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Taiwan","organization":"National Tsing-Hua University","country":{"code":"TW","name":"Taiwan"},"ror":"00zdnkx70"},{"value":"Physics Division, National Center for Theoretical Sciences, Taipei, 10617, Taiwan","organization":"Physics Division, National Center for Theoretical Sciences","country":{"code":"TW","name":"Taiwan"},"ror":"02mh1d616"},{"value":"Center for Theory-Computation-Data Science Research, National Tsing-Hua University, Hsinchu, 30013, Taiwan","organization":"National Tsing-Hua University","country":{"code":"TW","name":"Taiwan"},"ror":"00zdnkx70"}],"orcid":"0000-0002-4831-8638"},{"first_name":"Himanshu","last_name":"Parihar","name":"Himanshu Parihar","affiliations":[{"value":"Physics Division, National Center for Theoretical Sciences, Taipei, 10617, Taiwan","organization":"Physics Division, National Center for Theoretical Sciences","country":{"code":"TW","name":"Taiwan"},"ror":"02mh1d616"},{"value":"Department of Physics, College of Science, Kyung Hee University, Seoul, 02447, Republic of Korea","organization":"Kyung Hee University","country":{"code":"KR","name":"South Korea"},"ror":"01zqcg218"},{"value":"Center for Theory-Computation-Data Science Research, National Tsing-Hua University, Hsinchu, 30013, Taiwan","organization":"National Tsing-Hua University","country":{"code":"TW","name":"Taiwan"},"ror":"00zdnkx70"}],"orcid":"0000-0003-4060-3175"}],"publication_info":[{"journal_volume":"2026","journal_issue":"10","journal_title":"Journal of High Energy Physics","material":"article","page_start":"1","page_end":"23","artid":"JHEP10(2026)022","volume_year":"2026","journal_issue_date":null,"publisher":"Springer"}],"subtitle":"","related_materials":[],"abstract":"We study quantum transport phenomena induced by anisotropic Lifshitz scale anomaly in a boundary Lifshitz field theory (BLFT) coupled to an external electromagnetic background. In this context, we obtain the anisotropic scale anomaly in Lifshitz field theories coupled to a background U(1) gauge field and subsequently compute the anomaly induced near boundary current in a BLFT. Focusing on 5D BLFTs, we find that the temporal and spatial components of the induced current exhibit distinct power law dependencies on the distance from the boundary, reflecting the intrinsic time-space anisotropy of the theory. We further derive this anomalous current holographically from the bulk dual of BLFT and find that the temporal component is independent of the boundary conditions while the spatial component depends explicitly on them. The distance dependence is in exact agreement with the dual field theory result.","reception_date":null,"_created_at":"2026-10-03T12:55:33.799984","_updated_at":"2026-10-03T12:55:39.823129+00:00","publication_date":"2026-10-02","id":111682,"copyright":[{"statement":"","year":2026,"holder":"The Author(s)"}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)022/13130_2026_Article_30189.xml.scoap.xml","created":"2026-10-03T12:55:39.449336+00:00","updated":"2026-10-03T12:55:39.449347+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)022/13130_2026_Article_30189_a.pdf","created":"2026-10-03T12:55:39.455515+00:00","updated":"2026-10-03T12:55:39.455525+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/4.0/","name":"CC-BY-4.0"}],"article_arxiv_category":[{"category":"hep-th","primary":true}],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1007/JHEP10(2026)022"},{"identifier_type":"arXiv","identifier_value":"2602.06901"}]},{"first_online_date":null,"title":"Stodolsky effect in the framework of generalised neutrino interactions","acceptance_date":null,"doi":"10.1007/JHEP10(2026)024","countries":["IN"],"authors":[{"first_name":"Siddhartha","last_name":"Bandyopadhyay","name":"Siddhartha Bandyopadhyay","affiliations":[{"value":"Indian Institute of Technology Kanpur, Kalyanpur, Kanpur, Uttar Pradesh, 208016, India","organization":"Indian Institute of Technology Kanpur","country":{"code":"IN","name":"India"},"ror":"05pjsgx75"},{"value":"Department of Physical Sciences, Indian Institute of Science Education and Research Berhampur, Ganjam, Odisha, 760003, India","organization":"Indian Institute of Science Education and Research Berhampur","country":{"code":"IN","name":"India"},"ror":"023vrr657"}],"orcid":"0009-0002-3455-643X"},{"first_name":"Ujjal","last_name":"Dey","name":"Ujjal Dey","affiliations":[{"value":"Department of Physical Sciences, Indian Institute of Science Education and Research Berhampur, Ganjam, Odisha, 760003, India","organization":"Indian Institute of Science Education and Research Berhampur","country":{"code":"IN","name":"India"},"ror":"023vrr657"}],"orcid":"0000-0002-9620-7561"}],"publication_info":[{"journal_volume":"2026","journal_issue":"10","journal_title":"Journal of High Energy Physics","material":"article","page_start":"1","page_end":"28","artid":"JHEP10(2026)024","volume_year":"2026","journal_issue_date":null,"publisher":"Springer"}],"subtitle":"","related_materials":[],"abstract":"We