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In this formulation, the generalized thermodynamic force is described by an Abelian thermodynamic connection, and ordinary Onsager dynamics is recovered by fixing its temporal component through the dissipation function.","copyright":[{"statement":"The Authors","year":2026,"holder":"The Authors"}],"authors":[{"first_name":"So","last_name":"Katagiri","name":"So Katagiri","affiliations":[{"value":"Major in Complex Systems Science, Graduate School of Science and Engineering, Ibaraki University, Nakanarusawa-cho, Hitachi, 316-8511, Japan","organization":"Major in Complex Systems Science, Graduate School of Science and Engineering, Ibaraki University","country":{"code":"JP","name":"Japan"}}],"orcid":"0000-0002-0709-3065"}],"countries":["JP"],"article_arxiv_category":[],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1016/j.nuclphysb.2026.117698/main.pdf","created":"2026-10-24T06:32:07.119684+00:00","updated":"2026-10-24T06:32:07.119695+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1016/j.nuclphysb.2026.117698/main.xml","created":"2026-10-24T06:32:07.128081+00:00","updated":"2026-10-24T06:32:07.128091+00:00"}],"related_materials":[],"first_online_date":null,"title":"A gauge-theoretic formulation of Nambu non-equilibrium thermodynamics"},{"related_licenses":[{"url":"http://creativecommons.org/licenses/by/3.0/","name":"CC-BY-3.0"}],"publication_date":"2026-10-23","acceptance_date":null,"id":112460,"_updated_at":"2026-10-25T00:05:45.346709+00:00","_created_at":"2026-10-25T00:05:40.623640","publication_info":[{"journal_volume":"883 C","journal_issue":"","journal_title":"Physics Letters B","material":"","page_start":"","page_end":"","artid":"141089","volume_year":"2026","journal_issue_date":null,"publisher":"Elsevier"}],"reception_date":null,"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1016/j.physletb.2026.141089"}],"subtitle":"","doi":"10.1016/j.physletb.2026.141089","abstract":"We construct and analyze static multipolar black holes in Einstein-vector-Gauss-Bonnet theory with a quadratic coupling function. The vectorized solutions bifurcate from the Schwarzschild black hole at discrete values of the Gauss-Bonnet coupling, obtained from a perturbative eigenvalue problem on the Schwarzschild background and labelled by the angular multipole number ℓ. We restrict to the fundamental radial branches. The electric sector contains the known spherically symmetric <math altimg='si3.svg'><mrow><mi>&#8467;</mi><mo linebreak='goodbreak'>=</mo><mn>0</mn></mrow></math> branch as well as axisymmetric branches with &#8467;&#8239;&gt;&#8239;0. These electric branches extend to larger values of the coupling. The magnetic sector features a sequence of axisymmetric branches, including the previously found magnetic dipole branch at <math altimg='si3.svg'><mrow><mi>&#8467;</mi><mo linebreak='goodbreak'>=</mo><mn>0</mn></mrow></math>. The magnetic branches instead exist only on finite intervals of the coupling, ending at critical solutions. Away from the bifurcation point, nonlinearities generate additional multipoles, but even-&#8467; and odd-&#8467; moments remain separated.","copyright":[{"statement":"The Authors","year":2026,"holder":"The Authors"}],"authors":[{"first_name":"Burkhard","last_name":"Kleihaus","name":"Burkhard Kleihaus","affiliations":[{"value":"Institut für Physik, Universität Oldenburg, Postfach 2503, D-26111, Oldenburg, Germany","organization":"Institut für Physik, Universität Oldenburg","country":{"code":"DE","name":"Germany"}}],"orcid":"0000-0001-9751-4400"},{"first_name":"Jutta","last_name":"Kunz","name":"Jutta Kunz","affiliations":[{"value":"Institut für Physik, Universität Oldenburg, Postfach 2503, D-26111, Oldenburg, Germany","organization":"Institut für Physik, Universität Oldenburg","country":{"code":"DE","name":"Germany"}}],"orcid":"0000-0001-7990-8713"}],"countries":["DE"],"article_arxiv_category":[],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1016/j.physletb.2026.141089/main.pdf","created":"2026-10-25T00:05:45.173784+00:00","updated":"2026-10-25T00:05:45.173795+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1016/j.physletb.2026.141089/main.xml","created":"2026-10-25T00:05:45.181579+00:00","updated":"2026-10-25T00:05:45.181589+00:00"}],"related_materials":[],"first_online_date":null,"title":"Static multipolar Einstein-vector-Gauss-Bonnet black holes"},{"related_licenses":[{"url":"http://creativecommons.org/licenses/by/4.0/","name":"CC-BY-4.0"}],"publication_date":"2026-10-23","acceptance_date":null,"id":112454,"_updated_at":"2026-10-24T12:55:50.800082+00:00","_created_at":"2026-10-24T12:55:26.003503","publication_info":[{"journal_volume":"2026","journal_issue":"10","journal_title":"Journal of High Energy Physics","material":"article","page_start":"1","page_end":"41","artid":"JHEP10(2026)236","volume_year":"2026","journal_issue_date":null,"publisher":"Springer"}],"reception_date":null,"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1007/JHEP10(2026)236"},{"identifier_type":"arXiv","identifier_value":"2607.21139"}],"subtitle":"","doi":"10.1007/JHEP10(2026)236","abstract":"We study energy-energy correlators (EEC) in planar $$ \\mathcal{N} $$ = 4 super Yang-Mills theory at strong ’t Hooft coupling $\\textit{λ}$. We consider the EEC in states created by half-BPS operators of arbitrary dimension $\\textit{p}$, and determine the corresponding event-shape function up to order $\\textit{λ}$ from the worldsheet representation of the AdS Virasoro-Shapiro amplitude with Kaluza-Klein external states. For $\\textit{p}$ = 2 we compute the second curvature correction, which completes the EEC through order $\\textit{λ}$ ; the new contribution improves the agreement with recently derived non-perturbative bounds at intermediate coupling. We further develop a complementary method in which the strong-coupling expansion coefficients of the EEC are extracted directly from the Wilson coefficients of low-energy expansion of the AdS Virasoro-Shapiro amplitude, and find the two approaches in perfect agreement.","copyright":[{"statement":"","year":2026,"holder":"The Author(s)"}],"authors":[{"first_name":"Max","last_name":"Jackson","name":"Max Jackson","affiliations":[{"value":"Centre for Theoretical Physics and Astronomy, Department of Physics and Astronomy, Queen Mary University of London, Mile End Road, London, E1 4NS, U.K.","organization":"Queen Mary University of London","country":{"code":"GB","name":"United Kingdom"},"ror":"026zzn846"}],"orcid":"0009-0000-7915-4704"},{"first_name":"Lecheng","last_name":"Ren","name":"Lecheng Ren","affiliations":[{"value":"Centre for Theoretical Physics and Astronomy, Department of Physics and Astronomy, Queen Mary University of London, Mile End Road, London, E1 4NS, U.K.","organization":"Queen Mary