{"total":19,"items":[{"citing_arxiv_id":"2606.29323","ref_index":24,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"$BMS_3$-like algebras via the $Z_N$-graded $u(1)^2$ Kac-Moody algebra","primary_cat":"hep-th","submitted_at":"2026-06-28T10:31:10+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Compactification of the non-compact algebraic varieties of Z_N-graded Sugawara constructions on u(1)^2 Kac-Moody yields BMS3-like algebras Vir ⋊ F with F nilpotent of depth r < N for N>2, with depth tied to singularity order.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.28967","ref_index":50,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"On analytic solution of the Maxwell's equation with non-zero currents","primary_cat":"math.AP","submitted_at":"2026-06-27T15:08:48+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"An algorithm and analytic solutions are derived for Maxwell's equations with non-zero currents under Ohm's law, generalized Ohm's law with Hall effect, and added local fields, with an application to parallel waves.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.28219","ref_index":1,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Higher dimensional quantum Hall effect and the analog of $W_\\infty$-algebra","primary_cat":"hep-th","submitted_at":"2026-06-26T16:10:35+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Gauge transformations are shown to be the analog of W_infinity transformations for higher-dimensional quantum Hall effect, with their extended algebra and commutator anomaly derived via topological descent and bulk-boundary cancellation.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.19403","ref_index":41,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Emergent Gauge Symmetries in Particle Physics and Cosmology","primary_cat":"hep-ph","submitted_at":"2026-06-17T11:37:59+00:00","verdict":"UNVERDICTED","verdict_confidence":"MODERATE","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Gauge symmetries of the Standard Model are suggested to be emergent, with an emergence scale of about 10^16 GeV making dark energy density similar in magnitude to light Majorana neutrino masses.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.17248","ref_index":14,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Spin effects in the particle current of Bose-Einstein condensates in synthetic gauge fields","primary_cat":"cond-mat.quant-gas","submitted_at":"2026-06-15T19:48:41+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Spin term in particle current of pseudospin-1/2 BECs in synthetic gauge fields is required for classical drift velocity matching in non-interacting ground states and decreases relative to orbital current with increasing interactions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.12367","ref_index":38,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Nonadditivity in Quantum Field Theory: Replica Energies, Scaling Filters, and the Renormalization Group","primary_cat":"hep-th","submitted_at":"2026-06-10T17:34:37+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Replica energy and associated differential filters isolate nonadditive contributions in QFT partition functions, yielding universal data such as central charge, sphere free energy F, and defect entropies.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.09201","ref_index":9,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Order parameters and ground-state phase diagram of the interacting topological Su-Schrieffer-Heeger model with extended-range hoppings","primary_cat":"cond-mat.str-el","submitted_at":"2026-06-08T08:33:11+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Derives order parameters and constructs the ground-state phase diagram for the interacting SSH model with extended hoppings, revealing multiple topological, SC-like, and CDW phases verified via large-system simulations.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.08868","ref_index":55,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Topological invariant responsible for the integer QHE and non-commutative geometry","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-06-07T22:47:29+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Expresses the integer QHE topological invariant N3 as a K-theory and cyclic cohomology pairing via the Wigner-transformed Matsubara Green function in 2D tight-binding models.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.05496","ref_index":43,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Ideal Quantum Geometry for Fractional Chern Insulators","primary_cat":"cond-mat.str-el","submitted_at":"2026-06-03T22:38:57+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"A survey of ideal Bloch bands saturating quantum geometric bounds and their link to the lowest Landau level for fractionalized phases.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.03932","ref_index":59,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Emergent Hall viscosity in the integer quantum Hall phases of graphene-like systems","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-06-02T17:22:59+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Emergent Hall viscosity for integer quantum Hall phases in graphene is derived as a sum of geometric and electronic terms that depends on two topological invariants obtained via Green function Wigner-Weyl calculus.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.02391","ref_index":136,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Boulder Lectures on Thermal Dynamics and Hydrodynamic EFTs","primary_cat":"hep-th","submitted_at":"2026-06-01T15:41:41+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"Lectures summarizing the construction of hydrodynamic EFTs through strong-to-weak symmetry breaking, with examples from spin chains to relativistic QFTs and UV/IR constraints on transport coefficients.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.10329","ref_index":15,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Partial Quantisation of Non-Hermitian Berry Phases in Time-Varying Media","primary_cat":"physics.optics","submitted_at":"2026-05-11T10:32:08+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Non-Hermitian Berry phases in time-varying media have a quantized real part due to symmetry, giving a topological index for systems including a non-Hermitian Su-Schrieffer-Heeger model.