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Density matrices in integrable face models
by Holger Frahm, Daniel Westerfeld
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Authors (as registered SciPost users):  Holger Frahm · Daniel Westerfeld 
Submission information  

Preprint Link:  https://arxiv.org/abs/2104.06269v1 (pdf) 
Date submitted:  20210414 12:06 
Submitted by:  Frahm, Holger 
Submitted to:  SciPost Physics 
Ontological classification  

Academic field:  Physics 
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Approach:  Theoretical 
Abstract
Using the properties of the local Boltzmann weights of integrable interactionroundaface (IRF or face) models we express local operators in terms of generalized transfer matrices. This allows for the derivation of discrete functional equations for the reduced density matrices in inhomogeneous generalizations of these models. We apply these equations to study the density matrices for IRF models of various solidonsolid type and quantum chains of nonAbelian $\bm{su(2)_3}$ or Fibonacci anyons. Similar as in the six vertex model we find that reduced density matrices for a sequence of consecutive sites can be 'factorized', i.e.\ expressed in terms of nearestneighbour correlators with coefficients which are independent of the model parameters. Explicit expressions are provided for correlation functions on up to three neighbouring sites.
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Reports on this Submission
Anonymous Report 3 on 202162 (Invited Report)
 Cite as: Anonymous, Report on arXiv:2104.06269v1, delivered 20210602, doi: 10.21468/SciPost.Report.3012
Strengths
First new and very interesting results on reduced density matrices of integrable face models and of their factorization properties
Weaknesses
On the presentation of the existing literature, on the notations and on the completeness of the steps in their proofs
Report
The manuscript starts the analysis of reduced density matrices of integrable face models with inhomogeneity parameters by deriving a discrete version of the quantum KnizhnikZamolodchikov type equation. The authors use this equation and some further unicity solution requirements to infer a factorized form for these correlation functions for (R)SOS models and a quantum chains of nonAbelian $su(2)_3$ Fibonacci anyons. This analysis produces explicit expressions of the reduced density matrices on two and three lattice sites.
The results are new and very interesting and they open the way to the generalization of the factorization properties of these correlation functions beyond those so far derived for the XXZ quantum spin chains. I recommend the publication of the paper in SciPost after the authors take cure of some improvements going from a more detailed presentation of the existing literature (in particular, on these correlation functions of related models) to a more detailed description of the used notations up to the clearness and completeness of the steps used in their proofs.
The two previous referees have done a very good job in identifying these improvements and their reports contain mainly the full list of required modifications and clarifications I have myself developed during the study of the manuscript. So, my advice is that the authors implement them. Let me just cite a couple of them that I would like to evidence. I agree with referee 1 on the fact that the large use of graphical notations (this also in the proofs) can result in a difficult access to a wide audience and the paper does not seem completely selfcontained in the explication of them. I share exactly the same impression of referee 2 that some steps in the proof are missing to consider their statements/results completely proven. One is the argument of the analytic prolongation which implies the unicity of the solution, they have a proof of this properties or they are making some well educated guess/conjecture? This is essential to prove the factorized form of these correlation functions.
A part from that, I found somehow misleading, in the framework of integrability, the use of the terminology “generalized transfer matrices” for the reconstruction of local operators. The transfer matrices of integrable models in general define the family of commuting operators while this is not the properties of local operators. The reconstructions here presented are rather the generators of the dynamical algebra dressed by true transfer matrices. At page 10 the sentence “For more complicated cases this expression needs to modified” should contain a missing “be”.
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Anonymous Report 2 on 2021523 (Invited Report)
 Cite as: Anonymous, Report on arXiv:2104.06269v1, delivered 20210523, doi: 10.21468/SciPost.Report.2955
Strengths
1.) Probably the first paper which touches the factorization of static correlation functions of the face models, so the paper may be opening up a new and interesting direction
Weaknesses
1.) Presentation of main results could be improved
2.) Discussion of the context could be improved
Report
The authors launch a study of reduced density matrices of integrable
face models. They express the reduced density matrices of the
inhomogeneous models as normalized expectation values of products of
monodromy operators, mimicking in a way the corresponding construction
for the vertex models. They show that the inhomogenous reduced density
matrices satisfy a discrete version of the rqKZ equation obtained
in [35,29]. This equation is then used to study the reduced density
matrices on two and three lattice sites for SOS and RSOS models and
also for a related model of nonAbelian anyons. As concrete results
the authors obtain the twosite reduced density matrix of the
SOS model for a vacuum state and relations for some of the
threesite reduced density matrices of two RSOS models (r = 4, 5)
with certain elements of the corresponding twosite density matrix.
The latter is then also upgraded to a special anyon model.