University of London","country":{"code":"GB","name":"United Kingdom"},"ror":"026zzn846"}],"orcid":"0000-0002-0846-8017"},{"first_name":"Bo","last_name":"Wang","name":"Bo Wang","affiliations":[{"value":"Department of Physics, Yale University, New Haven, CT, 06511, USA","organization":"Yale University","country":{"code":"US","name":"United States"},"ror":"03v76x132"},{"value":"Zhejiang Institute of Modern Physics, School of Physics, Zhejiang University, Zhejiang, Hangzhou, 310058, China","organization":"Zhejiang University","country":{"code":"CN","name":"China"},"ror":"00a2xv884"}],"orcid":"0000-0002-7119-0791"},{"first_name":"Congkao","last_name":"Wen","name":"Congkao Wen","affiliations":[{"value":"Centre for Theoretical Physics and Astronomy, Department of Physics and Astronomy, Queen Mary University of London, Mile End Road, London, E1 4NS, U.K.","organization":"Queen Mary University of London","country":{"code":"GB","name":"United Kingdom"},"ror":"026zzn846"}],"orcid":"0000-0002-5174-1576"}],"countries":["CN","US","GB"],"article_arxiv_category":[{"category":"hep-th","primary":true},{"category":"hep-ph","primary":false}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)236/13130_2026_Article_30403.xml.scoap.xml","created":"2026-10-24T12:55:50.582338+00:00","updated":"2026-10-24T12:55:50.582349+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)236/13130_2026_Article_30403_a.pdf","created":"2026-10-24T12:55:50.586349+00:00","updated":"2026-10-24T12:55:50.586359+00:00"}],"related_materials":[],"first_online_date":null,"title":"Energy-energy correlators at strong coupling"},{"related_licenses":[{"url":"http://creativecommons.org/licenses/by/4.0/","name":"CC-BY-4.0"}],"publication_date":"2026-10-23","acceptance_date":null,"id":112453,"_updated_at":"2026-10-24T12:55:49.881514+00:00","_created_at":"2026-10-24T12:55:28.987018","publication_info":[{"journal_volume":"2026","journal_issue":"10","journal_title":"Journal of High Energy Physics","material":"article","page_start":"1","page_end":"39","artid":"JHEP10(2026)245","volume_year":"2026","journal_issue_date":null,"publisher":"Springer"}],"reception_date":null,"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1007/JHEP10(2026)245"},{"identifier_type":"arXiv","identifier_value":"2608.02720"}],"subtitle":"","doi":"10.1007/JHEP10(2026)245","abstract":"Thermal fluctuations are generally expected to destroy order and restore symmetries at sufficiently high temperatures. Recently, however, a family of scalar theories in 2 + 1 dimensions was shown to exhibit $\\textit{ℤ}$ symmetry breaking that persists to arbitrarily high temperatures using a variety of approaches, including the $\\textit{ϵ}$-expansion, the FRG, and large-$\\textit{N}$ techniques. Although the similarities among these theories suggest that they belong to the same universality class, this connection has not been established explicitly. In this work, we fill this gap. Using large-$\\textit{N}$ methods, we analytically study the biconical vector model in a range of spacetime dimensions, including 2 + 1, at leading and next-to-leading order in the 1/$\\textit{N}$ expansion. We determine the RG flow, fixed-point structure, and the CFT data of the infrared theory, reproducing and extending previous results and thereby unifying the apparently distinct constructions within a common analytic framework. We derive the effective potential, establish its stable minima at zero and finite temperature, and demonstrate spontaneous $\\textit{ℤ}$ symmetry breaking at arbitrarily high temperatures for large finite $\\textit{N}$.","copyright":[{"statement":"","year":2026,"holder":"The Author(s)"}],"authors":[{"first_name":"Michael","last_name":"Smolkin","name":"Michael Smolkin","affiliations":[{"value":"The Racah Institute of Physics, The Hebrew University of Jerusalem, Jerusalem, 91904, Israel","organization":"The Hebrew University of Jerusalem","country":{"code":"IL","name":"Israel"},"ror":"03qxff017"}],"orcid":"0000-0003-4638-6386"},{"first_name":"Lev","last_name":"Yung","name":"Lev Yung","affiliations":[{"value":"The Racah Institute of Physics, The Hebrew University of Jerusalem, Jerusalem, 91904, Israel","organization":"The Hebrew University of Jerusalem","country":{"code":"IL","name":"Israel"},"ror":"03qxff017"}],"orcid":"0009-0007-9992-6338"}],"countries":["IL"],"article_arxiv_category":[{"category":"hep-th","primary":true},{"category":"cond-mat.str-el","primary":false}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)245/13130_2026_Article_30412.xml.scoap.xml","created":"2026-10-24T12:55:49.770567+00:00","updated":"2026-10-24T12:55:49.770577+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)245/13130_2026_Article_30412_a.pdf","created":"2026-10-24T12:55:49.775381+00:00","updated":"2026-10-24T12:55:49.775389+00:00"}],"related_materials":[],"first_online_date":null,"title":"Thermal order in the biconical model"},{"related_licenses":[{"url":"http://creativecommons.org/licenses/by/4.0/","name":"CC-BY-4.0"}],"publication_date":"2026-10-23","acceptance_date":null,"id":112452,"_updated_at":"2026-10-24T12:55:45.387218+00:00","_created_at":"2026-10-24T12:55:37.292955","publication_info":[{"journal_volume":"2026","journal_issue":"10","journal_title":"Journal of High Energy Physics","material":"article","page_start":"1","page_end":"40","artid":"JHEP10(2026)238","volume_year":"2026","journal_issue_date":null,"publisher":"Springer"}],"reception_date":null,"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1007/JHEP10(2026)238"},{"identifier_type":"arXiv","identifier_value":"2507.08588"}],"subtitle":"","doi":"10.1007/JHEP10(2026)238","abstract":"$$ T\\overline{T} $$ -deformed CFTs are known to possess nonlocal Virasoro×Virasoro symmetries, whose currents depend on integration of the stress tensor. Unfortunately, these symmetries do not act in a tractable manner on the undeformed operators, which are defined by evolving local operators in the undeformed CFT on a constant-time slice using the deformed Hamiltonian. In this paper, we explicitly construct two distinct classes of operators: (i) dressed operators, which are primary with respect to the Virasoro×Virasoro symmetries, and (ii) physical operators, a new type of operator that depends on fundamental fields at specific points and is therefore local at the classical level. While dressed operators preserve the conformal symmetry structure, they are themselves nonlocal in the sense that they depend on integrated quantities. Physical operators, by contrast, depend only on local fields. Moreover, physical operators can be expressed in terms of dressed operators, and this relation can be promoted to a definition of such operators at the quantum level. This enables the use of Virasoro×Virasoro symmetries to systematically compute physical quantities such as correlation