study the Stodolsky effect utilizing the most general form of neutrino interactions with electrons below the electroweak scale by considering all possible Lorentz invariant operators respecting SU(3) ⨂ U(1) symmetry. We perform our calculation for both Dirac and Majorana neutrinos and find that in the most general setting, only the non-standard neutrino interactions and the tensor interaction terms provide a non-zero contribution, apart from the Standard Model contribution. We investigate the implications for the possible detection of the cosmic neutrino background (C$\\textit{ν}$B) by analysing the energy shifts that are characteristic of the Stodolsky effect. We also discuss the implication of considerable asymmetry in the C$\\textit{ν}$B on the present scenario.","reception_date":null,"_created_at":"2026-10-03T12:55:33.665965","_updated_at":"2026-10-03T12:55:39.813974+00:00","publication_date":"2026-10-02","id":111683,"copyright":[{"statement":"","year":2026,"holder":"The Author(s)"}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)024/13130_2026_Article_30191.xml.scoap.xml","created":"2026-10-03T12:55:39.519740+00:00","updated":"2026-10-03T12:55:39.519751+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)024/13130_2026_Article_30191_a.pdf","created":"2026-10-03T12:55:39.542742+00:00","updated":"2026-10-03T12:55:39.542754+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/4.0/","name":"CC-BY-4.0"}],"article_arxiv_category":[{"category":"hep-ph","primary":true},{"category":"astro-ph.CO","primary":false}],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1007/JHEP10(2026)024"},{"identifier_type":"arXiv","identifier_value":"2603.10114"}]},{"first_online_date":null,"title":"Discrete symmetries of Feynman integrals","acceptance_date":null,"doi":"10.1007/JHEP10(2026)031","countries":["DE"],"authors":[{"first_name":"Claude","last_name":"Duhr","name":"Claude Duhr","affiliations":[{"value":"Bethe Center for Theoretical Physics, Universität Bonn, Wegelerstraße 10, Bonn, D-53115, Germany","organization":"Universität Bonn","country":{"code":"DE","name":"Germany"},"ror":"041nas322"}],"orcid":"0000-0001-5820-3570"},{"first_name":"Sara","last_name":"Maggio","name":"Sara Maggio","affiliations":[{"value":"Bethe Center for Theoretical Physics, Universität Bonn, Wegelerstraße 10, Bonn, D-53115, Germany","organization":"Universität Bonn","country":{"code":"DE","name":"Germany"},"ror":"041nas322"}],"orcid":"0000-0002-5266-9449"},{"first_name":"Cathrin","last_name":"Semper","name":"Cathrin Semper","affiliations":[{"value":"Bethe Center for Theoretical Physics, Universität Bonn, Wegelerstraße 10, Bonn, D-53115, Germany","organization":"Universität Bonn","country":{"code":"DE","name":"Germany"},"ror":"041nas322"}],"orcid":"0009-0008-2948-9731"},{"first_name":"Sven","last_name":"Stawinski","name":"Sven Stawinski","affiliations":[{"value":"Bethe Center for Theoretical Physics, Universität Bonn, Wegelerstraße 10, Bonn, D-53115, Germany","organization":"Universität Bonn","country":{"code":"DE","name":"Germany"},"ror":"041nas322"}],"orcid":"0009-0007-3246-6357"}],"publication_info":[{"journal_volume":"2026","journal_issue":"10","journal_title":"Journal of High Energy Physics","material":"article","page_start":"1","page_end":"132","artid":"JHEP10(2026)031","volume_year":"2026","journal_issue_date":null,"publisher":"Springer"}],"subtitle":"","related_materials":[],"abstract":"We perform a comprehensive study of a certain class of discrete symmetries of families of Feynman integrals, defined as affine changes of variables that map different sectors of the family into each other. We show that these transformations are always encoded into permutations of the Feynman parameters that relate the Lee-Pomeransky polynomials of the two sectors, irrespective of the integral representation used to define the Feynman integrals. We then construct an affine map in loop-momentum space that encodes such a permutation. We also show that these symmetries can be naturally embedded into the framework of twisted cohomology theories, and the period and intersection parings are invariant under the symmetry transformations. If we focus on symmetries within a fixed sector, we obtain a group acting on the twisted cohomology group, and we study the decomposition of this action into irreducible representations. One of our main mathematical results is that the character of this representation is proportional to the Euler characteristic of the corresponding fixed-point set. We then study the implications for Feynman integrals, in particular for the intersection matrix in a canonical basis. We also present a formula for the number of master integrals in a given sector in the presence of a non-trivial symmetry group in terms of the Euler characteristics of fixed-point sets. As an application, we obtain the numbers of master integrals for banana integrals with up to four loops for arbitrary configurations of non-zero masses. In order to achieve our results, we had to