To my best knowlegde this is the first observation of a
factorization property of static correlation functions, that was
known for the XXZ chain (or the associated sixvertex model),
in a face model. This observation is quite interesting as there
have been speculations whether or not such a factorization
would be a general property of YangBaxter integrable models.
For this reason I recommend the publication of the paper in
SciPost.
Being the second referee I have the privilege of having read
the first referee report. Like the first referee I am not entirely
happy with the presentation of the results and with the way
the authors try to make connection with the existing literature.
As I read the first report I will refrain from futher commenting
on theorem 1. I also agree on his/her remarks on the graphical
notation.
In addition, I would like to comment on the factorization of
the correlation functions of the XXZ model and, in passing,
suggest to be more precise in certain statements and in making
reference to previous work.
In the first paragraph of the introduction the authors write
"$\dots$ a remarkable property of the reduced density matrices
has been found [6,7]: correlation functions of spins on N
consequtive sites can be expressed as sums of terms factorizing
into products of nearestneighbour (twopoint) functions of
the generalized model. Their coefficients are recursively
defined elementary functions of N spectral parameters and do not
depend on model parameters such as the system size or choice
of inhomogenities." Here two things are mixed. In fact the
factorization was explained in [6,7]. But these papers are
based on the qKZ (or rqKZ) equation which is only valid
for the infinite chain. Those times most of the protagonists
in the field believed that factorization was a "property of
the vacuum". Factorization at finite temperature (or finite
length) was first observed in the study of the threesite
reduced density matrix of the XXX chain in the works
[R1] Factorization of multiple integrals representing the
density matrix of a finite segment of the Heisenberg spin chain,
H. E. Boos et al., J. Stat. Mech. 0604: P04001, 2006
[R2] Density matrices for finite segments of Heisenberg chains
of arbitrary length, J. Damerau et al., J. Phys. A 40 (2007) 4439
Those days these works were a surprise to many people.
The factorization in the most general case of generalized
density matrices of the XXZ chain was then proven in the works
[R3] Hidden Grassmann Structure in the XXZ Model II: Creation
Operators, H. Boos et al., Commun. Math. Phys. 286:
875, 2009
[R4] Hidden Grassmann Structure in the XXZ Model III: Introducing
Matsubara direction, M. Jimbo, T. Miwa and F. Smirnov,
J. Phys. A 42: 304018, 2009
The approach based on "discrete functional equation", [35,29]
came only later and offered an alternative proof of the
factorization. I think it would be rather helpful to the
readers if the original works would be mentioned and if
it would be explained which are the advantages and disadvantages
of the different methods.
In my understanding the situation is as follows. As compared
to the Fermionic basis approach the approach using the
discrete functional equations is much easier to generalize.
One has to be careful though, as the functional equation
approach of [35,29] requires, in my understanding, several
more steps which are missing in the present paper. In [29]
it was shown, that the discrete functional equations of
rqKZ type when supplied with an asymptotic reduction, obtained
by sending one of the spectral parameters to infinity, have
a unique solution. Then the solution of the usual
rqKZ equation [7] was plugged in and was shown to solve
the functional equation und the asymptotic reduction. This
provided an alternative proof of the factorization. However,
this proof was not constructive. It required the preknowledge
of the solution.
In the present work the authors claim in the first paragraph
of the conclusions that the "discrete functional equation"
[$\dots$] "determine the functional dependence of $D_N$ on
these spectral parameter. Given the analytical properties
inherited from the Boltzmann weights of the model considered
these equations have a unique solution for any transfer matrix
eigenstate." I am not sure what they want to say here.
As far as I understand it, there is no proof of this statement
in the paper and no refererence. Is this a conjecture? I think
the statement cannot be true without further requirements
like asymptotic conditions. A proof of such a statement for
the Heisenberg model is given in [29]. Do the authors claim
that a similar proof holds for the face models? They should
be more specific here.
As I said above, in my understanding the uniqueness of the
solutions of the discrete functional equations if supplied
with appropriate asymptotic conditions is essential for the
proof of the factorization of the correlation functions in
[29]. Another ingredient of the proof is the Ansatz, taken
from [7], for the factorized form of the reduced density matrix.
This includes, in particular, knowledge of the number of
unknown functions. The authors observe that `in certain
topological sectors' the answer requires a single function.
How many are there in general? Is it known or is there a
conjecture?
So far, in case of the XXZ model, an advantage of the Fermionic
basis approach over the approach using discrete functional
equations is that it characterizes these unknown functions,
which are onepoint and twopoint functions that constitute
the beginning of the recursion. In the paper this concerns
the function $f(\lambda, \mu)$. In the Fermionic basis
approach there are two functions $\rho$ and $\omega$ which
were characterized by means of integral formula and difference
equations in [R4] and in terms of solutions of nonlinear
integral equations in the work
[R5] On the physical part of the factorized correlation
functions of the XXZ chain, H. Boos and F. Göhmann,
J. Phys. A 42: 315001, 2009
Equation (67) of [R5] shows that the functions $\omega$,
expressed by means of solutions of nonlinear integral
equations satisfies a basic discrete functional equation.
