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Entanglement spreading in nonequilibrium integrable systems
by Pasquale Calabrese
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Authors (as registered SciPost users):  Pasquale Calabrese 
Submission information  

Preprint Link:  https://arxiv.org/abs/2008.11080v1 (pdf) 
Date submitted:  20200826 12:10 
Submitted by:  Calabrese, Pasquale 
Submitted to:  SciPost Physics Lecture Notes 
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Ontological classification  

Academic field:  Physics 
Specialties: 

Approach:  Theoretical 
Abstract
These are lecture notes for a short course given at the Les Houches Summer School on "Integrability in Atomic and Condensed Matter Physics", in summer 2018. Here, I pedagogically discuss recent advances in the study of the entanglement spreading during the nonequilibrium dynamics of isolated integrable quantum systems. I first introduce the idea that the stationary thermodynamic entropy is the entanglement accumulated during the nonequilibrium dynamics and then use such an idea to provide quantitive predictions for the time evolution of the entanglement entropy in arbitrary integrable models, regardless of the interaction strength.
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Reports on this Submission
Anonymous Report 3 on 20201210
(Invited Report) Cite as: Anonymous, Report on arXiv:2008.11080v1, delivered 20201210, doi: 10.21468/SciPost.Report.2275
Strengths
Well written
Pedagogic
Selfcontained
Weaknesses
None.
Report
In "Entanglement spreading in nonequilibrium integrable systems", the author summarizes a set of lectures given at the 2018 Les Houches school on "Integrability in Atomic and Condensed Matter Physics". These lecture notes provide a brief overview of the how the evolution of entanglement can be understood in a system after a quantum quench.
The notes begin with a definition of what is meant by thermalization in a closed quantum system (important so as to establish the framework of the discussion) and then follow with a brief discussion of the notion of entanglement entropy. The notes then move into their central section, a discussion of the quasiparticle picture of entanglement spreading. This picture provides an intuitive semiclassical description to the growth of entanglement after a quantum quench. It envisions entanglement growing because a quench, which pumps finite energy density into a system, creates pairs of counterpropagating quasiparticles which fly apart after the quench, so spreading entanglement (and correlations) throughout the system. This simple picture, originally developed by the author with John Cardy in the context of quenches in conformal field theories (CFTs), has proven to be remarkably robust and applied to sundry cases beyond that of mere CFTs.
Having developed the quasiparticle picture, the author then goes on to show that it is not a mere cartoon but that it can be used to provide a quantitatively accurate computation of the growth of entanglement entropy postquench. He ends these notes with a number of limitations on the immediate applicability of the quasiparticle picture including to the postquench evolution of the Renyi entropies and to the nonequilibrium dynamics of nonintegrable systems.
I believe these notes meet the criteria set out for SciPost Lecture notes inasmuch as they cover a topic of current interest to the community and they provide a clear, wellreferenced, introduction to the concept of entanglement spreading.
Requested changes
My only comments are minor ones, mostly asking for typos or solecisms in the English to be fixed. Page numbers here are with reference to v2 on the arXiv.
i) Eqn. 4: There is a product \prod_i missing on the r.h.s. of Eqn. 4.
ii) pg 4: "that would be a nonsense" > "that would be nonsensical"
iii) top of pg. 6: "get similar values" > "approximately equal."
iv) pg 7: It might be worth stressing that oppositely counterpropagating quasiparticles results from a translationally invariant quench where the finite energy density state that results has zero momentum.
vi) pg 11: "It then exists ..." > "There then exists ..."
vii) pg. 13: "In turns, the developing ..." > "Correspondingly, the development ..."
viii) pg. 15: "Unfortunately, it is still not know" > "Unfortunately, it is still not known"
ix) Perhaps somewhere in the vicinity of Section 7.5 a paragraph discussing the results of the author's own Ref. 51 might make sense. This is a nice result and can be readily be understood in terms of the quasiparticle picture.