combine tools from various different areas of mathematics, including graph theory, group theory and algebraic topology.","reception_date":null,"_created_at":"2026-10-03T12:55:33.796235","_updated_at":"2026-10-03T12:55:39.774460+00:00","publication_date":"2026-10-02","id":111681,"copyright":[{"statement":"","year":2026,"holder":"The Author(s)"}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)031/13130_2026_Article_30198.xml.scoap.xml","created":"2026-10-03T12:55:39.430573+00:00","updated":"2026-10-03T12:55:39.430584+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)031/13130_2026_Article_30198_a.pdf","created":"2026-10-03T12:55:39.440226+00:00","updated":"2026-10-03T12:55:39.440238+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/4.0/","name":"CC-BY-4.0"}],"article_arxiv_category":[{"category":"hep-th","primary":true},{"category":"math-ph","primary":false},{"category":"math.MP","primary":false}],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1007/JHEP10(2026)031"},{"identifier_type":"arXiv","identifier_value":"2604.08332"}]},{"first_online_date":null,"title":"Axion couplings in orbifold GUTs","acceptance_date":null,"doi":"10.1007/JHEP10(2026)032","countries":["CH","GB","US"],"authors":[{"first_name":"Prateek","last_name":"Agrawal","name":"Prateek Agrawal","affiliations":[{"value":"Rudolf Peierls Centre for Theoretical Physics, University of Oxford, Parks Road, Oxford, OX1 3PU, U.K.","organization":"University of Oxford","country":{"code":"GB","name":"United Kingdom"},"ror":"052gg0110"},{"value":"Department of Physics, University of California, Santa Barbara, CA, 93106, USA","organization":"University of California","country":{"code":"US","name":"United States"},"ror":"01spssf70"}],"orcid":"0000-0001-9947-0632"},{"first_name":"Michael","last_name":"Nee","name":"Michael Nee","affiliations":[{"value":"Department of Physics, Harvard University, Cambridge, MA, 02138, USA","organization":"Harvard University","country":{"code":"US","name":"United States"},"ror":"03vek6s52"}],"orcid":"0000-0003-1345-3941"},{"first_name":"Mario","last_name":"Reig","name":"Mario Reig","affiliations":[{"value":"Rudolf Peierls Centre for Theoretical Physics, University of Oxford, Parks Road, Oxford, OX1 3PU, U.K.","organization":"University of Oxford","country":{"code":"GB","name":"United Kingdom"},"ror":"052gg0110"},{"value":"Theoretical Physics Department, CERN, Geneva 23, 1211, Switzerland","organization":"Theoretical Physics Department, CERN","country":{"code":"CH","name":"Switzerland"},"ror":"01ggx4157"}],"orcid":"0000-0001-6815-5605"}],"publication_info":[{"journal_volume":"2026","journal_issue":"10","journal_title":"Journal of High Energy Physics","material":"article","page_start":"1","page_end":"25","artid":"JHEP10(2026)032","volume_year":"2026","journal_issue_date":null,"publisher":"Springer"}],"subtitle":"","related_materials":[],"abstract":"We consider the coupling of axions to gauge bosons in higher-dimensional Grand Unified Theories (GUT) inspired by string theory constructions with D-branes on orbifold singularities, the so-called orbifold GUTs. Due to their topological properties, axion couplings to gauge bosons are independent of the gauge symmetry reduction mechanism and the background geometry — they only depend on the embedding of the SM into the UV gauge group. There are two kinds of axions in this class of theories: axions coming from gauge fields in the bulk and axions localised on the boundaries. The axion-photon coupling for the bulk axions coincide with the results from 4-dimensional GUTs, where axions which couple to photons necessarily couple also to QCD. The brane-localised axions can couple to photons independently of the QCD coupling, but if gauge couplings are approximately unified, they have a much more severe quality problem. We show that in generic UV completions they are expected to get large masses from instantons on the boundaries. This means that the ratio $\\textit{g}$ /$\\textit{m}$ is below (or equal to) the QCD axion value for all axions in orbifold GUTs, as is the case for unified theories in 4d.","reception_date":null,"_created_at":"2026-10-03T12:55:33.618536","_updated_at":"2026-10-03T12:55:39.355615+00:00","publication_date":"2026-10-02","id":111677,"copyright":[{"statement":"","year":2026,"holder":"The Author(s)"}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)032/13130_2026_Article_30199.xml.scoap.xml","created":"2026-10-03T12:55:39.004141+00:00","updated":"2026-10-03T12:55:39.004156+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)032/13130_2026_Article_30199_a.pdf","created":"2026-10-03T12:55:39.030762+00:00","updated":"2026-10-03T12:55:39.030776+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/4.0/","name":"CC-BY-4.0"}],"article_arxiv_category":[{"category":"hep-ph","primary":true},{"category":"hep-th","primary":false}],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1007/JHEP10(2026)032"},{"identifier_type":"arXiv","identifier_value":"2511.21830"}]},{"first_online_date":null,"title":"When