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As Contributors: | Everard van Nieuwenburg |

Arxiv Link: | http://arxiv.org/abs/1802.08262v2 |

Date submitted: | 2018-03-07 |

Submitted by: | van Nieuwenburg, Everard |

Submitted to: | SciPost Physics |

Domain(s): | Theoretical |

Subject area: | Quantum Physics |

We show that a quantum many-body system may be controlled by means of Floquet engineering, i.e., their properties may be controlled and manipulated by employing periodic driving. We present a concrete driving scheme that allows control over the nature of mobile units and the amount of diffusion in generic many-body systems. We demonstrate these ideas for the Fermi-Hubbard model, where the drive renders doubly occupied sites (doublons) the mobile excitations in the system. In particular, we show that the amount of diffusion in the system and the level of fermion-pairing may be controlled and understood solely in terms of the doublon dynamics. We find that under certain circumstances the diffusion in the system may be eliminated completely. We conclude our work by generalizing these ideas to generic many-body systems.

Has been resubmitted

Resubmission 1802.08262v3 (7 June 2018)

Submission 1802.08262v2 (7 March 2018)

Interesting and relevant topic.

See report.

1) Not very clear notation

2) Numerics only for dilute case

3) Incomplete list of references

4) Confusing discussion of transport

Disclaimer: I am one of the authors of the numerical study of transport in interacting Floquet systems Ref. [22, SciPost Phys. 3, 029 (2017)], which is challenged in the discussion of the present paper.

The authors present a very interesting study of the fate of dynamical localization in periodically driven systems in the presence of interactions. For such systems, it was shown recently in the numerical study in Ref. [22, SciPost Phys. 3, 029 (2017)] that interactions generically destroy localization and induce diffusive transport. In the present manuscript it is argued using perturbation theory that there are situations where dynamical localization can survive even in an interacting system. The argument is based on a perturbative construction of a hierarchy of increasingly complex mobile entities, identifying a criterion (constant offset of the oscillating electric field, or periodic drive of the interaction) under which not only the effective single particle states are localized due to dynamical localization, but also two particle entities, notably doublons or neighborons. The authors also present numerical simulations in support of their results as well as a comparison to the full many-body simulations of Ref. [22].

Overall, the results are very interesting and promising, since they also yield an analytical form for the effective hopping, which matches the diffusion constant calculated in Ref. [22], however there are several points in this study, which I think could be improved:

+ The list of references should be extended:

- The references concerning discrete time crystals miss the pioneering work by Khemani, Lazarides, Moessner and Sondhi Phys. Rev. Lett. 116, 250401 (2016) and by Else, Bauer and Nayak Phys. Rev. Lett. 117, 090402 (2016).

- The authors use a transformation of Floquet systems into a static problem, which to the best of my knowledge was first introduced by Jon H. Shirley Phys. Rev. 138, B979 (1965).

+ The presentation of the derivation of the main result is somewhat obscure and could be improved significantly. In particular it appears that some details and definitions are missing, thus making the derivation hard to follow.

The main difficulty in the presentation of the section “II Background” seems to arise due to the repetition of the work of Jon Shirley (PR 138, B979 (1965)), leaving out important details. I suggest to refer to Shirley’s derivation and to follow his presentation to mitigate these problems. An example of the non standard form is e.g. Eq. (8), where it remains obscure where the photons come from and what the “Floquet form” is. In particular, Eq. (8) corresponds only to *one* solution of Eq. (3), whereas the Floquet theorem is a statement about the fundamental system of the differential equation, which one could for example get by writing the operator c_n (which is an LxL matrix) as a vector of length $L^2$.

+ The discussion of the results in Sec IV A should be clarified. As far as I understand it, within second order perturbation theory an effective model in Eq. (15) is derived, which is a simple tight binding model of doublons. Therefore, transport of doublons can only be ballistic. The authors write e.g. two lines after the heading B. Doublon Localization “and the system becomes diffusive due to the free motion of doublons”, which is clearly incompatible with Eq. (15).

+ My main critique is the discussion of the numerical results from Ref. [22]. These results show very clearly that the MSD, quantifying stroboscopic transport in a half filled, truly many-body driven system, grows linearly in time. It was shown in Ref. [22], that the domain of the linear growth grows also linearly with system size up to quite large system sizes, as predicted for clean diffusion, indicating that indeed bulk transport is probed and that the results do not suffer from transient boundary effects. Also note that the MSD is directly connected to the current-current correlation function and is therefore a direct measure of the nature of transport. The authors argue that transport in the same system (spinless fermions, which are discussed only in the appendix), is in fact ballistic and was incorrectly interpreted as diffusive due to finite size effects. This statement seems to be in conflict with the numerical evidence. Moreover, neither in the main text nor in the appendix the authors present the equation of motion for the neighborons, which is relevant for the system in Ref. [22]. If this equation contains interactions between the neighbourons, generically diffusion would be expected.

In the numerical data of Ref. [22], a clear ballistic regime exists for very short times (constant as a function of system size), corresponding to a mean free path of one or two lattice sites, as expected in a half filled system, before the asymptotic diffusive transport kicks in.