Anonymous Report 2 on 2020107 (Invited Report)
 Cite as: Anonymous, Report on arXiv:2008.11080v1, delivered 20201007, doi: 10.21468/SciPost.Report.2056
Strengths
1 Very pedagogical
2Easy to read for newcomers
3 Avoids technical discussions
4Quite complete coverage of key topics and related questions
5Very good and balanced literature coverage as a source for further reading
Weaknesses
No weaknesses as far as I can see.
Report
This review provides and excellent and very pedagogical introduction into the theoretical description of entanglement spreading in nonequyilibrium integrable systems. The basic concepts  nonequilibrium dynamics in quantum quenches, thermalization in closed quantum systems, eigenstate thermalizatiin hypothesis, notion of integrability in quantum systems, vonNeumann
and Renyi entanglement entropies, entanglement dynamics in free systems and its calculation, as well as the picture of entanglement spreading via quasiparticle production and ballistic spreading are introduced. The review is kept nontechnical and refers the reader to specialized literature where necessary.
The review further makes contact to experimental efforts with quantum gases and ion traps, discusses perspectives on how to describe entanglement spreading in nonintegrable systems and open systems and closes with a brief mentiuoning of generalized hydrodynamics as powerful tool to deal with spatially inhomogeneous systems.
In my opinion, this will be a very useful and excellent review on the topic and I recommend its publication in essentially its present form. Some minor points and optional suggestions are listed below for the author's consideration.
Requested changes
1 Page 2: von Neumann is misspelled: Von instead of von.
2 Page 4, 5 lines below Eq 7: double "the"
3 References to numerical tests of ETH are perhaps a bit selective, in particular, since no recent papers are cited. I cannot make a specific recommendation about what to cite, but there are many other people who contributed significantly (e.g., Lea Santos, Peter Prelovsek, Lev Vidmar, Robin Steinigeweg, Jochen Gemmer, and others). This is not central to the review's main topic, though.
4 Page 5: is the question of completeness of sets of conserved operators settled for typical integrable models, such as e.g., the spin1/2 Heisenberg chain? I am not aware of a mathematical proof, in particular, given the newly discovered quasilocal charges. See the sentence at the end of the 1st paragraph.
5 Page 5: Is "Neither" perhaps a typo and should read "Noether"?
6 Page 8, 2nd paragraph: missing "of" in "pairs quasiparticles"
7 In Sec. 6.4.7, one could add a reference to Phys. Rev. B 90, 075144 (2014)
8 The author could (optionally) add an outlook onto open technical and conceptual questions.
Anonymous Report 1 on 2020103 (Invited Report)
 Cite as: Anonymous, Report on arXiv:2008.11080v1, delivered 20201003, doi: 10.21468/SciPost.Report.2041
Strengths
1An excellent account of entanglement spreading in integrable quantum systems out of equilibrium.
2All the relevant literature is cited, particularly useful to the newcomers to the field.
3Very pedagogical structure of the notes.
Weaknesses
1Some chapters have unclear motivation.
2Some statements may not be clear to nonexperts.
Report
This lecture course is an excellent summary of a very timely topic of entanglement spreading in integrable quantum systems out of equilibrium. The first three chapters give an indepth introduction leading up to the discussion of entanglement entropy in manybody quantum systems. The rest of the material is concerned with the quasiparticle picture, giving a short background and recounting the most important advancements in the field.
Overall, I find these notes very well written and I like how they are structured: introductory material is given an indepth treatment, while more difficult concepts are summarised and properly cited. This gives students and newcomers to the field a strong background and a good overview of the current state of the field. However, I also feel that there is not enough motivation given at the beginning of some chapters, which may confuse the students significantly as to why are we interested in some of the derivations and problems. There are also multiple statements which may seem puzzling to the newcomers.
I recommend publishing this text in SciPost Physics Lecture Notes, but only after minor additions and corrections listed below are addressed by the author.