renormalisation remembers: UV/IR mixing as an entanglement bridge","acceptance_date":null,"doi":"10.1007/JHEP10(2026)025","countries":["GB"],"authors":[{"first_name":"Steven","last_name":"Abel","name":"Steven Abel","affiliations":[{"value":"Institute for Particle Physics Phenomenology and Department of Mathematical Sciences, Durham University, Durham, DH1 3LE, U.K.","organization":"Durham University","country":{"code":"GB","name":"United Kingdom"},"ror":"01v29qb04"}],"orcid":"0000-0003-1213-907X"}],"publication_info":[{"journal_volume":"2026","journal_issue":"10","journal_title":"Journal of High Energy Physics","material":"article","page_start":"1","page_end":"60","artid":"JHEP10(2026)025","volume_year":"2026","journal_issue_date":null,"publisher":"Springer"}],"subtitle":"","related_materials":[],"abstract":"Renormalisation is traditionally understood to be a Wilsonian memoryless process in which ultraviolet (UV) degrees of freedom gradually decouple, leaving an autonomous infrared (IR) description. However this need not be the case: in UV/IR mixed theories correlations between widely separated scales can persist. In this work I recast UV/IR mixing as a Hilbert-space phenomenon, realised as correlations across renormalisation scales. This formulation is implemented using the Born-Reciprocal Tensor Network (BRTN), a new configuration of tensor network that is globally symmetric under phase-space reciprocity. On this network I prepare the vacuum and reproduce the expected radiative corrections. The resulting renormalisation geometry exhibits memory, with a bridge linking reciprocal representations of IR physics, whose cross-bridge entanglement provides a precise criterion for the viability of an effective description. I analyse when this criterion is met, and show that there is a large-volume limit, with the fundamental scale held fixed, in which the obstruction to a local description dilutes: Wilsonian behaviour is restored and renormalisation forgets. The BRTN therefore provides a concrete and calculable platform for UV/IR mixing.","reception_date":null,"_created_at":"2026-10-03T12:55:33.554239","_updated_at":"2026-10-03T12:55:39.312236+00:00","publication_date":"2026-10-02","id":111678,"copyright":[{"statement":"","year":2026,"holder":"The Author(s)"}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)025/13130_2026_Article_30192.xml.scoap.xml","created":"2026-10-03T12:55:39.034137+00:00","updated":"2026-10-03T12:55:39.034147+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)025/13130_2026_Article_30192_a.pdf","created":"2026-10-03T12:55:39.089993+00:00","updated":"2026-10-03T12:55:39.090012+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/4.0/","name":"CC-BY-4.0"}],"article_arxiv_category":[{"category":"hep-th","primary":true},{"category":"hep-ph","primary":false},{"category":"quant-ph","primary":false}],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1007/JHEP10(2026)025"},{"identifier_type":"arXiv","identifier_value":"2606.17147"}]},{"first_online_date":null,"title":"Constraining the swift memory burden effect with GW250114-like events","acceptance_date":null,"doi":"10.1007/JHEP10(2026)034","countries":["PT"],"authors":[{"first_name":"Chen","last_name":"Yuan","name":"Chen Yuan","affiliations":[{"value":"CENTRA, Departamento de Física, Instituto Superior Técnico — IST, Universidade de Lisboa — UL, Avenida Rovisco Pais 1, Lisboa, 1049-001, Portugal","organization":"Universidade de Lisboa — UL","country":{"code":"PT","name":"Portugal"},"ror":"01c27hj86"}],"orcid":"0000-0001-8560-5487"},{"first_name":"Richard","last_name":"Brito","name":"Richard Brito","affiliations":[{"value":"CENTRA, Departamento de Física, Instituto Superior Técnico — IST, Universidade de Lisboa — UL, Avenida Rovisco Pais 1, Lisboa, 1049-001, Portugal","organization":"Universidade de Lisboa — UL","country":{"code":"PT","name":"Portugal"},"ror":"01c27hj86"}],"orcid":"0000-0002-7807-3053"}],"publication_info":[{"journal_volume":"2026","journal_issue":"10","journal_title":"Journal of High Energy Physics","material":"article","page_start":"1","page_end":"16","artid":"JHEP10(2026)034","volume_year":"2026","journal_issue_date":null,"publisher":"Springer"}],"subtitle":"","related_materials":[],"abstract":"Black hole spectroscopy allows to infer the properties of the remnant of a binary black hole coalescence. Motivated by the recent proposal that a black hole’s information load can alter its classical response to small perturbations, an effect known as the swift memory burden (SMB), we develop a minimal phenomenological framework to analyze the ringdown of a binary black hole merger and confront it with the data from the GW250114 event. In particular, we model the SMB imprint through a suppression factor derived as an upper bound and adopt the least-suppressive form. We perform a Bayesian analysis combining the frequencies of the (220) and (440) quasi-normal modes and obtain a lower bound log $\\textit{p}$ ≳ 2, where $\\textit{p}$ controls