functions. We calculate the two-point correlation functions of these operators in momentum space and find that our results align with both string theory predictions and field theory calculations. Additionally, we explore the relationship between physical operators and alternative operator definitions proposed in the literature.","copyright":[{"statement":"","year":2026,"holder":"The Author(s)"}],"authors":[{"first_name":"Liangyu","last_name":"Chen","name":"Liangyu Chen","affiliations":[{"value":"Yau Mathematical Sciences Center, Tsinghua University, Jingzhai, Haidian District, Beijing, 100084, China","organization":"Tsinghua University","country":{"code":"CN","name":"China"},"ror":"03cve4549"}],"orcid":"0000-0002-5543-2754"},{"first_name":"Zhengyuan","last_name":"Du","name":"Zhengyuan Du","affiliations":[{"value":"Center for the Fundamental Laws of Nature, Harvard University, 17 Oxford Street, Cambridge, MA, 02138, USA","organization":"Harvard University","country":{"code":"US","name":"United States"},"ror":"03vek6s52"},{"value":"Yau Mathematical Sciences Center, Tsinghua University, Jingzhai, Haidian District, Beijing, 100084, China","organization":"Tsinghua University","country":{"code":"CN","name":"China"},"ror":"03cve4549"},{"value":"Department of Mathematical Sciences, Tsinghua University, No. 1 Tsinghua Garden, Haidian District, Beijing, 100084, China","organization":"Tsinghua University","country":{"code":"CN","name":"China"},"ror":"03cve4549"}],"orcid":"0009-0000-1568-4343"},{"first_name":"Kangning","last_name":"Liu","name":"Kangning Liu","affiliations":[{"value":"Yau Mathematical Sciences Center, Tsinghua University, Jingzhai, Haidian District, Beijing, 100084, China","organization":"Tsinghua University","country":{"code":"CN","name":"China"},"ror":"03cve4549"},{"value":"Department of Mathematical Sciences, Tsinghua University, No. 1 Tsinghua Garden, Haidian District, Beijing, 100084, China","organization":"Tsinghua University","country":{"code":"CN","name":"China"},"ror":"03cve4549"}],"orcid":"0009-0009-5266-3600"},{"first_name":"Wei","last_name":"Song","name":"Wei Song","affiliations":[{"value":"Peng Huanwu Center for Fundamental Theory, 96 Jinzhai Road, Hefei, Anhui, 230026, China","organization":"Peng Huanwu Center for Fundamental Theory","country":{"code":"CN","name":"China"},"ror":"01s9dmg43"},{"value":"Yau Mathematical Sciences Center, Tsinghua University, Jingzhai, Haidian District, Beijing, 100084, China","organization":"Tsinghua University","country":{"code":"CN","name":"China"},"ror":"03cve4549"},{"value":"Department of Mathematical Sciences, Tsinghua University, No. 1 Tsinghua Garden, Haidian District, Beijing, 100084, China","organization":"Tsinghua University","country":{"code":"CN","name":"China"},"ror":"03cve4549"}],"orcid":"0000-0001-6625-719X"}],"countries":["CN","US"],"article_arxiv_category":[{"category":"hep-th","primary":true}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)238/13130_2026_Article_30405.xml.scoap.xml","created":"2026-10-24T12:55:45.163307+00:00","updated":"2026-10-24T12:55:45.163317+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)238/13130_2026_Article_30405_a.pdf","created":"2026-10-24T12:55:45.170772+00:00","updated":"2026-10-24T12:55:45.170782+00:00"}],"related_materials":[],"first_online_date":null,"title":"Symmetries and operators in $$ T\\overline{T} $$ deformed CFTs"},{"related_licenses":[{"url":"http://creativecommons.org/licenses/by/4.0/","name":"CC-BY-4.0"}],"publication_date":"2026-10-23","acceptance_date":null,"id":112451,"_updated_at":"2026-10-24T12:55:30.115464+00:00","_created_at":"2026-10-24T12:55:26.168744","publication_info":[{"journal_volume":"2026","journal_issue":"10","journal_title":"Journal of High Energy Physics","material":"article","page_start":"1","page_end":"17","artid":"JHEP10(2026)246","volume_year":"2026","journal_issue_date":null,"publisher":"Springer"}],"reception_date":null,"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1007/JHEP10(2026)246"},{"identifier_type":"arXiv","identifier_value":"2606.28492"}],"subtitle":"","doi":"10.1007/JHEP10(2026)246","abstract":"The Monte Carlo (MC) replica method quantifies parameter uncertainties in global fits of parton distribution functions (PDFs) and Standard Model Effective Field Theory (SMEFT) Wilson coefficients by fitting a model to many noise-perturbed copies of the data and taking the empirical distribution of the best-fit parameters as the uncertainty. The method reproduces the Bayesian posterior exactly only when the model is linear in its parameters, and departs from it in the nonlinear case. We derive the leading-order distribution the method produces and compare it with the Laplace approximation of the Bayesian posterior: the two differ by a single computable matrix, the residual-weighted Hessian of the model at the best fit, whose sign and magnitude set the over- or under-estimation of the parameter uncertainties. This closed-form expression quantifies when and by how much the MC method departs from Bayesian inference. We illustrate it on two single-parameter examples solvable in closed form and point to its evaluation in full PDF and SMEFT fits as a natural next step.","copyright":[{"statement":"","year":2026,"holder":"The Author(s)"}],"authors":[{"first_name":"Mark","last_name":"Costantini","name":"Mark Costantini","affiliations":[{"value":"DAMTP, University of Cambridge, Wilberforce Road, Cambridge, CB3 0WA, U.K.","organization":"University of Cambridge","country":{"code":"GB","name":"United Kingdom"},"ror":"013meh722"}],"orcid":"0009-0002-3891-584X"}],"countries":["GB"],"article_arxiv_category":[{"category":"hep-ph","primary":true}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)246/13130_2026_Article_30413.xml.scoap.xml","created":"2026-10-24T12:55:29.995796+00:00","updated":"2026-10-24T12:55:29.995805+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)246/13130_2026_Article_30413_a.pdf","created":"2026-10-24T12:55:30.010972+00:00","updated":"2026-10-24T12:55:30.010982+00:00"}],"related_materials":[],"first_online_date":null,"title":"Propagating data noise through the fit: the Monte Carlo replica distribution"},{"related_licenses":[{"url":"http://creativecommons.org/licenses/by/4.0/","name":"CC-BY-4.0"}],"publication_date":"2026-10-23","acceptance_date":null,"id":112439,"_updated_at":"2026-10-24T06:55:40.539730+00:00","_created_at":"2026-10-24T06:55:31.658885","publication_info":[{"journal_volume":"2026","journal_issue":"10","journal_title":"Journal of High Energy Physics","material":"article","page_start":"1","page_end":"39","artid":"JHEP10(2026)244","volume_year":"2026","journal_issue_date":null,"publisher":"Springer"}],"reception_date":null,"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1007/JHEP10(2026)244"},{"identifier_type":"arXiv","identifier_value":"2606.09732"}],"subtitle":"","doi":"10.1007/JHEP10(2026)244","abstract":"We