In the approach of [29] this was used as an input. Such
an input as well as the general form of the solution,
taking from [7] in case of the XXX chain, seems to be
still missing in the context of the face models. I think
it would be helpful if the authors could be more precise
here. They do obtain the function $g(\lambda, \mu)$ in
section 5.1 for a very special case of the density matrix
build from a vacuum state. It would be helpful if the
authors could comment on the possibilities to calculate
e.g. the function $f(\lambda, \mu)$ in (5.2).
What is also a pity for the curious readers is that the
authors say in the introduction that they "propose
an algorithm for the efficient computation of the
structure coefficient", but this algorithm is only
vaguely described in the body of the paper, such that it
would probably be hard for the readers to reproduce e.g.
equation (5.33). Again it would be helpful if the authors
could be more precise.
In the last sentence of their conclusions the authors
bring up the interesting question whether factorization is
peculiar of the XXZ model and related models or rather
a general property of integrable models. Here it could
be mentioned that discrete functional equations of the
type considered in the paper are know in a rather general
context of quantumgroup related vertex models,
[R6] Reduced qKZ equation: general case, A. Klümper,
Kh. Nirov, A. Razumov, J. Phys. A 53: 015202, 2020
but an algorithm for connecting, say, the threesite functions
with the twosite functions, as proposed by the authors,
is unknown in this general case. In fact, I would expect
that the equations proposed in [R6] do not uniquely fix the structure
of the correlation functions.
Requested changes
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Anonymous Report 1 on 2021517 (Invited Report)
 Cite as: Anonymous, Report on arXiv:2104.06269v1, delivered 20210517, doi: 10.21468/SciPost.Report.2906
Report
In this work, the authors study integrable face models (sometimes called IRF or SOS models) with inhomogeneity parameters and derive some discrete functional equations for their reduced density matrices. These discrete equations may be considered as some finitesize analog of the qKZ equations. Similar equations have already been obtained in the literature for temperature correlation functions in the Heisenberg spin chain. The derivation of these equations rely on basic algebraic properties satisfied by the Boltzmann weights of model, such as the YangBaxter equation, the unitarity condition, the crossing symmetry and the initial condition. In a last part of the paper, the functional equation is used to explicitly compute the density matrix elements on 2 or 3 sites in some particular examples: the critical CSOS model, the critical RSOS model, and a model of Fibonacci anyons.
I find this work interesting and a priori suitable for publications in SciPost Physics. However, I have several remarks or questions.
1) References to previous works in not always accurate and sometimes confused in the introduction:
 On page 2, it is written: “while the corresponding modified (dynamical) YangBaxter algebra allows for a solution of the spectral problem by means of an algebraic Bethe ansatz [11] or in the framework of Sklyanin’s Separation of Variables [12, 13] this modification does, however, pose a problem for the computation of physical quantities such as correlation functions. One reason is the lack of a onetoone mapping between height configurations in the SOS formulation and spin configurations in the dynamical sixvertex model which may lead to boundary contributions to certain expectation values even in the thermodynamic limit [14]. "
I find this sentence extremely confusing. Correlation functions for SOS models where for instance computed in:
[R1] S. Lukyanov and Y. Pugai, Multipoint local height probabilities in the integrable RSOS model, Nucl. Phys. B 473 (1996), 631–658.
[R2] D. LevyBencheton and V. Terras, Multipoint local height probabilities of the CSOS model within the algebraic Bethe ansatz framework, J. Stat. Mech. (2014) P04014.
I don’t see in these two works any problem with a "lack of a onetoone mapping between height configurations in the SOS formulation and spin configurations in the dynamical sixvertex model". In fact, the two formulations are in my understanding completely equivalent. Maybe the authors refer to the correspondence introduced by Baxter with the eightvertex model, which is in fact not a onetoone mapping (and is indeed a problem for the computation of correlation functions of the eightvertex model itself, but not for those of the SOS model)? Or maybe they refer to the fact that the particular restriction of generic SOS models into RSOS model, for which the height are chosen in a finite set, may lead to some difficulties in the writing of some ABA solution of the model? But even in that case other approaches to correlation functions are possible, as in [R1], and the difficulty is not particularly linked to a rewriting or not of the algebra in the Felder and Varchenko [11] (i.e. dynamical) way. Hence, this sentence should be modified and clarified, and the two above works [R1] and [R2] about the computation of correlation functions in such models should be added here. One have indeed the wrong impression when reading the introduction that nothing has been done so far concerning the computation of correlation functions of SOS models.