how the gaps reopen when the black hole’s master mode occupation departs from the critical value. Moreover, using a Fisher information matrix (high signal-to-noise ratio) approximation, we forecast the lower bound log $\\textit{p}$ ≳ 3 for a GW250114-like event observed with Cosmic Explorer or Einstein Telescope. Within this minimal, weak-effect framework, our results disfavour rapid gap reopening, shedding light on how the swift memory burden effect can be probed with current and next-generation detectors.","reception_date":null,"_created_at":"2026-10-03T12:55:33.630911","_updated_at":"2026-10-03T12:55:39.302931+00:00","publication_date":"2026-10-02","id":111679,"copyright":[{"statement":"","year":2026,"holder":"The Author(s)"}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)034/13130_2026_Article_30201.xml.scoap.xml","created":"2026-10-03T12:55:39.032051+00:00","updated":"2026-10-03T12:55:39.032061+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)034/13130_2026_Article_30201_a.pdf","created":"2026-10-03T12:55:39.056029+00:00","updated":"2026-10-03T12:55:39.056040+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/4.0/","name":"CC-BY-4.0"}],"article_arxiv_category":[{"category":"gr-qc","primary":true},{"category":"astro-ph.HE","primary":false},{"category":"hep-ph","primary":false},{"category":"hep-th","primary":false}],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1007/JHEP10(2026)034"},{"identifier_type":"arXiv","identifier_value":"2510.19916"}]},{"first_online_date":null,"title":"Generalized replica manifolds. Part I. Surgery and averaging","acceptance_date":null,"doi":"10.1007/JHEP10(2026)023","countries":["US"],"authors":[{"first_name":"Mohamed","last_name":"Radwan","name":"Mohamed Radwan","affiliations":[{"value":"Department of Physics and Astronomy, University of Kentucky, Lexington, KY, 40506, USA","organization":"University of Kentucky","country":{"code":"US","name":"United States"},"ror":"02k3smh20"}],"orcid":"0009-0005-9819-9656"}],"publication_info":[{"journal_volume":"2026","journal_issue":"10","journal_title":"Journal of High Energy Physics","material":"article","page_start":"1","page_end":"62","artid":"JHEP10(2026)023","volume_year":"2026","journal_issue_date":null,"publisher":"Springer"}],"subtitle":"","related_materials":[],"abstract":"We develop a simple framework for implementing a type of path integral “surgery” through a correlated averaging over codimension-one defects/extended operators. This technique is then used to construct replica manifolds by effectively cutting and gluing the path integral without explicitly modifying the underlying manifold. We argue that restricted forms of this averaging may be used to calculate Rényi entanglement entropy corresponding to a wide range of choices of subsystem partitioning. When the entanglement entropy being calculated in this way does not simply correspond to entanglement between subregions, we call the resulting objects from this surgery “generalized replica manifolds”. We show how this framework extends to gauge theories and, in particular, how in non-Abelian gauge theories it establishes a connection between replica calculations of a gauge-invariant notion of entanglement between color degrees of freedom and a quiver gauge theory structure. Finally, we discuss how this framework looks in the context of large-$\\textit{N}$ theories and holography, with a bird’s-eye view of potential future directions. This paper focuses on averaging over operators that form a representation of the Heisenberg group; a subsequent paper will focus on how we can extend this framework to more general operator averaging.","reception_date":null,"_created_at":"2026-10-03T12:55:33.591270","_updated_at":"2026-10-03T12:55:39.237833+00:00","publication_date":"2026-10-02","id":111680,"copyright":[{"statement":"","year":2026,"holder":"The Author(s)"}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)023/13130_2026_Article_30190.xml.scoap.xml","created":"2026-10-03T12:55:39.031351+00:00","updated":"2026-10-03T12:55:39.031362+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)023/13130_2026_Article_30190_a.pdf","created":"2026-10-03T12:55:39.055998+00:00","updated":"2026-10-03T12:55:39.056008+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/4.0/","name":"CC-BY-4.0"}],"article_arxiv_category":[{"category":"hep-th","primary":true}],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1007/JHEP10(2026)023"},{"identifier_type":"arXiv","identifier_value":"2510.20900"}]},{"first_online_date":null,"title":"Scaling properties of net-baryon number fluctuations at the deconfinement critical point","acceptance_date":null,"doi":"10.1103/lcgf-r6vy","countries":["PL","JP"],"authors":[{"first_name":"Michał","last_name":"Szymański","name":"Michał Szymański","affiliations":[{"value":"Institute of Theoretical Physics, <a href=\"https://ror.org/00yae6e25\">University of Wrocław</a>, Plac Maksa Borna 9, PL-50204 Wrocław, Poland","organization":"Institute of Theoretical Physics, University