calculate the “kinematic” corrections $$ t/{P}_z^2 $$ and $$ {m}_N^2/{P}_z^2 $$ to the short distance expansion of gauge-invariant nonlocal quark-antiquark operators sandwiched between nucleon states with different momenta. Here $\\textit{t}$ is the momentum transfer, $\\textit{m}$ is the nucleon mass and $\\textit{P}$ is the momentum component in the direction of the quark-antiquark separation, which is assumed to be large. These matrix elements can be calculated in lattice QCD and, at leading twist, expressed in terms of moments of the generalized parton distributions (GPDs). Our results allow one to control one of principal uncertainties in such calculations and extend their region of applicability to larger momentum transfers, which is important in the quest to access the three-dimension image of the proton. The calculated corrections turn out to be significant for a realistic lattice QCD setup.","copyright":[{"statement":"","year":2026,"holder":"The Author(s)"}],"authors":[{"first_name":"Vladimir","last_name":"Braun","name":"Vladimir Braun","affiliations":[{"value":"Institut für Theoretische Physik, Universität Regensburg, Regensburg, D-93040, Germany","organization":"Universität Regensburg","country":{"code":"DE","name":"Germany"},"ror":"01eezs655"}],"orcid":"0000-0001-5400-2974"},{"first_name":"Hua-Yu","last_name":"Jiang","name":"Hua-Yu Jiang","affiliations":[{"value":"Institute of Particle and Nuclear Physics, Henan Normal University, Xinxiang, Henan, 453007, P.R. China","organization":"Henan Normal University","country":{"code":"CN","name":"China"},"ror":"00s13br28"}],"orcid":"0000-0002-4910-0104"}],"countries":["DE","CN"],"article_arxiv_category":[{"category":"hep-ph","primary":true}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)244/13130_2026_Article_30411.xml.scoap.xml","created":"2026-10-24T06:55:40.486162+00:00","updated":"2026-10-24T06:55:40.486173+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)244/13130_2026_Article_30411_a.pdf","created":"2026-10-24T06:55:40.490552+00:00","updated":"2026-10-24T06:55:40.490560+00:00"}],"related_materials":[],"first_online_date":null,"title":"Finite-$\\textit{t}$ and target mass corrections for the short-distance expansion of quasi(pseudo) GPDs"},{"related_licenses":[{"url":"http://creativecommons.org/licenses/by/4.0/","name":"CC-BY-4.0"}],"publication_date":"2026-10-23","acceptance_date":null,"id":112438,"_updated_at":"2026-10-24T06:55:39.175965+00:00","_created_at":"2026-10-24T06:55:31.453012","publication_info":[{"journal_volume":"2026","journal_issue":"10","journal_title":"Journal of High Energy Physics","material":"article","page_start":"1","page_end":"31","artid":"JHEP10(2026)237","volume_year":"2026","journal_issue_date":null,"publisher":"Springer"}],"reception_date":null,"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1007/JHEP10(2026)237"},{"identifier_type":"arXiv","identifier_value":"2607.24933"}],"subtitle":"","doi":"10.1007/JHEP10(2026)237","abstract":"How do dark matter-nucleus interactions transition from the regimes of coherent scattering, where single phonons are produced, to that of individual nuclear recoils? Answering this question relies on understanding multiphonon excitations. Multiphonons are important for interpreting low-threshold direct detection experiments, yet are computationally prohibitive to compute. In this paper, we employ a 1D $\\textit{N}$ -site crystal lattice model where dark matter scattering can be computed exactly. We show that the only difference between coherent and incoherent scattering is that conservation of crystal momentum is enforced in coherent scattering. The momentum conservation constraint becomes less important as more phonons are produced, yielding the transition to incoherent scattering. Using numerical calculations of the 1D structure factor, we also obtain quantitative validation of using an incoherent approximation to compute sub-GeV dark matter scattering in realistic 3D crystals.","copyright":[{"statement":"","year":2026,"holder":"The Author(s)"}],"authors":[{"first_name":"Lynn","last_name":"Lin","name":"Lynn Lin","affiliations":[{"value":"Department of Physics, University of California San Diego, La Jolla, CA, 92093, USA","organization":"University of California San Diego","country":{"code":"US","name":"United States"},"ror":"0168r3w48"}],"orcid":"0009-0008-4454-6757"},{"first_name":"Tongyan","last_name":"Lin","name":"Tongyan Lin","affiliations":[{"value":"Department of Physics, University of California San Diego, La Jolla, CA, 92093, USA","organization":"University of California San Diego","country":{"code":"US","name":"United States"},"ror":"0168r3w48"}],"orcid":"0000-0003-4969-3285"},{"first_name":"Momei","last_name":"Fang","name":"Momei Fang","affiliations":[{"value":"Department of Physics, University of California San Diego, La Jolla, CA, 92093, USA","organization":"University of California San Diego","country":{"code":"US","name":"United States"},"ror":"0168r3w48"}],"orcid":"0009-0004-0085-9453"}],"countries":["US"],"article_arxiv_category":[{"category":"hep-ph","primary":true},{"category":"hep-ex","primary":false}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)237/13130_2026_Article_30404.xml.scoap.xml","created":"2026-10-24T06:55:39.017479+00:00","updated":"2026-10-24T06:55:39.017489+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP10(2026)237/13130_2026_Article_30404_a.pdf","created":"2026-10-24T06:55:39.030244+00:00","updated":"2026-10-24T06:55:39.030254+00:00"}],"related_materials":[],"first_online_date":null,"title":"Coherence from interference: a solvable model of sub-GeV dark matter-nucleus scattering"},{"related_licenses":[{"url":"http://creativecommons.org/licenses/by/4.0/","name":"CC-BY-4.0"}],"publication_date":"2026-10-23","acceptance_date":null,"id":112402,"_updated_at":"2026-10-24T00:01:11.503974+00:00","_created_at":"2026-10-23T18:00:22.543169+00:00","publication_info":[{"journal_volume":"114","journal_issue":"7","journal_title":"Physical Review D","material":"other","page_start":"","page_end":"","artid":"","volume_year":"2026","journal_issue_date":null,"publisher":"APS"}],"reception_date":null,"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1103/m91q-kgbw"},{"identifier_type":"arXiv","identifier_value":"2602.23835"}],"subtitle":"","doi":"10.1103/m91q-kgbw","abstract":"<p>Using <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msup><mi>e</mi><mo>+</mo></msup><msup><mi>e</mi><mo>−</mo></msup></math> collision data corresponding to an integrated luminosity of <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mn>44</mn><mtext> </mtext><mtext> </mtext><msup><mi>fb</mi><mrow><mo>−</mo><mn>1</mn></mrow></msup></math> collected with