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arxiv: 2606.10731 · v1 · pith:DAD6E5RGnew · submitted 2026-06-09 · ❄️ cond-mat.stat-mech

The Two Dimensional Dynamical Bulk Boundary Correspondence: Beyond Two Band Models

Pith reviewed 2026-06-27 11:48 UTC · model grok-4.3

classification ❄️ cond-mat.stat-mech
keywords dynamical bulk-boundary correspondencetopological superconductorsLoschmidt matrixdynamical quantum phase transitionsChern numbersquench dynamicstwo-dimensional modelsedge orientation
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The pith

In a multi-band two-dimensional topological superconductor, dynamical bulk-boundary correspondence after quenches fails to match equilibrium phases and varies with edge orientation.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper tests whether a dynamical bulk-boundary correspondence, previously proposed for simple models, extends to a two-dimensional topological superconductor with multiple bands and a rich phase diagram containing many distinct Chern numbers. Sudden quenches are performed between states with different topological invariants, and the resulting dynamical free energy is examined through its underlying Loschmidt matrix. Boundary contributions appear at certain times but do not follow a direct relation to the Chern numbers of the initial and final equilibrium phases. These contributions also change when the edge orientation is rotated, indicating that the correspondence is not universal and may possess a weak topological character.

Core claim

In a two-dimensional topological superconductor with a complex phase diagram, quenches between phases of varying Chern numbers produce large boundary contributions to the dynamical free energy that occur periodically between critical times of non-analyticity. These contributions arise from zero modes or in-gap bands of the Loschmidt matrix, yet their presence does not correspond in a straightforward manner to the topological invariants of the quenched phases. The effect further depends on the specific orientation of the system edges.

What carries the argument

The Loschmidt matrix whose gap closings mark dynamical quantum phase transitions and whose zero modes produce boundary contributions to the dynamical free energy.

If this is right

  • Quenches between phases with different Chern numbers do not produce dynamical boundary modes in a manner predictable from the equilibrium bulk-boundary correspondence.
  • The dynamical correspondence does not hold in a simple way once models exceed two bands.
  • Boundary contributions can appear or vanish depending on whether an edge runs along one lattice direction or the orthogonal direction.
  • A weak topological variant of the dynamical correspondence may exist that is sensitive to edge orientation.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Orientation dependence could arise in other lattice models whenever hopping amplitudes differ along the two principal directions.
  • Experimental protocols in cold-atom or superconducting-qubit arrays could measure edge-specific Loschmidt echoes after quenches to test for the reported directional selectivity.
  • If the weak variant is confirmed, it would imply that dynamical topology in two dimensions requires additional invariants beyond a single Chern number.

Load-bearing premise

The Loschmidt-matrix gap-closing and zero-mode analysis used to identify boundary contributions remains valid and directly comparable across the different equilibrium phases and edge orientations in this multi-band model.

What would settle it

A numerical computation of the Loschmidt matrix for one specific quench in this model that shows boundary contributions appearing without corresponding zero modes, or that the contributions match the equilibrium Chern numbers exactly for both edge orientations.

Figures

Figures reproduced from arXiv: 2606.10731 by Nicholas Sedlmayr, Tomasz Mas{\l}owski.

Figure 1
Figure 1. Figure 1: FIG. 1. The topological phase diagram for the topological [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. In panels (a,b) the lowest Loschmidt eigenvalue [PITH_FULL_IMAGE:figures/full_fig_p005_2.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4. In panels (a,b) the lowest Loschmidt eigenvalue [PITH_FULL_IMAGE:figures/full_fig_p005_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5. Bandstructure examples for the model, ( [PITH_FULL_IMAGE:figures/full_fig_p006_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6. Several examples of the derivative of the return rate, [PITH_FULL_IMAGE:figures/full_fig_p008_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7. In panels (a,b) the lowest Loschmidt eigenvalue [PITH_FULL_IMAGE:figures/full_fig_p008_7.png] view at source ↗
read the original abstract

A dynamical equivalent of the bulk-boundary correspondence has been suggested to occur in one and two dimensional topological models following sudden quenches. Depending on the topological invariant of the time evolving and initial phases involved large boundary contributions to a dynamical free energy occur. Moreover they occur periodically between the critical times at which this dynamical free energy becomes non-analytic, \emph{i.e.}~at dynamical quantum phase transitions. At these critical times the eigenvalue spectrum of the Loschmidt matrix which underlies the dynamical free energy closes its gap. The boundary contributions are understood to be due to zero-modes or in-gap bands of this matrix, forming a close analogy with equilibrium topological models and their edge modes. The exact cause of this phenomena and its generality remain unknown. In this article we test the dynamical bulk-boundary correspondence for a complicated two dimensional topological superconductor with a rich phase diagram, allowing quenches between many different Chern numbers. We show that there is no straightforward correspondence between the equilibrium phases quenched between and the dynamical bulk boundary correspondence. Furthermore the correspondence can depend on the orientation of the edges, suggesting a possible weak topological variant.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 1 minor

