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Bose polaron in a quantum fluid of light
by Amit Vashisht, Maxime Richard, Anna Minguzzi
This is not the latest submitted version.
Submission summary
| Authors (as registered SciPost users): | Anna Minguzzi · Maxime Richard · Amit Vashisht |
| Submission information | |
|---|---|
| Preprint Link: | scipost_202107_00019v1 (pdf) |
| Date submitted: | July 12, 2021, 4:29 p.m. |
| Submitted by: | Amit Vashisht |
| Submitted to: | SciPost Physics |
| Ontological classification | |
|---|---|
| Academic field: | Physics |
| Specialties: |
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| Approach: | Theoretical |
Abstract
We study the Bose-polaron problem in a nonequilibrium setting, by considering an impurity embedded in a quantum fluid of light realized by exciton-polaritons in a microcavity, subject to a coherent drive and dissipation on account of pump and cavity losses. We obtain the polaron effective mass, the drag force acting on the impurity, and determine polaron trajectories at a semiclassical level. We find different dynamical regimes, originating from the unique features of the excitation spectrum of driven-dissipative polariton fluids, in particular a non-trivial regime of motion against the flow. Our work promotes the study of impurity dynamics as an alternative testbed for probing superfluidity in quantum fluids of light.
Current status:
Reports on this Submission
Report #2 by Anonymous (Referee 2) on 2021-9-15 (Invited Report)
- Cite as: Anonymous, Report on arXiv:scipost_202107_00019v1, delivered 2021-09-15, doi: 10.21468/SciPost.Report.3524
Strengths
2-Effective graphics
3-Well written
Weaknesses
2-Lacks some discussion
Report
First of all I think that the means (numerical, analytical...) with which the results are obtained should be stated more clearly, for example at the beginning of Section 4.
Another point that in my opinion is important to discuss is the experimental relevance of these calculations. In particular: how would a moving impurity be realized in an exciton-polariton condensate?
Moreover I think that the results of Ref. [22] are not quoted with sufficient clarity, since some of the results obtained here regarding the negative drag were anticipated in that paper, albeit with a much simpler model of a fixed impurity. A discussion of those results should be included in the Introduction.
Finally the exposition may benefit from adding some explanations to the theoretical part of Section 3, as I indicate in the "Requested changes", where I also indicate some minor points.
Even if I think that (after these changes) this work is well worth publishing, I am not sure that it meets one of the very selective expectations of SciPost Physics. While the paper contains interesting results obtained in an original way, I must admit that I do not see a groundbreaking discovery, a novel link between different fields or much follow-up work. For these reasons in my opinion the paper would fit better in SciPost Physics Core.
Requested changes
In order of appearance
1-I think the predictions of Ref.[22] should be reported in the introduction
2-A discussion of the experimental relevance of the calculations should be included
3-Operators $\hat{a}_\mathbf{k}$ in Eq. (2) and $\hat{\alpha}_\mathbf{k}$ in Eq. (4) are not defined
4-Maybe the $\hat{p}$ operator in equation (3) (and also in (10)) should be bold
5-I think the density n appearing after equation (8) is not defined
6-At the end of Sec. 2.1 and at the beginning of Sec. 2.2 it would be nice to have references for the Bogoliubov-Frolich Hamiltonian and the Lee Low Pines transformation
7-When $\Pi$ is an operator it should have the hat
8-After Eq. (22) a coherent state of excitations is considered. When is this a valid procedure? I think some comment is worth adding.
9-At the end Sec. 3.2 I think the definition of the effective mass and of $\eta$ and how they follow from Eq. (26) should be explained in more detail
10-Also the definition of the drag force in Eq. (28) would benefit from some more details. Also I think $n_{imp}$ is not defined.
11-Eq. (28) and (29) should have only one number
12-In the line after (29) ie should be i.e.
13-A discussion of the solution methods should be added in Section 4
14-At the end of the second paragraph of Sec. 4.1 the value $\Delta/gn=2$ is used to distinguish the different regimes, but in Fig. 2 $\Delta/gn=1$ appears as a threshold
15-I could not find a definition of the $\Gamma$ independent of $\mathbf{k}$ that is used in Section 4
16-Is "decreasing $\Gamma$" in at the end of Sec. 4 supposed to be "increasing $\Gamma$"
17-In the conclusions it is stated that for $\Delta>0$ the impurity is subjected to negative drag force, but this does not always happen for $\Delta>0$
18-In the caption of Fig. 6, in the list of values of $\Delta$, there is a cursive "and"
Report #1 by Anonymous (Referee 1) on 2021-8-25 (Invited Report)
- Cite as: Anonymous, Report on arXiv:scipost_202107_00019v1, delivered 2021-08-25, doi: 10.21468/SciPost.Report.3438
Report
The manuscript by A. Vashisht et al. discusses the properties of a single impurity in a driven-dissipative polariton bath. The paper is very well written, the problem is experimentally interesting, the formalism is clearly explained, and the equations and the results appear correct. As such, I can surely recommend publication of this manuscript in SciPost.
Upon resubmission, I think the Authors may extend the discussion on the key result presented here, i.e., the presence of a region of negative effective mass. In particular, is there an intuitive understanding of why such effect appears when the Bogolubov dispersion becomes complex? If I understood correctly, such effect was already noticed in earlier works on static impurities (Refs. [22,23]). In this case, this discussion may be placed already in the Introduction.
Here below follow further minor remarks and suggestions, presented in chronological order, that the authors may want to take into account.