the BESIII detector at the BEPCII Collider, we report the first measurement of Born cross sections and effective form factors for <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msup><mi>e</mi><mo>+</mo></msup><msup><mi>e</mi><mo>−</mo></msup><mo stretchy=\"false\">→</mo><msup><mi mathvariant=\"normal\">Σ</mi><mo>−</mo></msup><msup><mover accent=\"true\"><mi mathvariant=\"normal\">Σ</mi><mo stretchy=\"false\">¯</mo></mover><mo>+</mo></msup></math> at center-of-mass energies between 3.51 and 4.95 GeV. With a fit to the <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msqrt><mi>s</mi></msqrt></math>-dependent dressed cross sections, the decay <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>ψ</mi><mo stretchy=\"false\">(</mo><mn>3770</mn><mo stretchy=\"false\">)</mo><mo stretchy=\"false\">→</mo><msup><mi mathvariant=\"normal\">Σ</mi><mo>−</mo></msup><msup><mover accent=\"true\"><mi mathvariant=\"normal\">Σ</mi><mo stretchy=\"false\">¯</mo></mover><mo>+</mo></msup></math> is observed for the first time with a significance of <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mrow><mn>5.5</mn><mi>σ</mi></mrow></math>, including systematic uncertainties. The corresponding branching fraction is determined to have two solutions, <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mrow><mo stretchy=\"false\">(</mo><mn>2.9</mn><mo>±</mo><mn>0.3</mn><mo stretchy=\"false\">)</mo><mo>×</mo><msup><mrow><mn>10</mn></mrow><mrow><mo>−</mo><mn>4</mn></mrow></msup></mrow></math> and <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mo stretchy=\"false\">(</mo><mn>1.1</mn><mo>±</mo><mn>0.1</mn><mo stretchy=\"false\">)</mo><mo>×</mo><msup><mn>10</mn><mrow><mo>−</mo><mn>4</mn></mrow></msup></math>, where the quoted uncertainties also include systematic uncertainties. Upper limits at the 90% confidence level on the product of the branching fraction and the electronic partial width are provided for other possible charmonium(like) states. The ratios of Born cross sections for the <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi mathvariant=\"normal\">Σ</mi></math> isospin-triplet states are determined and can be used to test the vector-meson-dominance model.</p>","copyright":[{"statement":"Published by the American Physical Society","year":2026,"holder":""}],"authors":[{"first_name":"M.","last_name":"Ablikim","name":"M. Ablikim","affiliations":[{"value":"Institute of High Energy Physics, Beijing 100049, People’s Republic of China","organization":"Institute of High Energy Physics, Beijing 100049, People’s Republic of China","country":{"code":"CN","name":"China"},"ror":"039shy520"}],"orcid":"0000-0002-3935-619X"},{"first_name":"M.N.","last_name":"Achasov","name":"M.N. Achasov","affiliations":[{"value":"Budker Institute of Nuclear Physics SB RAS (BINP), Novosibirsk 630090, Russian Federation","organization":"Budker Institute of Nuclear Physics SB RAS (BINP), Novosibirsk 630090, Russian Federation","country":{"code":"RU","name":"Russia"}}],"orcid":"0000-0002-9400-8622"},{"first_name":"P.","last_name":"Adlarson","name":"P. Adlarson","affiliations":[{"value":"Uppsala University, Box 516, SE-75120 Uppsala, Sweden","organization":"Uppsala University, Box 516, SE-75120 Uppsala, Sweden","country":{"code":"SE","name":"Sweden"},"ror":"048a87296"}],"orcid":"0000-0001-6280-3851"},{"first_name":"X.C.","last_name":"Ai","name":"X.C. Ai","affiliations":[{"value":"Zhengzhou University, Zhengzhou 450001, People’s Republic of China","organization":"Zhengzhou University, Zhengzhou 450001, People’s Republic of China","country":{"code":"CN","name":"China"},"ror":"04tgrpw60"}],"orcid":"0000-0003-3856-2415"},{"first_name":"C.S.","last_name":"Akondi","name":"C.S. Akondi","affiliations":[{"value":"University of Ferrara, I-44122, Ferrara, Italy","organization":"University of Ferrara, I-44122, Ferrara, Italy","country":{"code":"IT","name":"Italy"},"ror":"041zkgm14"},{"value":"INFN Sezione di Ferrara, INFN Sezione di Ferrara, I-44122, Ferrara, Italy","organization":"INFN Sezione di Ferrara, INFN Sezione di Ferrara, I-44122, Ferrara, Italy","country":{"code":"IT","name":"Italy"},"ror":"00zs3y046"}],"orcid":"0000-0001-6303-5217"},{"first_name":"R.","last_name":"Aliberti","name":"R. Aliberti","affiliations":[{"value":"Johannes Gutenberg University of Mainz, Johann-Joachim-Becher-Weg 45, D-55099 Mainz, Germany","organization":"Johannes Gutenberg University of Mainz, Johann-Joachim-Becher-Weg 45, D-55099 Mainz, Germany","country":{"code":"DE","name":"Germany"},"ror":"023b0x485"}],"orcid":"0000-0003-3500-4012"},{"first_name":"A.","last_name":"Amoroso","name":"A. Amoroso","affiliations":[{"value":"INFN, I-10125, Turin, Italy","organization":"INFN, I-10125, Turin, Italy","country":{"code":"IT","name":"Italy"},"ror":"01vj6ck58"},{"value":"University of Turin and INFN, University of Turin, I-10125, Turin, Italy","organization":"University of Turin and INFN, University of Turin, I-10125, Turin, Italy","country":{"code":"IT","name":"Italy"},"ror":"01vj6ck58"}],"orcid":"0000-0002-3095-8610"},{"first_name":"Q.","last_name":"An","name":"Q. An","affiliations":[{"value":"State Key Laboratory of Particle Detection and Electronics, Beijing 100049, Hefei 230026, People’s Republic of China","organization":"State Key Laboratory of Particle Detection and Electronics, Beijing 100049, Hefei 230026, People’s Republic of China","country":{"code":"CN","name":"China"},"ror":"0303gny42"},{"value":"University of Science and Technology of China, Hefei 230026, People’s Republic of China","organization":"University of Science and Technology of China, Hefei 230026, People’s Republic of China","country":{"code":"CN","name":"China"},"ror":"027s68j25"}]},{"first_name":"Y.H.","last_name":"An","name":"Y.H. An","affiliations":[{"value":"Zhengzhou University, Zhengzhou 450001, People’s Republic of China","organization":"Zhengzhou University, Zhengzhou 450001, People’s Republic of China","country":{"code":"CN","name":"China"},"ror":"04tgrpw60"}],"orcid":"0009-0008-3419-0849"},{"first_name":"Y.","last_name":"Bai","name":"Y. Bai","affiliations":[{"value":"Southeast University, Nanjing 211100, People’s Republic of China","organization":"Southeast University, Nanjing 211100, People’s Republic of China","country":{"code":"CN","name":"China"},"ror":"041pakw92"}],"orcid":"0000-0001-6593-5665"},{"first_name":"O.","last_name":"Bakina","name":"O. Bakina","affiliations":[{"value":"Joint Institute for Nuclear Research, 141980 Dubna, Moscow region, Russian Federation","organization":"Joint Institute for Nuclear Research, 141980 Dubna, Moscow region, Russian Federation","country":{"code":"JINR","name":"JINR"}}],"orcid":"0009-0005-0719-7461"},{"first_name":"Y.","last_name":"Ban","name":"Y. Ban","affiliations":[{"value":"Peking University, Beijing 100871, People’s Republic of