of Wrocław, Plac Maksa Borna 9, PL-50204 Wrocław, Poland","country":{"code":"PL","name":"Poland"},"ror":"00yae6e25"}],"orcid":"0000-0002-3110-9039"},{"first_name":"Pok Man","last_name":"Lo","name":"Pok Man Lo","affiliations":[{"value":"Institute of Theoretical Physics, <a href=\"https://ror.org/00yae6e25\">University of Wrocław</a>, Plac Maksa Borna 9, PL-50204 Wrocław, Poland","organization":"Institute of Theoretical Physics, University of Wrocław, Plac Maksa Borna 9, PL-50204 Wrocław, Poland","country":{"code":"PL","name":"Poland"},"ror":"00yae6e25"}],"orcid":"0000-0002-2866-7996"},{"first_name":"Krzysztof","last_name":"Redlich","name":"Krzysztof Redlich","affiliations":[{"value":"Institute of Theoretical Physics, <a href=\"https://ror.org/00yae6e25\">University of Wrocław</a>, Plac Maksa Borna 9, PL-50204 Wrocław, Poland and <a href=\"https://ror.org/01dr6c206\">Polish Academy of Sciences PAN</a>, Podwale 75, PL-50449 Wrocław, Poland","organization":"Institute of Theoretical Physics, University of Wrocław, Plac Maksa Borna 9, PL-50204 Wrocław, Poland and Polish Academy of Sciences PAN, Podwale 75, PL-50449 Wrocław, Poland","country":{"code":"PL","name":"Poland"},"ror":"01dr6c206"}],"orcid":"0000-0002-2629-1710"},{"first_name":"Chihiro","last_name":"Sasaki","name":"Chihiro Sasaki","affiliations":[{"value":"Institute of Theoretical Physics, <a href=\"https://ror.org/00yae6e25\">University of Wrocław</a>, Plac Maksa Borna 9, PL-50204 Wrocław, Poland and International Institute for Sustainability with Knotted Chiral Meta Matter (WPI-SKCM<sup>2</sup>), <a href=\"https://ror.org/03t78wx29\">Hiroshima University</a>, Higashi-Hiroshima, Hiroshima 739-8531, Japan","organization":"Institute of Theoretical Physics, University of Wrocław, Plac Maksa Borna 9, PL-50204 Wrocław, Poland and International Institute for Sustainability with Knotted Chiral Meta Matter (WPI-SKCM<sup>2</sup>), Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8531, Japan","country":{"code":"JP","name":"Japan"},"ror":"03t78wx29"}],"orcid":"0000-0003-4612-3375"}],"publication_info":[{"journal_volume":"114","journal_issue":"7","journal_title":"Physical Review D","material":"article","page_start":"","page_end":"","artid":"","volume_year":"2026","journal_issue_date":null,"publisher":"APS"}],"subtitle":"","related_materials":[],"abstract":"<p>We investigate the critical behavior of the first four cumulants of the net-baryon number near the deconfinement critical point in QCD in the limit of heavy quarks. By connecting baryon-number fluctuations to Polyakov loop susceptibilities, we analyze their mean-field scaling properties at zero and nonzero baryon chemical potentials. In the mean-field approximation we derive critical exponents via the Landau theory and validate them through explicit numerical calculations in an effective Polyakov loop model. Using a Ginzburg-Landau criterion as a diagnostic of beyond-mean-field effects, we estimate the size of the critical region and find that it shrinks with increasing baryon density. By utilizing the exact scaling function in the 3D Ising model, we estimate critical exponents beyond the mean-field approximation.</p>","reception_date":null,"_created_at":"2026-10-02T18:00:39.058846+00:00","_updated_at":"2026-10-03T00:00:55.968008+00:00","publication_date":"2026-10-02","id":111662,"copyright":[{"statement":"Published by the American Physical Society","year":2026,"holder":""}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/lcgf-r6vy/lcgf-r6vy.pdf","created":"2026-10-02T18:00:54.522153+00:00","updated":"2026-10-02T18:00:54.522164+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/lcgf-r6vy/lcgf-r6vy.xml","created":"2026-10-02T18:00:54.535595+00:00","updated":"2026-10-02T18:00:54.535610+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/4.0/","name":"CC-BY-4.0"}],"article_arxiv_category":[{"category":"hep-ph","primary":true}],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1103/lcgf-r6vy"},{"identifier_type":"arXiv","identifier_value":"2605.08543"}]},{"first_online_date":null,"title":"Impact of future dihadron production measurements on the transversity distributions and tensor charges of the nucleon","acceptance_date":null,"doi":"10.1103/z2yx-bbk5","countries":["US"],"authors":[{"first_name":"Y.","last_name":"Sawaya","name":"Y. Sawaya","affiliations":[{"value":"Department of Physics, SERC, <a href=\"https://ror.org/00kx1jb78\">Temple University</a>, Philadelphia, Pennsylvania 19122, USA","organization":"Department of Physics, SERC, Temple University, Philadelphia, Pennsylvania 19122, USA","country":{"code":"US","name":"United States"},"ror":"00kx1jb78"}],"orcid":"0009-0000-9106-5165"},{"first_name":"C.","last_name":"Cocuzza","name":"C. Cocuzza","affiliations":[{"value":"Department of Physics, <a href=\"https://ror.org/03hsf0573\">College of William and Mary</a>, Williamsburg, Virginia 23185, USA","organization":"Department of Physics, College of William and Mary, Williamsburg, Virginia 23185, USA","country":{"code":"US","name":"United