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SymTFT construction of gapless exotic-foliated dual models

by Fabio Apruzzi, Francesco Bedogna, Salvo Mancani

Submission summary

Authors (as registered SciPost users): Salvatore Mancani
Submission information
Preprint Link: https://arxiv.org/abs/2504.11449v2  (pdf)
Date submitted: Aug. 5, 2025, 10:38 a.m.
Submitted by: Salvatore Mancani
Submitted to: SciPost Physics
Ontological classification
Academic field: Physics
Specialties:
  • Condensed Matter Physics - Theory
  • High-Energy Physics - Theory
Approach: Theoretical

Abstract

We construct Symmetry Topological Field Theories (SymTFTs) for continuous subsystem symmetries, which are inherently non-Lorentz-invariant. Our framework produces dual bulk descriptions -- gapped foliated and exotic SymTFTs -- that generate gapless boundary theories with spontaneous subsystem symmetry breaking via interval compactification. In analogy with the sandwich construction of SymTFT, we call this Mille-feuille. This is done by specifying gapped and symmetry-breaking boundary conditions. In this way we obtain the foliated dual realizations of various models, including the XY plaquette, XYZ cube, and $\phi$, $\hat{\phi}$ theories. This also captures self-duality symmetries as condensation defects and provides a systematic method for generating free theories that non-linearly realize subsystem symmetries.

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:
In refereeing

Reports on this Submission

Report #1 by Anonymous (Referee 1) on 2025-11-3 (Invited Report)

Report

The symmetry topological field theory (SymTFT) is an important tool to study dualities and symmetries. It has been generalized to describe the discrete subsystem symmetries and ordinary continuous symmetries. The authors extend this idea to construct SymTFT for continuous subsystem symmetries. Their focus is to reproduce gapless model with continuous subsystem symmetry, which is given by choosing gapped and symmetry-breaking boundary conditions of the SymTFT. They also discuss the duality between two formulations of the bulk SymTFT, using foliated field theory or exotic field theory, which is also a natural generalization from the discrete cases.

This work is a natural generalization in this field and will help the further study of gapless models, or spontaneous symmetry breaking phases, with subsystem symmetries. However, I hope the authors can clarify the following points in the requested changes.

Requested changes

The SymTFT gains its power at separating the symmetrical and dynamical data at different boundaries, and is universal for different models if the symmetry is given. In this paper the authors only studied one specific choice of boundary condition that is used to reproduce the models reviewed in section 3. This may diminish this article's significance and impact. Therefore, I hope the authors can address the following questions:

  1. Is it easy to study or classify different topological boundary conditions (e.g. Dirichlet or Neumann) using Mille-feuille method?
  2. What is the bulk operator that implement the change of boundary conditions? (Is it the condensation operator?)
  3. What is the dual models after changing a different boundary conditions?
  4. Usually the condensation operators obeys noninvertible fusion rules. What is the fusion rules in this case?
  5. Does the Mille-feuille method help us understand the UV-IR mixing related to subsystem symmetry? For example, after Eq (4.20), the authors claimed "For instance, we required scale invariance when constructing the physical boundary, not allowing for some terms that, due to UV/IR mixing, will contribute to the energy at leading order. As a consequence, the energy of our ground state is shifted. " Can you give the details of this?

At least, I hope the authors can clarify the questions in the example related to XY-plaquette models.

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