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Measurement-induced criticality in extended and long-range unitary circuits
by Shraddha Sharma, Xhek Turkeshi, Rosario Fazio, Marcello Dalmonte
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|Authors (as registered SciPost users):||Marcello Dalmonte · Shraddha Sharma · Xhek Turkeshi|
|Preprint Link:||https://arxiv.org/abs/2110.14403v2 (pdf)|
|Date submitted:||2021-11-10 05:42|
|Submitted by:||Sharma, Shraddha|
|Submitted to:||SciPost Physics Core|
We explore the dynamical phases of unitary Clifford circuits with variable-range interactions, coupled to a monitoring environment. We investigate two classes of models, distinguished by the action of the unitary gates, which either are organized in clusters of finite-range two-body gates, or are pair-wise interactions randomly distributed throughout the system with a power-law distribution. We find the range of the interactions plays a key role in characterizing both phases and their measurement-induced transitions. For the cluster unitary gates we find a transition between a phase with volume-law scaling of the entanglement entropy and a phase with area-law entanglement entropy. Our results indicate that the universality class of the phase transition is compatible to that of short range hybrid Clifford circuits. Oppositely, in the case of power-law distributed gates, we find the universality class of the phase transition changes continuously with the parameter controlling the range of interactions. In particular, for intermediate values of the control parameter, we find a non-conformal critical line which separates a phase with volume-law scaling of the entanglement entropy from one with sub-extensive scaling. Within this region, we find the entanglement entropy and the logarithmic negativity present a cross-over from a phase with algebraic growth of entanglement with system size, and an area-law phase.
Submission & Refereeing History
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- Report 4 submitted on 2021-12-22 16:22 by Anonymous
- Report 3 submitted on 2021-12-21 12:16 by Anonymous
- Report 2 submitted on 2021-12-15 11:08 by Anonymous
- Report 1 submitted on 2021-11-30 09:13 by Anonymous
Reports on this Submission
- Cite as: Anonymous, Report on arXiv:2110.14403v2, delivered 2021-12-22, doi: 10.21468/SciPost.Report.4082
1 - Timeliness
2 - Fresh and fruitful idea to compare the information dynamics in quantum circuits with clustered and long-range unitary gates
3 - Several complementary observables are studied numerically
1 - The models studied numerically are introduced and described in not particularly clear terms
2 - The manuscript presents numerical studies only, without any attempts of describing and explaining the results in analytical terms (within some toy model, or, at least, by means of plausible speculations)
3 - The current version of the manuscript only reports observations; the work would highly benefit from strengthening the conclusions based on these observations and highlighting the relevance of these conclusions to the field
The manuscript addresses numerically entanglement in the two specific models of quantum circuits with spatial correlations. The subject of the study is very topical; the obtained results, showing the difference in the information dynamics and the entanglement phase diagrams between the two models, are novel and interesting.
Unfortunately, the authors suggest no general conclusions based on their numerical results, which could emphasize the relevance of the work to the field. The statements like "... the fixed point is compatible with the one of short-range Clifford circuits" and "... consistent with the one reported in Ref. , suggesting that ... the measurement induced transition is governed by the same underlying ... theory despite the protocols being different" are too specific to the models addressed in the paper. Apparently, these models were chosen to demonstrate some more general properties of the corresponding classes of systems. For this purpose, a more extended discussion of the numerical observations in analytical terms is necessary.
The description of the models and the protocol should be modified. The main problem is that the unitary gate defined in Eq. (3) does not seem to define the CHRC as described in Fig. 1. Indeed, if one naturally assumes that Eq. (3) describes each of U-blocks in Fig. 1a, i.e., the time variable t corresponds to the whole block there, the "fine structure" (internal architecture) of the large U-block shown in Fig. 1b (left) is not actually defined in Eq. (3). Indeed, the pattern of the elementary small boxes in Fig. 1b (left) is very specific, suggesting the introduction of a certain "time-ordering" inside the large U-block, which is missing in the formal equation for U(t). ("The unitary gates U(t) are laid out in a manner that mimics a soft-shoulder potential extending over M sites" -- is this layout crucial for the CHRC model, or one can use an arbitrary ordering?). If, however, the time step t refers to a horizontal slice in Fig. 1b(left) rather than in Fig. 1a, Eq. (3) does not describe Fig. 1b(left) since all sites i are involved in the product in Eq. (3), while there are empty sites in each elementary slice in Fig. 1b(left). To avoid confusion, the authors should define their models (and notation) in a much more careful way!
The randomness in the gates, as well as the definition of averaging over this type of randomness, should also be described explicitly in analytical terms.
In addition to this major point, there are also related minor issues:
- The circuit realization Km in Eq. (1) requires an explicit analytical representation in the form Km=... (may be given after defining the elements of the hybrid circuit)
- It would be nice to add the label (+-) to the projectors in Eq. (2)
- The caption of Fig. 1 says: "M = 4 in the above illustration". However, this is not what is seen in the figure, where the dashed links between the largest pairs of the smallest blocks have different lengths (in particular, the top left block obviously has M>4)
- The different colors used for pairs in Fig. 1b(right) should be explained in the figure caption
Now, turning to the results, it would be nice to have the data points for M=3 and M=5 in Fig. 4, especially in the upper right panel for nu (by the way, the panels are not labeled in contrast to what the figure caption says). Is it clear why M=6 is the "magic cluster range" beyond which the area-law phase disappears?
Figure 7: It is not clear what the numerical evidence for the vertical dashed-dotted line at alpha=2 is provided. Is it at all possible, with available system sizes and accuracy shown by error bars, to distinguish in such a phase diagram between the "algebraic phase" and a crossover region separating the area-law and volume-law phases?