States"},"ror":"03hsf0573"}],"orcid":"0000-0003-4922-9247"},{"first_name":"G.","last_name":"Matousek","name":"G. Matousek","affiliations":[{"value":"Department of Physics, <a href=\"https://ror.org/00py81415\">Duke University</a>, Durham, North Carolina 27708, USA","organization":"Department of Physics, Duke University, Durham, North Carolina 27708, USA","country":{"code":"US","name":"United States"},"ror":"056w6an22"}]},{"first_name":"M.","last_name":"McEneaney","name":"M. McEneaney","affiliations":[{"value":"Department of Physics, <a href=\"https://ror.org/00py81415\">Duke University</a>, Durham, North Carolina 27708, USA","organization":"Department of Physics, Duke University, Durham, North Carolina 27708, USA","country":{"code":"US","name":"United States"},"ror":"056w6an22"}],"orcid":"0009-0006-3519-9744"},{"first_name":"A.","last_name":"Metz","name":"A. Metz","affiliations":[{"value":"Department of Physics, SERC, <a href=\"https://ror.org/00kx1jb78\">Temple University</a>, Philadelphia, Pennsylvania 19122, USA","organization":"Department of Physics, SERC, Temple University, Philadelphia, Pennsylvania 19122, USA","country":{"code":"US","name":"United States"},"ror":"00kx1jb78"}],"orcid":"0000-0002-0223-5618"},{"first_name":"D.","last_name":"Pitonyak","name":"D. Pitonyak","affiliations":[{"value":"Department of Physics, <a href=\"https://ror.org/05py5qd41\">Lebanon Valley College</a>, Annville, Pennsylvania 17003, USA","organization":"Department of Physics, Lebanon Valley College, Annville, Pennsylvania 17003, USA","country":{"code":"US","name":"United States"},"ror":"05py5qd41"}],"orcid":"0000-0001-8822-1323"},{"first_name":"A.","last_name":"Prokudin","name":"A. Prokudin","affiliations":[{"value":"<a href=\"https://ror.org/02vwzrd76\">Jefferson Lab</a>, Newport News, Virginia 23606, USA","organization":"Jefferson Lab, Newport News, Virginia 23606, USA","country":{"code":"US","name":"United States"},"ror":"000qn5756"},{"value":"Division of Science, <a href=\"https://ror.org/04p491231\">Penn State University Berks</a>, Reading, Pennsylvania 19610, USA","organization":"Division of Science, Penn State University Berks, Reading, Pennsylvania 19610, USA","country":{"code":"US","name":"United States"},"ror":"04p491231"}],"orcid":"0000-0001-5956-4159"},{"first_name":"N.","last_name":"Sato","name":"N. Sato","affiliations":[{"value":"<a href=\"https://ror.org/02vwzrd76\">Jefferson Lab</a>, Newport News, Virginia 23606, USA","organization":"Jefferson Lab, Newport News, Virginia 23606, USA","country":{"code":"US","name":"United States"},"ror":"000qn5756"}]},{"first_name":"A.","last_name":"Vossen","name":"A. Vossen","affiliations":[{"value":"Department of Physics, <a href=\"https://ror.org/00py81415\">Duke University</a>, Durham, North Carolina 27708, USA","organization":"Department of Physics, Duke University, Durham, North Carolina 27708, USA","country":{"code":"US","name":"United States"},"ror":"056w6an22"}]}],"publication_info":[{"journal_volume":"114","journal_issue":"7","journal_title":"Physical Review D","material":"article","page_start":"","page_end":"","artid":"","volume_year":"2026","journal_issue_date":null,"publisher":"APS"}],"subtitle":"","related_materials":[],"abstract":"<p>We assess the impact of future measurements of dihadron production in semi-inclusive deep-inelastic scattering from the CLAS12 and proposed SoLID experiments at Jefferson Lab, as well as from the ePIC experiment at the future Electron-Ion Collider (EIC), on the transversity parton distribution functions (PDFs) and the corresponding tensor charges of the nucleon. To this end, we generate pseudodata for these experiments for a proton target (CLAS12 and ePIC) and a <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mrow><mmultiscripts><mrow><mi>He</mi></mrow><mprescripts></mprescripts><none></none><mrow><mn>3</mn></mrow></mmultiscripts></mrow></math> target (SoLID and ePIC), and we include these pseudodata in the JAMDiFF global analysis of existing experimental dihadron data. We find that future data from Jefferson Lab will significantly reduce uncertainties in the transversity PDFs in the region of intermediate-to-large quark momentum fractions <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>x</mi></math>, while the EIC will provide strong constraints across the entire range of <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>x</mi></math>, allowing for the first experimental test of the predicted small-<math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>x</mi></math> behavior of the transversity PDFs. In discussing the reduction of uncertainties in the tensor charges, we also compare the results from the data analyses with those from lattice QCD, highlighting scenarios in which compatibility or tension between the two would arise.