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"von Klitzing, Developments in the quantum hall effect, Philos. Trans. A Math. Phys. Eng. Sci.363, 2203 (2005). [13] D. Tong, Lectures on the quantum hall effect (2016), arXiv:1606.06687 [hep-th]. [14] S. Moudgalya, B. A. Bernevig, and N. Regnault, Quan- tum many-body scars and hilbert space fragmentation: a review of exact results, Rep. Prog. Phys.85, 086501 (2022). [15] A. Chandran, T. Iadecola, V. Khemani, and R. Moessner, Quantum many-body scars: A quasiparticle perspective, Annu. Rev. Condens. Matter Phys.14(2023). [16] M. Testorf, Perturbation theory as a unified approach to describe diffractive optical elements, Journal of the Optical Society of America A16, 1115 (1999). [17] J. L. Remo, Second-order perturbation theory for"},{"citing_arxiv_id":"2604.10163","ref_index":41,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Hall transports from Taub-NUT AdS black holes","primary_cat":"hep-th","submitted_at":"2026-04-11T11:20:16+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Taub-NUT AdS black holes yield finite Hall transport coefficients originating from frame-dragging effects in holographic calculations.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"We perform our analysis in both low and high temperature regimes. •In Section 6, we finally conclude our discussion with some interesting future projects. 2 A quick review of Ohmic and Hall Conduc- tivities In this Section, we provide a brief review of the transport properties in QFT, in particular, focusing on the definitions of Ohmic and Hall conductivities [41]. Trans- port properties describe how a system responds to an external electromagnetic field. When both electric and magnetic fields are present, the induced current (J i) can be expressed in terms of the conductivity tensor (σ ij) as follows:J i =σ ijEj. 3 For an isotropic system, the conductivity tensor [4] can be described as σij = \u0012 σxx σxy −σxy σxx"},{"citing_arxiv_id":"2604.05889","ref_index":4,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Edge modes in Chern-Simons theory on a strip","primary_cat":"hep-th","submitted_at":"2026-04-07T13:51:48+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Chern-Simons theory on a strip yields boundary current algebras for oppositely propagating chiral bosons whose velocities follow from a bulk-boundary consistency condition and are independent of strip width.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"From a field-theoretic viewpoint, finite-width geometries with disconnected boundaries, such as a strip, provide the simplest setting to study how locality and boundary conditions de- termine the boundary dynamics of a gauge theory in the presence of two edges. In such setups, the prevailing expectation is that counter-propagating chiral modes appear at opposite boundaries [4, 9]. This expectation is supported both by semiclassical intuition (e.g. skipping orbits) and by effective field theory descriptions of annulus and multi-edge geometries [10]. However, in most anal- yses the boundary conditions (BC) are either fixed in a phenomenological way or the discussion effectively reduces to a single boundary. To the best of our knowledge, a fully explicit derivation"},{"citing_arxiv_id":"2512.10870","ref_index":34,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Structure of Chern-Simons Graviton Scattering Amplitudes from Topological Graviton Equivalence Theorem and Double Copy","primary_cat":"hep-th","submitted_at":"2025-12-11T18:01:18+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Establishes the Topological Graviton Equivalence Theorem to prove large energy cancellations in N-point massive graviton amplitudes and constructs three- and four-point amplitudes via double copy from topologically massive Yang-Mills.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2501.17927","ref_index":143,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Engineering of Anyons on M5-Probes via Flux Quantization","primary_cat":"hep-th","submitted_at":"2025-01-29T19:00:04+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Flux quantization of the M5-brane tensor field in twisted Cohomotopy yields Pontrjagin homology observables that reproduce abelian Chern-Simons theory and braid actions on defect anyons.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"However this can only be a local description on a single chart (as is common for Lan- grangian field theories): Neither J nor F may admit global coboundaries a and A, respectively. Instead, both must be subjected to some kind of flux-quantization. For F this must be classical Dirac charge quantization, which however is incompatible with integrality of J when k ̸= 1 (cf. [153, p. 35][143, p 159]). But without this, the implications break concerning topological order from abelian CS theory (ground state degeneracy, modular functoriality, ...). Therefore we must ask: Question: Is there a non-Lagrangian theory for quasi-particles of properly flux-quantized FQH systems? Answer: Yes!: The main result to be discussed here is that the key features of the anyonic topological order as seen in fractional"},{"citing_arxiv_id":"2410.20835","ref_index":265,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Non-identical anyon algebras from compact-field quantum geometry","primary_cat":"quant-ph","submitted_at":"2024-10-28T08:34:22+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Quantum geometry in lattice compact scalar fields induces pair-dependent Chern couplings that produce non-identical anyons.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2406.06212","ref_index":9,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Sub-Landau levels in two-dimensional electron system in magnetic field","primary_cat":"cond-mat.str-el","submitted_at":"2024-06-10T12:24:07+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Exact two-electron solutions in strong magnetic field organize into sub-Landau levels by relative angular momentum m, defining correlation subspaces that retain center-of-mass degeneracy and enable construction of pair-based many-body trial states.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2308.01980","ref_index":38,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Can Majorana zero modes in quantum Hall edges survive edge reconstruction?","primary_cat":"cond-mat.mes-hall","submitted_at":"2023-08-03T18:22:53+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Edge reconstruction of a ν=1 quantum Hall edge into a ν=1/3 side strip doubles topological sectors to Z2×Z2 degeneracy, producing 4π Josephson periodicity with energetically decoupled Z2 states.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}