism. However, since N(t) presents only small fluctuations

around its mean value $N_0(t)$, one can replace $N$ by $N_0(t)$ when computing the

stochastic term. Then, the resulting equation for $\delta N = N - N_0$ has

a stochastic term which does not depend on $\delta N$ (see Eq. 3). In such

a case the Ito and Stratonovich formalisms are equivalent.

In order not to confuse the reader not familiar with stochastic differential

equations, we prefer to remove the footnote. The reader aware of the subtle

details of stochastic equations will figure out himself that differences

between Ito and Stratonovich equations are irrelevant here.

2. The loss process may be assumed to be of Poissonian nature, as long as we

consider it on a time interval dt small enough so that the number of lost

atoms is very small compared to $N_0$: then the loss rate is constant

during the time interval dt, which amounts to a Poissonian process.

3. The question of the presence of multiple loss processes could a priori

be addressed within our formalism, provided Eq.20 is modified to account for

each loss process. Then Eq.23 would be modified as well. We foresee that

the temperature will still take values close to $mc^2$. We believe that such

a question, while interesting and relevant, deserves a separate study,

and we prefer to skip it in the present paper.

4. Unfortunately, we do not have a simple argument that shows that the

ratio $k_B T/(mc^2)$ goes towards a stationary value as a result of losses.

In the introduction and later in the text (after Eq.3 and after Eqs.23-26),

we emphasize the underlying physics: cooling due to the decrease of density

fluctuations on the one hand, and heating due to the stochastic nature of losses,

on the other. To our knowledge however, only quantitative calculations permit to

conclude that the relevant quantity, which takes a stationary value, is the

ratio $k_B T/(mc^2)$.

5. In the conclusion, we added a brief discussion what

may eventually happen with the ultracold gas as the density and temperature are

lowered. It indeed crucially depends on the system dimensionnality whether quantum

degeneracy increases or decreases.