Requested changes
1) Abstract: I would strongly suggest mentioning the word "quasiparticle picture" in the abstract, as this topic takes most of the discussions in these lecture notes.
2) Page 2, "despite the fact that the dynamics governing the evolution is unitary and the initial state is pure": It would be useful to explain why is this surprising, i.e. that unitary evolution should lead to deterministic dynamics, where one can rewind time and read off the initial nonequilibrium state of the system. "Thermalisation" implies, however, that such rewinding should not be possible.
3) Page 3, "Let us consider a spatial bipartition of the system": More motivation is needed here, specifically why are we interested in bipartition and local operators. One can, for example, mention that in experiments we can usually only access local observables. This then naturally implies that the question "do we see thermalisation in quantum systems?" should be reformulated to "do local measurements see thermalisation?".
4) Page 5, "only integrals of motion with some locality or extensivity properties must be included in the GGE": At this point, it would be useful to give a simple example of what integrals of motion can enter GGE, as a direct comparison to the example of projectors on the eigenstates, which *cannot* enter GGE.
5) Page 6, Eq. 15: It would be useful to mention that the natural logarithm used in the definition of entropies is sometimes changed to $\log_2$, or even, $\log_{10}$. $\log_2$ is often used in the context of quantum information, where the natural unit of entropy is the maximum entropy of a spinhalf singlet state.
6) Page 6: "Then, for integer n >= 2, they are the only quantities that are measurable in coldatom and iontrap experiments": I would suggest mentioning here that the n=2 Renyi entropy is directly related to purity, a quantity of interest for quantum information science.
7) Figure 2: For panel (b), please indicate what is the $\Delta$ used.
8) Page 9, "(the anisotropic Heisenberg model)": Since in the figures and later in the lecture notes, the name "XXZ chain" is used, I would say "(the anisotropic Heisenberg model, also known as the XXZ chain)".
9) Page 10, "The interpretation of Eq. (25) is obvious": For inexperienced students, it may not be so obvious, so it would be good to mention that the form of H(n) can be derived easily considering a 2x2 diagonal density matrix with n and (1n) on the diagonal, corresponding to occupied and unoccupied modes.
10) Page 11, "JordanWigner and Bogoliubov transformations": I would strongly suggest putting references here. Even better, one could add a reference to a stepbystep derivation from Eq. 29 to Eq. 30.
11) Page 12, "Intuitively, a nstring solution corresponds to a bound state of n elementary particles with n = 1.": I am puzzled by the clause "with n=1". Surely, the definition of a generic nstring solution should not include this clause?
12) Page 14: I would strongly suggest promoting the whole subchapter 6.4 to chapter 7, as it serves as a conclusion for these lecture notes and an outlook for the future.
13) Page 17, Chapters 6.4.5 and 6.4.6: Although the author briefly mentions the topic of random quantum circuits, it would be good to stress here that there has been extraordinary interest in these systems in the recent years. They have been used to probe entanglement dynamics in various scenarios, e.g. competition between unitary evolution and measurements, which can lead to extensive or subextensive entanglement behaviours, a topic which also ties into Ch. 6.4.6 on open systems and effects of the environment.
14) Minor spelling/interpunction:
* "Neither theorem" > "Noether's theorem" (page 5)
* add a period to the end of the sentence "Here we just summarise the main ingredients we need and then move back to the entanglement dynamics" (page 12)
* "a nstring solution" > "an nstring solution" (page 12)
* add a period to the end of the paragraph in chapter 6.4.6 (page 18)
15) Minor editing of equations, as it is sometimes difficult to read:
* cos x > cos(x), sin x > sin(x) in Eqs. 1618
* space after the variables of integration in Eqs. 2022, 34, 37, 42
Author: Pasquale Calabrese on 20201211 [id 1073]
(in reply to Report 3 on 20201210)I thank the referee for reading my Lectures notes and for the very positive comments.
Unfortunately, I cannot fix the minor eight typos she/he spotted because the manuscript is already published.
Pasquale Calabrese