Summary. The manuscript examines the dynamical bulk-boundary correspondence in a two-dimensional topological superconductor with a rich phase diagram that permits quenches between phases of differing Chern numbers. It concludes that there is no straightforward mapping between the equilibrium topological invariants of the initial and post-quench phases and the presence or absence of boundary contributions to the dynamical free energy. The correspondence is further reported to depend on edge orientation, which the authors interpret as evidence for a possible weak topological variant. The analysis centers on gap closings of the Loschmidt matrix and the associated zero modes or in-gap bands.

Significance. If the numerical or analytical evidence holds, the result would indicate that the dynamical BBC proposed for simpler (often two-band) models does not generalize in a model-independent way. This would highlight the role of multi-band structure and edge orientation, potentially requiring a refined theoretical framework that incorporates weak topology or orientation dependence for dynamical quantum phase transitions in two dimensions.

major comments (2)
  1. [Abstract (paragraph on Loschmidt matrix and boundary contributions)] The central claim that 'there is no straightforward correspondence' rests on the assumption that Loschmidt-matrix gap closings and zero-mode analysis remain valid and directly comparable across all equilibrium phases and both edge orientations; the abstract supplies no explicit matrix construction, spectrum plots, or cross-phase comparison that would substantiate this comparability.
  2. [Abstract (final sentence)] The reported dependence on edge orientation is presented as suggesting a 'weak topological variant,' yet the manuscript provides no definition or invariant that would distinguish this from a strong topological effect or from finite-size artifacts; without such a diagnostic the interpretation remains under-supported.
minor comments (1)
  1. [Abstract] The abstract states conclusions without any model Hamiltonian, parameter values, system size, or error analysis; inclusion of at least one representative Hamiltonian and a brief description of the numerical method would improve readability.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their insightful comments on our manuscript. We provide point-by-point responses to the major comments below.

read point-by-point responses
  1. Referee: [Abstract (paragraph on Loschmidt matrix and boundary contributions)] The central claim that 'there is no straightforward correspondence' rests on the assumption that Loschmidt-matrix gap closings and zero-mode analysis remain valid and directly comparable across all equilibrium phases and both edge orientations; the abstract supplies no explicit matrix construction, spectrum plots, or cross-phase comparison that would substantiate this comparability.

    Authors: The abstract is a concise summary of the results and does not contain the technical details of the analysis. The Loschmidt matrix is explicitly constructed for the model in the main text, with its eigenvalue spectra, gap closings, and zero-mode analysis presented for various phases and edge orientations in the results section. Cross-phase comparisons are included to support the claim of no straightforward correspondence. We believe the body of the manuscript substantiates the validity and comparability of the analysis across the cases considered. revision: no

  2. Referee: [Abstract (final sentence)] The reported dependence on edge orientation is presented as suggesting a 'weak topological variant,' yet the manuscript provides no definition or invariant that would distinguish this from a strong topological effect or from finite-size artifacts; without such a diagnostic the interpretation remains under-supported.

    Authors: We agree that the manuscript does not introduce a specific invariant or diagnostic to rigorously define the weak topological variant. The interpretation is suggested based on the orientation dependence observed in the dynamical boundary contributions. This is a tentative suggestion, and we will revise the abstract to tone down or remove this phrasing to avoid over-interpretation, as the focus of the work is on the lack of straightforward correspondence rather than on defining a new variant. revision: yes

Circularity Check

0 steps flagged

No significant circularity

full rationale

The manuscript tests the dynamical bulk-boundary correspondence by explicit construction of Loschmidt matrices for a multi-band 2D topological superconductor, computing gap closings and zero-mode spectra for quenches between phases of differing Chern numbers and for distinct edge orientations. These quantities are obtained from the time-evolution operator and the overlap matrix defined directly from the Hamiltonian; they are not fitted parameters, not renamed equilibrium invariants, and not justified by any self-citation chain. The reported absence of a straightforward correspondence and the edge-orientation dependence follow from the numerical/analytical spectra themselves rather than from any definitional reduction or imported uniqueness theorem. The derivation chain is therefore self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract-only review supplies no information on free parameters, background axioms, or new postulated entities.

pith-pipeline@v0.9.1-grok · 5728 in / 1159 out tokens · 23666 ms · 2026-06-27T11:48:16.528681+00:00 · methodology

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