By the way, in the aforementioned sentence, whether [11] refers to the ABA solution of the SOS models relying on the dynamical YangBaxter algebra, [12,13] do not refer at all to SOS models! The Separation of Variables solution of such models have been done in
[R3] G. Niccoli, An antiperiodic dynamical sixvertex model: I. Complete spectrum by SOV, matrix elements of the identity on separate states and connections to the periodic eightvertex model, J. Phys. A: Math. Theor. 46 (2013), 075003
and in Reference [19] of the present paper. The two references [R3] and [19] should be cited here.
 In the next sentence, it is written “the inverse problem relating local observables to elements of the YangBaxter algebra [16,17], have been obtained only for the particular cases of the cyclic (CSOS) and the antiperiodic SOS models such that multipoint height probabilities could be calculated [18, 19]". In this sentence is mixed at the same level two different things: a particular restriction of the model (CSOS), and a particular choice of boundary conditions for the general SOS model. However, the solution of the inverse problem of [18] (formulated there for periodic boundary conditions) is not particularly specific to CSOS models since it uses only basic properties of the Rmatrix of the model which are strictly equivalent to (2.12)(2.15) of the present paper (as far as I understand, the range of values of the heights play no role there). As a matter of fact, it was directly generalized in [19] to any twisted boundary conditions (and not only antiperiodic), where there a completely general SOS model is considered. So the solution of the inverse problem obtained in [18,19] seems to me not less general as the one obtained in the present paper. This sentence should therefore be modified.
 The next sentence, "we address some of the issues appearing in the calculation of correlation functions in generic face models in particular on finite lattices while avoiding the use of the correspondence to a dynamical vertex model", is also confusing. As already mentioned above, I do not understand what the authors mean by a “correspondence” with a dynamical vertex model at this stage. Do they speak about the vertexIRF correspondence? But this usually means the correspondence introduced by Baxter to study the eightvertex model from SOS, which is of course not relevant here. Or do they mean the reformulation of the Boltzmann weights of the SOS model as the elements of some Rmatrix solution of a dynamical YangBaxter equation, as in Felder’s works? But this is purely formal to underline the algebra behind the model, and cannot be called “correspondence”: at the level of the present paper it is just a question of choice of notations. Once again, the authors should clarify what they mean here and modify the sentence accordingly.
2) Notations and definitions could sometimes be improved:
 On equation (2.1), what does it mean to have a definition with “may be” and “may not be”? In a definition, one should use “are” or “are not”.
 What does it mean to “read from topleft to bottomright” on a graphic like at the top page 4? Please clarify.
 There seems to be a mixing of notations where indices or subscripts represent the fact that the operator is “sandwiched” between states, as in (2.7), or where the subscripts or indices seem to represent only the corner values, as in (2.10). I find it not completely clear. Can the authors be more explicit when defining (2.10)?
 Many crucial formulas are written only graphically. I find this not completely clear, especially when appears “turned squares” without explanations, considering that the identification of the upper left corner is important for the value of the Boltzmann weight. Although this type of representations is quite standard in the literature, I think it is important, for the article to be selfcontained and easier to read, to have clear definitions without need to refer to previous papers to understand them. Can the authors write, for clarity, the explicit analytical form of the formulas (2.12), (2.13), (2.14), (2.15) and (4.1) in addition to the graphical one?
3) About the solution of the ‘inverse problem’ on p.78:
 As mentioned above, the solution of the inverse problem of [18] seems to me as general as the one proposed in this section. But probably to consider the local operator (2.11) one has to combine the results of [18] with the local weights considered in [R2]. Maybe the authors could comment about this and on how their result could be related to the ones of [18][R2]? They should of course also modify the sentence “A first step towards the solution of the inverse problem for face models has been achieved in Ref. [18] for the cyclic solidonsolid (CSOS) model which can be related to the eightvertex model by considering a dynamical version of the YangBaxter equation [11, 26, 27]" accordingly.
 Would it be possible to have a general proof of the result, with details for L>2 to see explicitly how the dressing of transfer matrices appear in the result?
4) About the applications of the functional equation:
 Is there a reason for which the authors restrict their study to critical models? Is the functional equation too complicated to solve in the general case where the Boltzmann weights explicitly depend on the height variable?
 The discrete functional equation obtained in [29] in temperature XXZ case was used there to show that the solution could be stated in terms of a single nearest neighbor correlator ω. The authors of the present paper observe a similar behavior in some topological sector of the RSOS model. However, in the CSOS case, they limit their study to the case N=2 and do not discuss this question. Is it because this property does not hold in that case? It would be nice that the authors comment about this since they conclude the paper by the sentence “this may well allow to shed some light on the question whether the factorization of correlation functions is a general property of integrable models which extends beyond RSOS models and spin1/2 chains".
Requested changes
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