{"total":13,"items":[{"citing_arxiv_id":"2605.27870","ref_index":25,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Revisiting boundary electromagnetic duality and edge modes","primary_cat":"hep-th","submitted_at":"2026-05-27T02:38:39+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"In 4D Maxwell theory, standard Neumann/Dirichlet boundary conditions render large gauge transformations and edge mode shifts as gauge redundancies, while modified conditions make them physical symmetries generated by topological surface operators, with new electromagnetic dual boundary conditions co","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.19331","ref_index":72,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Locality in effective field theory for inflationary soft modes","primary_cat":"gr-qc","submitted_at":"2026-05-19T04:08:34+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"The authors define a locality condition for hard-mode states during inflation that unifies local effective dynamics for soft modes, suppression of loop corrections, generalized soft theorems, and absence of infrared divergences in observable correlators.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.05130","ref_index":6,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Subleading Chern-Simons soft factors in perturbative de Sitter","primary_cat":"hep-th","submitted_at":"2026-05-06T17:00:17+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Subleading Chern-Simons soft factors stay insensitive to perturbative 1/ℓ² de Sitter corrections, indicating topological universality at the amplitude level.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Goldberger,Scattering of low-energy photons by particles of spin 1/2, Phys. Rev.96(1954) 1433. [3] F.E. Low,Scattering of light of very low frequency by systems of spin 1/2,Phys. Rev.96(1954) 1428. [4] F.E. Low,Bremsstrahlung of very low-energy quanta in elementary particle collisions,Phys. Rev. 110(1958) 974. [5] S. Weinberg,Infrared photons and gravitons,Phys. Rev.140(1965) B516. [6] T. He, P. Mitra, A.P. Porfyriadis and A. Strominger,New Symmetries of Massless QED,JHEP 10(2014) 112 [1407.3789]. [7] M. Campiglia and A. Laddha,Subleading soft photons and large gauge transformations,JHEP 11(2016) 012 [1605.09677]. [8] D. Kapec, M. Pate and A. Strominger,New Symmetries of QED,Adv. Theor. Math. Phys.21 (2017) 1769 [1506.02906]. [9] V."},{"citing_arxiv_id":"2604.26016","ref_index":54,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"The Schrodinger Equation as a Gauge Theory","primary_cat":"hep-th","submitted_at":"2026-04-28T18:00:24+00:00","verdict":null,"verdict_confidence":null,"novelty_score":null,"formal_verification":null,"one_line_summary":null,"context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Fischer, \"Inherent nonlinearity of fluid motion and acoustic gravitational wave memory,\" Phys. Rev. D105, no.2, 022003 (2022) [arXiv:2011.05837 [gr-qc]]. [52] S. Weinberg, \"Infrared photons and gravitons,\" Phys. Rev.140, B516-B524 (1965) [53] A. Strominger, \"On BMS Invariance of Gravitational Scattering,\" JHEP07, 152 (2014) [arXiv:1312.2229 [hep-th]]. [54] T. He, P. Mitra, A. P. Porfyriadis and A. Strominger, \"New Symmetries of Massless QED,\" JHEP10, 112 (2014) [arXiv:1407.3789 [hep-th]]. [55] A. Strominger and A. Zhiboedov, \"Gravitational Memory, BMS Supertranslations and Soft Theorems,\" JHEP01, 086 (2016) [arXiv:1411.5745 [hep-th]]. [56] A. Tolish and R. M. Wald, \"Retarded Fields of Null Particles and the Memory Effect,\""},{"citing_arxiv_id":"2604.11602","ref_index":33,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Celestial 1-form symmetries","primary_cat":"hep-th","submitted_at":"2026-04-13T15:11:07+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"In self-dual Yang-Mills the S-algebra becomes an algebra of 1-form symmetries whose 2-form currents link integrability to the equality of Carrollian corner charges and celestial chiral algebra modes.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Expanding this aroundq= 0 to extractτ s, we obtain the conserved 2-forms JsdM τ=ϵ = ∞X s=0 vs s! ∂s zϵ(z)Bs .(5.8) As we have seen, these currents owe their existence to the integrability and hierarchies of the self-dual theory which underlie the construction ofB s. At this stage, we are ready to relate these to the leading soft photon asymptotic symmetries of sd Maxwell theory [33]. If we restrict (5.8) to, say, future null infinity v→0 +, we obtain lim v→0+ JsdM τ=ϵ =ϵ(z)B I + .(5.9) Integrating this over a light cone cutS 2 u of fixeduonI +, we get the conserved charges Qϵ = Z S2u ϵ(z)B .(5.10) This makes contact with the recent investigations [10, 11] of the connections between asymptotic and 1-form symmetries in electromagnetism."},{"citing_arxiv_id":"2604.06088","ref_index":11,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Comments on Symmetry Operators, Asymptotic Charges and Soft Theorems","primary_cat":"hep-th","submitted_at":"2026-04-07T17:02:25+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"1-form symmetries in the QED soft sector generate asymptotic charges whose central extension implies soft photon theorems and fixes a two-soft-photon contact term.