</p>","reception_date":null,"_created_at":"2026-10-02T18:00:19.316056+00:00","_updated_at":"2026-10-03T00:00:44.376946+00:00","publication_date":"2026-10-02","id":111657,"copyright":[{"statement":"Published by the American Physical Society","year":2026,"holder":""}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/z2yx-bbk5/z2yx-bbk5.pdf","created":"2026-10-02T18:00:35.801675+00:00","updated":"2026-10-02T18:00:35.801684+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/z2yx-bbk5/z2yx-bbk5.xml","created":"2026-10-02T18:00:35.805443+00:00","updated":"2026-10-02T18:00:35.805451+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/4.0/","name":"CC-BY-4.0"}],"article_arxiv_category":[{"category":"hep-ph","primary":true},{"category":"hep-ex","primary":false},{"category":"nucl-th","primary":false}],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1103/z2yx-bbk5"},{"identifier_type":"arXiv","identifier_value":"2606.00362"}]},{"first_online_date":null,"title":"Multiparticle states investigation with the tensor renormalization group method","acceptance_date":null,"doi":"10.1103/zhq7-swns","countries":["JP"],"authors":[{"first_name":"Fathiyya Izzatun","last_name":"Az-zahra","name":"Fathiyya Izzatun Az-zahra","affiliations":[{"value":"Institute for Theoretical Physics, <a href=\"https://ror.org/02hwp6a56\">Kanazawa University</a>, Kanazawa 920-1192, Japan","organization":"Institute for Theoretical Physics, Kanazawa University, Kanazawa 920-1192, Japan","country":{"code":"JP","name":"Japan"},"ror":"02hwp6a56"}],"orcid":"0009-0002-2942-9954"},{"first_name":"Shinji","last_name":"Takeda","name":"Shinji Takeda","affiliations":[{"value":"Institute for Theoretical Physics, <a href=\"https://ror.org/02hwp6a56\">Kanazawa University</a>, Kanazawa 920-1192, Japan","organization":"Institute for Theoretical Physics, Kanazawa University, Kanazawa 920-1192, Japan","country":{"code":"JP","name":"Japan"},"ror":"02hwp6a56"}],"orcid":"0000-0003-2485-5233"},{"first_name":"Takeshi","last_name":"Yamazaki","name":"Takeshi Yamazaki","affiliations":[{"value":"Center for Computational Sciences, <a href=\"https://ror.org/02956yf07\">University of Tsukuba</a>, Tsukuba 305-8577, Japan","organization":"Center for Computational Sciences, University of Tsukuba, Tsukuba 305-8577, Japan","country":{"code":"JP","name":"Japan"},"ror":"02956yf07"},{"value":"Institute of Pure and Applied Sciences, <a href=\"https://ror.org/02956yf07\">University of Tsukuba</a>, Tsukuba 305-8571, Japan","organization":"Institute of Pure and Applied Sciences, University of Tsukuba, Tsukuba 305-8571, Japan","country":{"code":"JP","name":"Japan"},"ror":"02956yf07"}],"orcid":"0000-0001-7238-7222"}],"publication_info":[{"journal_volume":"114","journal_issue":"7","journal_title":"Physical Review D","material":"article","page_start":"","page_end":"","artid":"","volume_year":"2026","journal_issue_date":null,"publisher":"APS"}],"subtitle":"","related_materials":[],"abstract":"<p>We investigate multiparticle states of the <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mrow><mo stretchy=\"false\">(</mo><mn>1</mn><mo>+</mo><mn>1</mn><mo stretchy=\"false\">)</mo><mi mathvariant=\"normal\">d</mi></mrow></math> Ising Model using a spectroscopy scheme based on the transfer matrix and tensor renormalization group method. The scheme begins with computing the energy spectrum of the system from the transfer matrix estimated by the coarse-grained tensor network. The quantum number and momentum of these energy eigenstates are not <i>a priori</i> known, thus we identify them using matrix elements of an interpolating operator that is numerically computed with an impurity tensor network. Furthermore, by observing the dependence of the energy as a function of system size, we identify the number of particles of the eigenstates and obtain one-, two-, and three-particle states for a specific quantum number and momentum. From the two-particle state sector, we compute the scattering phase shift using Lüscher’s formula and the wave function approach, and observe their consistency with theoretical prediction. Using the information of the two-particle scattering phase shift, we investigate the degeneracy of the two-particle states, the theoretical prediction of the three-particle finite volume energy, and also the degeneracy in the three-particle states.</p>","reception_date":null,"_created_at":"2026-10-02T18:00:19.095033+00:00","_updated_at":"2026-10-03T00:00:44.018265+00:00","publication_date":"2026-10-02","id":111661,"copyright":[{"statement":"Published by the American Physical Society","year":2026,"holder":""}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/zhq7-swns/zhq7-swns.pdf","created":"2026-10-02T18:00:41.191817+00:00","updated":"2026-10-02T18:00:41.191826+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/zhq7-swns/zhq7-swns.xml","created":"2026-10-02T18:00:41.210579+00:00","updated":"2026-10-02T18:00:41.210593+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/4.0/","name":"CC-BY-4.0"}],"article_arxiv_category":[{"category":"hep-lat","primary":true}],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1103/zhq7-swns"},{"identifier_type":"arXiv","identifier_value":"2606.22321"}]}]}