SciPost Submission Page
A free fermions in disguise model with claws
by Kohei Fukai, István Vona, Balázs Pozsgay
Submission summary
| Authors (as registered SciPost users): | Kouhei Fukai |
| Submission information | |
|---|---|
| Preprint Link: | scipost_202510_00039v1 (pdf) |
| Date submitted: | Oct. 22, 2025, 8:14 p.m. |
| Submitted by: | Kouhei Fukai |
| Submitted to: | SciPost Physics |
| Ontological classification | |
|---|---|
| Academic field: | Physics |
| Specialties: |
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| Approach: | Theoretical |
Abstract
Recently, several spin chain models have been discovered that admit solutions in terms of "free fermions in disguise." A graph-theoretical treatment of such models was also established, giving sufficient conditions for free fermionic solvability. These conditions involve a particular property of the so-called frustration graph of the Hamiltonian, namely that it must be claw-free. Additionally, one set of sufficient conditions also requires the absence of so-called even holes. In this paper, we present a model with disguised free fermions where the frustration graph contains both claws and even holes. Special relations between coupling constants ensure that the free fermionic property still holds. The transfer matrix of this model can be factorized in a special case, thereby proving the conjectured free fermionic nature of a special quantum circuit published recently by two of the present authors. This is the first example of free fermions in disguise with both claws and even holes simultaneously.
Author indications on fulfilling journal expectations
- Provide a novel and synergetic link between different research areas.
- Open a new pathway in an existing or a new research direction, with clear potential for multi-pronged follow-up work
- Detail a groundbreaking theoretical/experimental/computational discovery
- Present a breakthrough on a previously-identified and long-standing research stumbling block
Current status:
Reports on this Submission
Report #2 by Paul Fendley (Referee 2) on 2026-1-28 (Invited Report)
Report
The model in this paper by Fukai, Vona and Pozsgay likewise violates these graphical conditions. The authors clearly explain how to solve it, generalizing these methods again. This model is in a sense the simplest example of a ffd model violating the graphical conditions. This model requires adding no new degrees of freedom to the ffd model, so the Hamiltonian can be viewed as a deformation of the original one. The FP model, on the other hand, is in essence two copies of the original coupled in a specific way. Moreover, the authors provide a more general method, giving hope that the graph-theory construction can be extended to such ffd models.
For these reasons I believe the paper deserves publication in SciPost. It solves a novel model using a novel construction.
The authors do not, however, note the considerable similarities with the FP model and its solution. Indeed, the authors state that they believe theirs is the first ffd model with "even holes" in the frustration graph. That's not true; the FP model has them. Moreover, their construction relies on noticing that the operators comprising an even hole implements a gauge symmetry, and its effect can be removed by fixing the gauge. The FP has the same structure; it's just that the gauge fixing there is built in from the beginning.
This observation of gauge symmetry is interesting and definitely an extension of the work In the FP paper. It would be useful, however, to make this connection clearer.
Requested changes
1) As indicated in the report, the authors need to explain better the connection with the FP model, and remove the claim that this is the first ffd example with even holes.
2) It makes sense to first introduce the model and its frustration graph before embarking on the proof of its ffd behavior. The authors indeed do that in section 3. However, they should reword a little to make it clearer that they are summarizing the results here, and indicate better where in the paper they prove it. For example toward the end of section 3.4, they state that the graphs in Fig 8 are free fermion, but don't say how they know that. In the caption of Fig 8 they state that these graphs "can be proven" to be free fermionic, but again don't indicate where. Likewise, the relation 3.11 is rather mysterious as it stands; an indication of where and how it gets used would be useful.
3) In the paragraph beginning "Among the remaining couplings..." in sec 3.4, don't they mean equation 3.13, not 3.11? (The former follows from the latter.)
4) In the following paragraph, they say that finding currents makes a model free fermionic, but that's not quite right -- the currents (presumably) make the model integrable, but not necessarily free fermionic. An example is the original ffd model, which has such currents for periodic b.c., but is not free-fermionic.
Recommendation
Publish (easily meets expectations and criteria for this Journal; among top 50%)
Strengths
1- Clarity: this paper is very clear. The problem is clearly defined, the proofd are well organised. The notation is clear. The derivations are thoughtfully expressed.
2- Novelty: while this result (the existence of such a model, with a graphical recognition and decomposition) is not surprising, the simplicity of the expression in this model is surprising.
Weaknesses
Report
Requested changes
I believe I noticed a few spelling errors and turns of phrase that were slightly confusing but I do not request any substantive changes
Recommendation
Publish (easily meets expectations and criteria for this Journal; among top 50%)