Finally, it would be interesting to compare the findings
In conclusion, while the manuscript present interesting new numerical results, I cannot recommend it for publication in its present form (see above). The models should be described in a more careful way, and some numerical observations should be further clarified. The manuscript can be reconsidered for publication after the authors have modified the manuscript accordingly. In addition, I strongly suggest that the authors extend the discussion section (which is currently only presents a list of observations) by adding some analytical arguments emphasizing the generality of their findings. Recent preprints https://arxiv.org/abs/2110.02988 and https://arxiv.org/abs/2111.08018 might be helpful in this respect.
PS. Minor grammar issues/typos (an incomplete list):
p. 2: "These systems comprise of random unitary gates..." --
perhaps, the authors meant "consist of" or "comprise" (without "of"); for a related discussion on "comprised of", see
p. 2: "where analytical results where obtained" -- were obtained
p. 3: "Our analysis suggest the fixed point" -- suggests (or "our analyses suggest", but this sounds weird)
p. 4: "the system belong to the same universality" -- belongs
p. 5: "A review of stabilizer formalism, Clifford group and on the efficient numerical implementation based on the Gottesmann-Knill theorem are detailed in the Appendix" -- please, reconsider the sentence
p. 6, figure caption: "The normalization of the probability distribution P(r) impose..." -- imposes
p. 8: "We remark that SR act as an order parameter..." -- acts
p. 13: "Overall, our analysis show compatibility..." -- shows
p. 15: "Another recent article  considering tractable
large-N models also investigate..." -- investigated
1 - Clarify the model in Sec. 2
2 - Respond to question concerning Figs. 4 and 7 from the report
3 - Strengthen the discussion of the observations, putting the findings in a more general context and adding (semi-)analytical arguments
4 - Correct typos
- Cite as: Anonymous, Report on arXiv:2110.14403v2, delivered 2021-12-21, doi: 10.21468/SciPost.Report.4073
1- The topic is very relevant and the numerical investigation of the two-different long-range circuit models is comprehensive to a set of other recently appeared long-range models.
2- The paper is very accessible and provides a short and crisp summary of the obtained results. I find it particularly well written.
3- The summary of the entanglement-based observables and the numerical procedure are very precise and helpful.
1- While I find it helpful for the reader to display a Hamiltonian, which corresponds to the circuit dynamics, the precise connection between the two Hamiltonians and the circuit dynamics is missing, and might therefore be misleading.
2- The manuscript presents an exhaustive list of results but falls short in providing a deeper discussion or conclusion about the physics in the long-range model. After reading the paper, it feels like a list of numbers and facts but I'm not sure if I have gained much deeper insights.
The manuscript by Sharma et al. represents a comprehensive examination of long-range unitary circuit dynamics subject to local measurements. It appears very timely, since the entanglement dynamics in long-range hybrid quantum circuits has attracted a lot of attention recently. The scientific evaluation and presentation is very accessible and of high standard. Overall, I support publication of the present manuscript in SciPost Physics Core.
Below I mention two recommendation for the authors for potential changes. I'd leave it up to them if they want to consider them or not.
1- The authors might want to consider the points I mention under weaknesses. Especially a rectification of the correspondence to a Hamiltonian evolution might be very helpful and in order. While there is probably an analogy to the Hamiltonian models, it is clear that the circuits cannot mimic those Hamiltonians. Any continuous evolution with the interacting Hamiltonians leaves the space of free wave functions (either stabilizers or free fermions/bosons) and thus corresponds to a different class of correlated many-body states.
2- A little bit more of discussion of the results might be helpful. For instance some understanding of the the long-range models (also in terms of entanglement generation) was provided in the Refs. 49-51 and it might not be the worst to repeat some aspects of this discussion very briefly.
- Cite as: Anonymous, Report on arXiv:2110.14403v2, delivered 2021-12-15, doi: 10.21468/SciPost.Report.4047
1.) high relevance
2.) well structured presentation
3.) thorough analysis
The authors study two instances of long-range hybrid random Clifford circuits. This permits effective classical simulations and various phase transitions are studied in this setting.
In case of circuits where the probability of long-range two-qubit gates decays algebraically they confirm and extend the results found in .
The authors furthermore study multi-qubit (clustered) interactions which, to my knowledge, is the first time this has been done explicitly. They find that when the clusters are below a certain size usual measurement induced criticality is found, while in the limit of large clusters scrambling always wins.
The results found in this paper corroborate the general picture of long-range interacting hybrid circuits outlined in  and [2,3] for free and interacting fermions respectively. The study of hybrid multi-qubit interactions goes well beyond setups studied so far and is therefore a relevant contribution to the newly emerging field of hybrid dynamics.
Due to the thorough and timely analysis I recommend this paper for publication.
Consider changing Fig. 8 to log-log plot (L or 1/L) to highlight algebraic scaling of entanglement entropy.
1.) p. 2 "... Clifford circuits provide a viable path to understand ..."
2.) p. 22 Reference  "T. Müller ..."
- Cite as: Anonymous, Report on arXiv:2110.14403v2, delivered 2021-11-30, doi: 10.21468/SciPost.Report.3969
2) thoroughly investigated
3) clearly communicated
The paper investigates random circuits, where the applied quantum gates are randomly drawn from the Clifford group and where Pauli measurements are randomly performed in between consecutive gates . This permits a classical investigation of the dynamics of the models. Phase transitions in the dynamical evolution are explored as the range of interactions (implemented by the chosen gates) is varied. The paper predicts a range of interesting observations as the behavior of the critical exponents is studied. While not unexpected, a quantitative investigation of the findings is a highly relevant contribution to the very active field of dynamics in random circuits. Moreover the investigations are likely to become relevant for possible future experiments provided sufficient qubit numbers are reached.