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Equilibrium Fluctuations in Maximally Noisy Extended Quantum Systems
by M. Bauer, D. Bernard, T. Jin
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Submission summary
As Contributors:  Tony Jin 
Arxiv Link:  https://arxiv.org/abs/1811.09427v2 (pdf) 
Date submitted:  20181130 01:00 
Submitted by:  Jin, Tony 
Submitted to:  SciPost Physics 
Academic field:  Physics 
Specialties: 

Approach:  Theoretical 
Abstract
We introduce and study a class of models of free fermions hopping between neighbouring sites with random Brownian amplitudes. These simple models describe stochastic, diffusive, quantum, unitary dynamics. We focus on periodic boundary conditions and derive the complete stationary distribution of the system. It is proven that the generating function of the latter is provided by the HarishChandraItzyksonZuber integral which allows us to access all fluctuations of the system state. The steady state is characterized by non trivial correlations which have a topological nature. Diagrammatic tools appropriate for the study of these correlations are presented. In the thermodynamic large system size limit, the system approaches a non random equilibrium state plus occupancy and coherence fluctuations of magnitude scaling proportionally with the inverse of the square root of the volume. The large deviation function for those fluctuations is determined. Although decoherence is effective on the mean steady state, we observe that subleading fluctuating coherences are dynamically produced from the inhomogeneities of the initial occupancy profile.
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Reports on this Submission
Anonymous Report 2 on 2019212 (Invited Report)
 Cite as: Anonymous, Report on arXiv:1811.09427v2, delivered 20190212, doi: 10.21468/SciPost.Report.821
Strengths
1. Contribution to study of noisy many body systems, of great current interest for theoretical (and possibly practical) reasons.
2. Introduces rigorous methods in harmony with a clear physical picture for the case of the stochastic XX model
3. Establishes a complete description of the steady state for this model, based on (i) Explicit computations for low cumulants of the single particle density matrix (ii) An exact description of the generating function of the same in terms of the HarishChandraItzyksonZuber integral.
4. Discusses generalizations and potential generalizations to other models.
Weaknesses
1. It would be good to understand the results of the present work in terms of the authors' earlier work (Ref. 12) on the noisy Heisenberg chain. Since there is no free fermion picture here, it would be surprising if the present results apply, though that seems to be the implication after Eq. 1.
2. In the same way, the occupation number statistics at the end of Section 3 are presumably quite different from those in the stationary state of the symmetric exclusion process, where each site has an independent Bernoulli distribution.
Report
The study of the dynamics of noisy many body systems is relatively undeveloped, and the present work is a very useful step in the direction of understanding the steady state of a particular model. Exploiting the free fermion structure allows the steady state to be determined in great detail by a variety of methods. The statistics of the single particle density matrix are established in two physically relevant regimes.
Some generalizations to other models are discussed, including the more interesting case of a genuinely interacting system.
Requested changes
Can the meaning of "non random" be clarified in the description of the steady state?
Clarify relation to noisy Heisenberg spin chain. Ref. 12 doesn't actually discuss the relation mentioned after Eq. (1).
End of Section 1: "the rules of the diagrammatic..." What?
Small typo at the end of Section 4: "can be resumed" to "can be resummed"
Anonymous Report 1 on 20181227 (Invited Report)
 Cite as: Anonymous, Report on arXiv:1811.09427v2, delivered 20181227, doi: 10.21468/SciPost.Report.770
Strengths
1 Exact results for a steadystate distribution of observables in a tightbinding model with stochastic hopping. Due to unitary invariance they can be expressed in terms of integrals known from RMT.
2 Could potentially be of relevance in a number of different contexts. Importantly, and the authors do comment (speculate) on that, is that the results could be valid more generally and not just for the specific model.
Weaknesses
Mostly minor presentational issues.
1 Perhaps more explicitly comment on related settings.
Report
As highlighted in the "Strengths" the paper presents very nice exact results. Besides providing an explicit result it also opens new questions, in particular about possible "universality" of fluctuations. I therefore recommend its publication.
Requested changes
Some optional minor comments (mostly regarding presentation) are:
1 In introduction, while the authors do connect with related settings, if possible, it would be nevertheless useful to be more explicit about the model studied. E.g., connection to random circuits (can one make an exact statement to what circuit eq.(1) corresponds to); that would be of interest as in (recent) quantum circuits community they make specific predictions about fluctuations (e.g., diffusive v. KPZ). To master equations (what kind of master eq. should one have in mind for eq.(2)).
On p.3, 3rd line, they likely mean "XX spin chain with dephasing", and not general XXZ (in order to get H_0 with hopping only like in eq.(2))?
2 2nd paragraph on p.3: it could be missunderstood that only stochastic models give access to fluctuations, which is not the case. Large deviation formalism can be used also for master equations (and has been applied also for e.g. diffusive XX chain with dephasing, PRE 89, 042140 '14). It would be useful to mention some literature on that, review by H.Touchette, Phys. Rep. 478, 1 (2009) would be a good choice, especially because the authors anyway use/mention large deviation functions in the text.
3 It is worth considering to mention in the Introduction with respect to the HCIZ integral also RMT or "integrals over unitary Haar measure"  I think this will ring more bells (and attract readers) than just some technical name.
4 Using "perturbative" in e.g. title of Sec.2,3: A casual reader might misinterpret that e.g. Sec.2 are "just" perturbative results (in some small parameter), rather than **exact** results for loworder correlations. I understand that "perturbative" is meant with respect to expansion of the full distribution function, but using some other name would be better (similarly in the last paragraph on p.3 "...to first few orders." might seem to imply some perturbative expansion, while it means first few loworder correlations).
5 After eq.(8): readers familiar with RMT results, specifically averaging over unitary measure, will recognize those formulas as they appear in numerous contexts (thermalization, form factors, random channels...). Sequentially reading the paper it would help if already at that point the authors would reaffirm that this is so (even if they do explain it in details in the very next section).
6 2nd sentence after eq.(8): explain what is meant by "topological nature".
7 Sentence before eq.(13): mention what q is.
8 Sec.4: can one compare the results obtained with some classical diffusive model (e.g. SSEP), what if anything is different?
9 Sec.5: considering that all the proofs and details are given in the appendices, I am wondering if also Sec.5 fits more in the appendix.
10 Sec.6 is very interesting. I see 1st results about independence on mu_j as showing that even with disorder a random hopping destroys any signs of localization. Next two paragraphs are intriguing. The authors argue that even with interactions the stationary distribution might stay the same. On the other hand, a (likely) scenario is also that the convergence radius goes to zero (with system size)? For exact results in the paper two conditions are crucial: (i) free model, (ii) unitary invariance. One can ask if both are necessary? At some point the authors do mention that the generators are ergodic (resulting in unitary invariance) only in the 1particle sector, so a free nature of the model seems crucial. On the other hand, here in Sec.6, the argument seems to be that fluctuations will be the same provided generators L_j span the whole group (which means for almost any generic "noisy" evolution)  that would mean a rather general universality of the results derived. An argument why this is perhaps too much to expect would be that fluctuations are on physical grounds connected to relaxation (if the regression theorem holds this is an exact statement)  they can be different for slow vs. fast relaxation, while in the presented work there is no dependence on relaxation.