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Ciafaloni, and G. Marchesini, \"Jet Structure and Infrared Sensitive Quantities in Perturbative QCD,\"Phys. Rept.100(1983) 201-272. [9] F. A. Berends and W. T. Giele, \"Multiple Soft Gluon Radiation in Parton Processes,\"Nucl. Phys. B313(1989) 595-633. [10] A. Strominger, \"Asymptotic Symmetries of Yang-Mills Theory,\"JHEP07(2014) 151,arXiv:1308.0589 [hep-th]. [11] T. He, P. Mitra, A. P. Porfyriadis, and A. Strominger, \"New Symmetries of Massless QED,\"JHEP10(2014) 112,arXiv:1407.3789 [hep-th]. [12] M. Campiglia and A. Laddha, \"Asymptotic symmetries of QED and Weinberg's soft photon theorem,\"JHEP07(2015) 115,arXiv:1505.05346 [hep-th]. [13] D. Kapec, M. Pate, and A. Strominger, \"New Symmetries of QED,\"Adv. Theor."},{"citing_arxiv_id":"2601.23019","ref_index":44,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Toward claiming a detection of gravitational memory","primary_cat":"gr-qc","submitted_at":"2026-01-30T14:27:25+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"A framework using scale separation in the Isaacson description defines observable gravitational memory rise for compact binary coalescences, providing a basis for hypothesis testing in LISA data.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Lasky, and E. Thrane, \"Measuring gravitational-wave memory in the first LIGO/Virgo gravitational-wave transient catalog,\" Phys. Rev. D101no. 2, (2020) 023011, arXiv:1911.12496 [astro-ph.HE]. [43] K. Islo, J. Simon, S. Burke-Spolaor, and X. Siemens, \"Prospects for Memory Detection with Low-Frequency Gravitational Wave Detectors,\"arXiv:1906.11936 [astro-ph.HE]. [44]NANOGravCollaboration, K. Aggarwalet al., \"The NANOGrav 11 yr Data Set: Limits on Gravitational Wave Memory,\"Astrophys. J.889(2020) 38, arXiv:1911.08488 [astro-ph.HE]. [45] L. M. Burko and G. Khanna, \"Climbing up the memory staircase: Equatorial zoom-whirl orbits,\" Phys. Rev. D102no. 8, (2020) 084035, arXiv:2007.12545 [gr-qc]. [46] O. M. Boersma, D."},{"citing_arxiv_id":"2512.09018","ref_index":7,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"From Asymptotically Flat Gravity to Finite Causal Diamonds","primary_cat":"hep-th","submitted_at":"2025-12-09T19:00:00+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"The soft sector phase space of asymptotically flat gravity equals the phase space of radial size fluctuations of a finite causal diamond in flat spacetime.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2511.02363","ref_index":8,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Testing Electromagnetic Memory via Acceleration-Induced Phase Imprints in Superconductors","primary_cat":"hep-ph","submitted_at":"2025-11-04T08:40:35+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Proposes a superconducting readout protocol that uses acceleration-induced electric fields in conductors to imprint and detect electromagnetic memory phase shifts.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2509.04974","ref_index":24,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Minkowski Space holography and Radon transform","primary_cat":"hep-th","submitted_at":"2025-09-05T09:57:09+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Relates free scalar in Minkowski space to codimension-two sphere field via Radon transform to dS/EAdS slice and bulk reconstruction, with Mellin modes as generalized hypergeometric functions via Lee-Pomeransky method.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2509.02542","ref_index":13,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Soft Theorems in Chern-Simons Matter Theories","primary_cat":"hep-th","submitted_at":"2025-09-02T17:44:01+00:00","verdict":null,"verdict_confidence":null,"novelty_score":null,"formal_verification":null,"one_line_summary":null,"context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2504.12521","ref_index":129,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Lectures on the Bondi--Metzner--Sachs group and related topics in infrared physics","primary_cat":"gr-qc","submitted_at":"2025-04-16T22:47:28+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Lecture notes that build the BMS group from prerequisites to applications in soft theorems, memory effects, and new material on asymptotic conformal Killing horizons.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"This is imposed by the IR structure of GR and required for the scattering probability to be non-vanishing. The natural question at this point is: what does this have to do with the BMS group? Despite both the Weinberg soft theorem and the BMS group being discovered in the 1960's, the relation between them would only become clear in the 2010's. He et al.[129] and Strominger [217] noticed that the Weinberg soft graviton theorem is actually a consequence of BMS invariance of gravitational scattering. More specifically, the Weinberg soft graviton theorem is equivalent to the Ward identity (6.16), as we shall show. The upshot is that the Weinberg soft graviton theorem and the supertranslations in the BMS group are two related aspects of the IR structure of GR."},{"citing_arxiv_id":"2501.07136","ref_index":36,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"On symmetries of gravitational on-shell boundary action at null infinity","primary_cat":"hep-th","submitted_at":"2025-01-13T08:53:58+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Fixing null-infinity boundary action ambiguities via 5-point amplitude constraints yields subleading soft theorems and proposes generalized Geroch-tensor Goldstone modes for sub^n-leading soft graviton insertions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}