China","organization":"Peking University, Beijing 100871, People’s Republic of China","country":{"code":"CN","name":"China"},"ror":"035adwg89"}],"orcid":"0000-0002-1912-0374"},{"first_name":"H.R.","last_name":"Bao","name":"H.R. Bao","affiliations":[{"value":"University of Chinese Academy of Sciences, Beijing 100049, People’s Republic of China","organization":"University of Chinese Academy of Sciences, Beijing 100049, People’s Republic of China","country":{"code":"CN","name":"China"},"ror":"05qbk4x57"}],"orcid":"0009-0002-7027-021X"},{"first_name":"X.L.","last_name":"Bao","name":"X.L. Bao","affiliations":[{"value":"North China Electric Power University, Beijing 102206, People’s Republic of China","organization":"North China Electric Power University, Beijing 102206, People’s Republic of China","country":{"code":"CN","name":"China"},"ror":"04qr5t414"}],"orcid":"0009-0000-3355-8359"},{"first_name":"V.","last_name":"Batozskaya","name":"V. Batozskaya","affiliations":[{"value":"Institute of High Energy Physics, Beijing 100049, People’s Republic of China","organization":"Institute of High Energy Physics, Beijing 100049, People’s Republic of China","country":{"code":"CN","name":"China"},"ror":"039shy520"},{"value":"National center for Nuclear Research, Warsaw 02-093, Poland","organization":"National center for Nuclear Research, Warsaw 02-093, Poland","country":{"code":"PL","name":"Poland"}}],"orcid":"0000-0003-1089-9200"},{"first_name":"K.","last_name":"Begzsuren","name":"K. Begzsuren","affiliations":[{"value":"Institute of Physics and Technology, Mongolian Academy of Sciences, Peace Avenue 54B, Ulaanbaatar 13330, Mongolia","organization":"Institute of Physics and Technology, Mongolian Academy of Sciences, Peace Avenue 54B, Ulaanbaatar 13330, Mongolia","country":{"code":"MN","name":"Mongolia"}}]},{"first_name":"N.","last_name":"Berger","name":"N. Berger","affiliations":[{"value":"Johannes Gutenberg University of Mainz, Johann-Joachim-Becher-Weg 45, D-55099 Mainz, Germany","organization":"Johannes Gutenberg University of Mainz, Johann-Joachim-Becher-Weg 45, D-55099 Mainz, Germany","country":{"code":"DE","name":"Germany"},"ror":"023b0x485"}],"orcid":"0000-0002-9659-8507"},{"first_name":"M.","last_name":"Berlowski","name":"M. Berlowski","affiliations":[{"value":"National center for Nuclear Research, Warsaw 02-093, Poland","organization":"National center for Nuclear Research, Warsaw 02-093, Poland","country":{"code":"PL","name":"Poland"}}],"orcid":"0000-0002-0080-6157"},{"first_name":"M.B.","last_name":"Bertani","name":"M.B. 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Zhu","affiliations":[{"value":"Institute of High Energy Physics, Beijing 100049, People’s Republic of China","organization":"Institute of High Energy Physics, Beijing 100049, People’s Republic of China","country":{"code":"CN","name":"China"},"ror":"039shy520"}],"orcid":"0000-0003-2618-0436"},{"first_name":"W.Z.","last_name":"Zhu","name":"W.Z. Zhu","affiliations":[{"value":"Henan Normal University, Xinxiang 453007, People’s Republic of China","organization":"Henan Normal University, Xinxiang 453007, People’s Republic of China","country":{"code":"CN","name":"China"},"ror":"00s13br28"}],"orcid":"0009-0006-8147-6423"},{"first_name":"Y.C.","last_name":"Zhu","name":"Y.C. 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Zhu","affiliations":[{"value":"University of Chinese Academy of Sciences, Beijing 100049, People’s Republic of China","organization":"University of Chinese Academy of Sciences, Beijing 100049, People’s Republic of China","country":{"code":"CN","name":"China"},"ror":"05qbk4x57"},{"value":"Institute of High Energy Physics, Beijing 100049, People’s Republic of China","organization":"Institute of High Energy Physics, Beijing 100049, People’s Republic of China","country":{"code":"CN","name":"China"},"ror":"039shy520"}],"orcid":"0000-0002-6229-5567"},{"first_name":"X.Y.","last_name":"Zhuang","name":"X.Y. Zhuang","affiliations":[{"value":"Nankai University, Tianjin 300071, People’s Republic of China","organization":"Nankai University, Tianjin 300071, People’s Republic of China","country":{"code":"CN","name":"China"},"ror":"00hq79z10"}],"orcid":"0009-0004-8990-7895"},{"first_name":"J.H.","last_name":"Zou","name":"J.H. Zou","affiliations":[{"value":"Institute of High Energy Physics, Beijing 100049, People’s Republic of China","organization":"Institute of High Energy Physics, Beijing 100049, People’s Republic of China","country":{"code":"CN","name":"China"},"ror":"039shy520"}],"orcid":"0000-0003-3581-2829"}],"countries":["KR","PK","CN","SE","IT","TH","RU","JINR","DE","MN","TR","GB","CL","IN","US","PL"],"article_arxiv_category":[{"category":"hep-ex","primary":true}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/m91q-kgbw/m91q-kgbw.pdf","created":"2026-10-23T18:01:03.171696+00:00","updated":"2026-10-23T18:01:03.171707+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/m91q-kgbw/m91q-kgbw.xml","created":"2026-10-23T18:01:03.180372+00:00","updated":"2026-10-23T18:01:03.180381+00:00"}],"related_materials":[],"first_online_date":null,"title":"Measurement of Born cross sections for <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mrow><msup><mrow><mi>e</mi></mrow><mrow><mo>+</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo>−</mo></mrow></msup><mo>→</mo><msup><mrow><mi mathvariant=\"normal\">Σ</mi></mrow><mrow><mo>−</mo></mrow></msup><msup><mrow><mover accent=\"true\"><mrow><mi mathvariant=\"normal\">Σ</mi></mrow><mrow><mo stretchy=\"false\">¯</mo></mrow></mover></mrow><mrow><mo>+</mo></mrow></msup></mrow></math> at <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mrow><msqrt><mrow><mi>s</mi></mrow></msqrt><mo>=</mo><mn>3.51</mn><mtext> </mtext><mi>–</mi><mtext> </mtext><mn>4.95</mn><mtext> </mtext><mtext> </mtext><mi>GeV</mi></mrow></math> and observation of <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mrow><mi>ψ</mi><mo stretchy=\"false\">(</mo><mn>3770</mn><mo stretchy=\"false\">)</mo><mo stretchy=\"false\">→</mo><msup><mrow><mi mathvariant=\"normal\">Σ</mi></mrow><mrow><mo>−</mo></mrow></msup><msup><mrow><mover accent=\"true\"><mrow><mi mathvariant=\"normal\">Σ</mi></mrow><mrow><mo stretchy=\"false\">¯</mo></mrow></mover></mrow><mrow><mo>+</mo></mrow></msup></mrow></math>"},{"related_licenses":[{"url":"http://creativecommons.org/licenses/by/4.0/","name":"CC-BY-4.0"}],"publication_date":"2026-10-23","acceptance_date":null,"id":112403,"_updated_at":"2026-10-24T00:00:50.017001+00:00","_created_at":"2026-10-23T18:00:22.478687+00:00","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"}],"reception_date":null,"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1103/7tk3-33s9"},{"identifier_type":"arXiv","identifier_value":"2602.21177"}],"subtitle":"","doi":"10.1103/7tk3-33s9","abstract":"<p>The dual-phase xenon time