Using the assumption that the bulk transport in Ref. [22] is instead ballistic (contradicting numerical evidence), the authors equate the diffusion constant found numerically in Ref. [22] to the ballistic neighboron velocity, yielding the stunning correspondence presented in Fig. 2. At this stage, it remains unclear to me how this correspondence occurs, since the logic presented is not only in conflict with the numerical evidence, but also not self-consistent (e.g. in ballistic systems the mean free path has to be larger than the system size). This is apparent from the figure label in Fig. 2c, where an effective velocity (solid line, result of this paper) is compared to a diffusion constant (points, numerical result from Ref. [22]).

Therefore it seems that some argument is missing in the logic to explain the good agreement with numerical simulations. Such an argument could be an analytical calculation of the mean-free path, which given the good agreement between the velocity and the diffusion coefficient, should be of the order of unity.

+ In the present work, two models are considered, most crucially the driven Fermi-Hubbard model (FHM) as well as the model of driven spinless fermions studied in Ref. [22]. The authors made an effort to separate the discussions of the two models by moving the spinless fermions model to the appendix., However they still compare their results to the results of Ref. [22], while the remaining results are for the behavior of doublons in the FHM. This leads to an intertwined discussion of the two models in Sec. IV, which is somewhat confusing. I suggest that the two models are strictly separated and not discussed in parallel to make it more clear.

In particular, the effective neighboron Hamiltonian for spinless fermions should be stated explicitly, since this is the model which is compared to the numerical results.

+ The authors present numerical data confirming the localization of doublons according to their perturbative analysis. However, they limit their simulations to the dilute case of only 3-4 particles in the lattice. In this case, they find that the doublon lifetime is very long, justifying the analysis. For the strongly interacting limit, the case of half filling is more relevant and was considered in Ref. [22]. It is known from an analysis of the lifetime of doublons (e.g. [Phys. Rev. Lett. 104, 080401 (2010)]), that in the case of half filling and an interaction energy of the order of the kinetic energy this time is rather short. In this limit, it is not clear if the analysis in this paper is relevant for long enough times.

+ In summary, these arguments also cast doubt on the claim that the localization of doublons survives at higher filling and is a disorder free mechanism of localizing a many-body system.

In conclusion, I think that this paper contains very interesting and important results, which are surely relevant for the dilute case. Furthermore, the very good agreement of the analytical calculation with the numerical data in Ref. [22] suggests that a deeper insight can be gained also in the dense regime. However, the current form of the discussion contradicts exact numerical simulations for large many-body systems, suggesting that there is maybe a missing argument to explain this good agreement in Fig. 2c, which could maybe be fixed by focussing on the analysis of the diffusion constant and the mean free path in the dense case. The analytical part of the article could benefit from a more detailed and clear presentation.

I cannot recommend publication of the paper in the present form, due to the apparent inconsistency in the discussion of the results. However, I am confident that the authors will be able to improve the discussion along the above comments. I am convinced that this will lead to a deeper theoretical understanding of diffusion in driven systems and make it a valuable contribution to SciPost Physics.

1) Correct discussion of transport

2) Improve presentation of analytical result

3) Separate discussion of spinful and spinless models

1) Interesting topic & careful study

2) Discussion on interaction effects on dynamical localization. This is an important aspect of Floquet engineering in interacting systems

3) High quality of the discussion

4) Analytical arguments supported by few-particle simulations

see report

The paper investigates the physics of dynamical localization in the presence of interaction. The authors show how in a regime where single particles are localized due to a fine-tuned Floquet driving term, two- and more particle excitations can still propagate. Importantly, the authors identify a long time scale tau, below which the localized single particle dynamics separates from the delocalized two particle dynamics. The paper also investigates how two-particle excitations are localized and generalizes the 1d results to higher dimensions and generalized Hamiltonians.

Overall this is a careful, high-quality study of an interesting problem. It addresses genuine interaction effects in the field of “Floquet engineering”.

I have, however, two remarks/questions which may require some modifications of the paper

1) The authors use several times the phrase “non-interacting hard core bosons”. While in 1d hard-core bosons can indeed be mapped to non-interacting fermions, hard core bosons in higher dimension actually are strongly interacting (they have a non-trivial scattering cross section and are, e.g., diffusive for finite temperature and densities rather than ballistic). I would or example expect that the system described by Eq (18) shows a non-trivial two doublon dynamic even when single-doublons are localized dynamically. I would recommend to point out the difference of 1d and higher d in this respect and avoid the term “non-interacting hard core bosons” in higher dimensions completely.

2) The authors claim that for a static linear doublon potential there is no diffusion “to all orders in perturbation theory”. This statement is not explained and perhaps misleading (depending on the precise definition of “diffusion”). Even in the presence of a linear potential a generic interacting system will show some sort of subdiffusion, see e.g. arXiv:1101.4508

Minor remarks: Below Eq. (12) “The last term…” should probably be replaced by “The first term…”. Below Eq. (18): The authors write “As in the 1D case, the non-diffusive phase is not fine tuned”. I guess this statement refers only to the static and not the dynamics case.

see report