projection chamber (TPC) is a powerful technology to detect rare interactions such as scatters of dark matter particles on nuclei. In particular, the built-in gain of ionization signals in a dual-phase TPC makes it sensitive to events in the few-electron regime, as expected from low-mass dark matter interactions. The pursuit of this low-energy sensitivity through ionization-only signal detection has so far been hindered by excessive electron backgrounds observed across experiments. Much of this background is attributed to the plate-out of <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mrow><mmultiscripts><mrow><mi>Rn</mi></mrow><mprescripts></mprescripts><none></none><mrow><mn>222</mn></mrow></mmultiscripts></mrow></math> decay chain isotopes on the high-voltage electrode grid surfaces that span the full cross section of the TPC. This work presents a first-principles model constructed for this background, the predictions of which are consistent with data from the LZ and LUX experiments. We then discuss strategies to mitigate this background in future dual-phase TPCs and the possibility of applying this grid background model to ionization-only dark matter searches.</p>","copyright":[{"statement":"Published by the American Physical Society","year":2026,"holder":""}],"authors":[{"first_name":"D.S.","last_name":"Akerib","name":"D.S. Akerib","affiliations":[{"value":"SLAC National Accelerator Laboratory, Menlo Park, California 94025-7015, USA","organization":"SLAC National Accelerator Laboratory, Menlo Park, California 94025-7015, USA","country":{"code":"US","name":"United States"}},{"value":"Kavli Institute for Particle Astrophysics and Cosmology, Stanford University, Stanford, California 94305-4085, USA","organization":"Kavli Institute for Particle Astrophysics and Cosmology, Stanford University, Stanford, California 94305-4085, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"A.K.","last_name":"Al Musalhi","name":"A.K. Al Musalhi","affiliations":[{"value":"University College London (UCL), Department of Physics and Astronomy, London WC1E 6BT, United Kingdom","organization":"University College London (UCL), Department of Physics and Astronomy, London WC1E 6BT, United Kingdom","country":{"code":"GB","name":"United Kingdom"}}]},{"first_name":"F.","last_name":"Alder","name":"F. Alder","affiliations":[{"value":"University College London (UCL), Department of Physics and Astronomy, London WC1E 6BT, United Kingdom","organization":"University College London (UCL), Department of Physics and Astronomy, London WC1E 6BT, United Kingdom","country":{"code":"GB","name":"United Kingdom"}}]},{"first_name":"B.J.","last_name":"Almquist","name":"B.J. Almquist","affiliations":[{"value":"Brown University, Department of Physics, Providence, Rhode Island 02912-9037, USA","organization":"Brown University, Department of Physics, Providence, Rhode Island 02912-9037, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"S.","last_name":"Alsum","name":"S. Alsum","affiliations":[{"value":"University of Wisconsin–Madison, Department of Physics, Madison, Wisconsin 53706-1390, USA","organization":"University of Wisconsin–Madison, Department of Physics, Madison, Wisconsin 53706-1390, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"C.S.","last_name":"Amarasinghe","name":"C.S. Amarasinghe","affiliations":[{"value":"University of California, Santa Barbara, Department of Physics, Santa Barbara, California 93106-9530, USA","organization":"University of California, Santa Barbara, Department of Physics, Santa Barbara, California 93106-9530, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"A.","last_name":"Ames","name":"A. Ames","affiliations":[{"value":"SLAC National Accelerator Laboratory, Menlo Park, California 94025-7015, USA","organization":"SLAC National Accelerator Laboratory, Menlo Park, California 94025-7015, USA","country":{"code":"US","name":"United States"}},{"value":"Kavli Institute for Particle Astrophysics and Cosmology, Stanford University, Stanford, California 94305-4085, USA","organization":"Kavli Institute for Particle Astrophysics and Cosmology, Stanford University, Stanford, California 94305-4085, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"T.J.","last_name":"Anderson","name":"T.J. Anderson","affiliations":[{"value":"SLAC National Accelerator Laboratory, Menlo Park, California 94025-7015, USA","organization":"SLAC National Accelerator Laboratory, Menlo Park, California 94025-7015, USA","country":{"code":"US","name":"United States"}},{"value":"Kavli Institute for Particle Astrophysics and Cosmology, Stanford University, Stanford, California 94305-4085, USA","organization":"Kavli Institute for Particle Astrophysics and Cosmology, Stanford University, Stanford, California 94305-4085, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"N.","last_name":"Angelides","name":"N. Angelides","affiliations":[{"value":"Imperial College London, Physics Department, Blackett Laboratory, London SW7 2AZ, United Kingdom","organization":"Imperial College London, Physics Department, Blackett Laboratory, London SW7 2AZ, United Kingdom","country":{"code":"GB","name":"United Kingdom"}}]},{"first_name":"H.M.","last_name":"Araújo","name":"H.M. Araújo","affiliations":[{"value":"Imperial College London, Physics Department, Blackett Laboratory, London SW7 2AZ, United Kingdom","organization":"Imperial College London, Physics Department, Blackett Laboratory, London SW7 2AZ, United Kingdom","country":{"code":"GB","name":"United Kingdom"}}]},{"first_name":"J.E.","last_name":"Armstrong","name":"J.E. Armstrong","affiliations":[{"value":"University of Maryland, Department of Physics, College Park, Maryland 20742-4111, USA","organization":"University of Maryland, Department of Physics, College Park, Maryland 20742-4111, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"M.","last_name":"Arthurs","name":"M. Arthurs","affiliations":[{"value":"SLAC National Accelerator Laboratory, Menlo Park, California 94025-7015, USA","organization":"SLAC National Accelerator Laboratory, Menlo Park, California 94025-7015, USA","country":{"code":"US","name":"United States"}},{"value":"Kavli Institute for Particle Astrophysics and Cosmology, Stanford University, Stanford, California 94305-4085, USA","organization":"Kavli Institute for Particle Astrophysics and Cosmology, Stanford University, Stanford, California 94305-4085, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"X.","last_name":"Bai","name":"X. Bai","affiliations":[{"value":"South Dakota School of Mines and Technology, Rapid City, South Dakota 57701-3901, USA","organization":"South Dakota School of Mines and Technology, Rapid City, South Dakota 57701-3901, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"A.","last_name":"Baker","name":"A. Baker","affiliations":[{"value":"Imperial College London, Physics Department, Blackett Laboratory, London SW7 2AZ, United Kingdom","organization":"Imperial College London, Physics Department, Blackett Laboratory, London SW7 2AZ, United Kingdom","country":{"code":"GB","name":"United Kingdom"}},{"value":"King’s College London, King’s College London, Department of Physics, London WC2R 2LS, United Kingdom","organization":"King’s College London, King’s College London, Department of Physics, London WC2R 2LS, United Kingdom","country":{"code":"GB","name":"United Kingdom"}}]},{"first_name":"J.","last_name":"Balajthy","name":"J. Balajthy","affiliations":[{"value":"University of California, Davis, Department of Physics, Davis, California 95616-5270, USA","organization":"University of California, Davis, Department of Physics, Davis, California 95616-5270, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"S.","last_name":"Balashov","name":"S. Balashov","affiliations":[{"value":"STFC Rutherford Appleton Laboratory (RAL), Didcot, OX11 0QX, United Kingdom","organization":"STFC Rutherford Appleton Laboratory (RAL), Didcot, OX11 0QX, United Kingdom","country":{"code":"GB","name":"United Kingdom"}}]},{"first_name":"J.","last_name":"Bang","name":"J. Bang","affiliations":[{"value":"Brown University, Department of Physics, Providence, Rhode Island 02912-9037, USA","organization":"Brown University, Department of Physics, Providence, Rhode Island 02912-9037, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"J.W.","last_name":"Bargemann","name":"J.W. Bargemann","affiliations":[{"value":"University of California, Santa Barbara, Department of Physics, Santa Barbara, California 93106-9530, USA","organization":"University of California, Santa Barbara, Department of Physics, Santa Barbara, California 93106-9530, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"E.E.","last_name":"Barillier","name":"E.E. Barillier","affiliations":[{"value":"University of Michigan, Randall Laboratory of Physics, Ann Arbor, Michigan 48109-1040, USA","organization":"University of Michigan, Randall Laboratory of Physics, Ann Arbor, Michigan 48109-1040, USA","country":{"code":"US","name":"United States"}},{"value":"University of Zurich, Department of Physics, 8057 Zurich, Switzerland","organization":"University of Zurich, Department of Physics, 8057 Zurich, Switzerland","country":{"code":"CH","name":"Switzerland"}}]},{"first_name":"A.","last_name":"Baxter","name":"A. Baxter","affiliations":[{"value":"University of Liverpool, Department of Physics, Liverpool L69 7ZE, United Kingdom","organization":"University of Liverpool, Department of Physics, Liverpool L69 7ZE, United Kingdom","country":{"code":"GB","name":"United Kingdom"}}]},{"first_name":"K.","last_name":"Beattie","name":"K. Beattie","affiliations":[{"value":"Lawrence Berkeley National Laboratory (LBNL), Berkeley, California 94720-8099, USA","organization":"Lawrence Berkeley National Laboratory (LBNL), Berkeley, California 94720-8099, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"T.","last_name":"Benson","name":"T. Benson","affiliations":[{"value":"University of Wisconsin–Madison, Department of Physics, Madison, Wisconsin 53706-1390, USA","organization":"University of Wisconsin–Madison, Department of Physics, Madison, Wisconsin 53706-1390, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"E.P.","last_name":"Bernard","name":"E.P. Bernard","affiliations":[{"value":"University of California, Berkeley, Department of Physics, Berkeley, California 94720-7300, USA","organization":"University of California, Berkeley, Department of Physics, Berkeley, California 94720-7300, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"A.","last_name":"Bernstein","name":"A. Bernstein","affiliations":[{"value":"<a href=\"https://ror.org/041nk4h53\">Lawrence Livermore National Laboratory (LLNL)</a>, Livermore, California 94550-9698, USA","organization":"Lawrence Livermore National Laboratory (LLNL), Livermore, California 94550-9698, USA","country":{"code":"US","name":"United States"},"ror":"041nk4h53"}]},{"first_name":"A.","last_name":"Bhatti","name":"A. Bhatti","affiliations":[{"value":"University of Maryland, Department of Physics, College Park, Maryland 20742-4111, USA","organization":"University of Maryland, Department of Physics, College Park, Maryland 20742-4111, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"T.P.","last_name":"Biesiadzinski","name":"T.P. Biesiadzinski","affiliations":[{"value":"SLAC National Accelerator Laboratory, Menlo Park, California 94025-7015, USA","organization":"SLAC National Accelerator Laboratory, Menlo Park, California 94025-7015, USA","country":{"code":"US","name":"United States"}},{"value":"Kavli Institute for Particle Astrophysics and Cosmology, Stanford University, Stanford, California 94305-4085, USA","organization":"Kavli Institute for Particle Astrophysics and Cosmology, Stanford University, Stanford, California 94305-4085, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"H.J.","last_name":"Birch","name":"H.J. Birch","affiliations":[{"value":"University of Michigan, Randall Laboratory of Physics, Ann Arbor, Michigan 48109-1040, USA","organization":"University of Michigan, Randall Laboratory of Physics, Ann Arbor, Michigan 48109-1040, USA","country":{"code":"US","name":"United States"}},{"value":"University of Zurich, Department of Physics, 8057 Zurich, Switzerland","organization":"University of Zurich, Department of Physics, 8057 Zurich, Switzerland","country":{"code":"CH","name":"Switzerland"}}]},{"first_name":"E.","last_name":"Bishop","name":"E. Bishop","affiliations":[{"value":"University of Edinburgh, SUPA, School of Physics and Astronomy, Edinburgh EH9 3FD, United Kingdom","organization":"University of Edinburgh, SUPA, School of Physics and Astronomy, Edinburgh EH9 3FD, United Kingdom","country":{"code":"GB","name":"United Kingdom"}}]},{"first_name":"G.M.","last_name":"Blockinger","name":"G.M. Blockinger","affiliations":[{"value":"University at Albany (SUNY), Department of Physics, Albany, New York 12222-0100, USA","organization":"University at Albany (SUNY), Department of Physics, Albany, New York 12222-0100, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"E.M.","last_name":"Boulton","name":"E.M. Boulton","affiliations":[{"value":"University of California, Berkeley, Department of Physics, Berkeley, California 94720-7300, USA","organization":"University of California, Berkeley, Department of Physics, Berkeley, California 94720-7300, USA","country":{"code":"US","name":"United States"}},{"value":"Yale University, Department of Physics, 217 Prospect Street, New Haven, Connecticut 06511, USA","organization":"Yale University, Department of Physics, 217 Prospect Street, New Haven, Connecticut 06511, USA","country":{"code":"US","name":"United States"}}]},{"first_name":"B.","last_name":"Boxer","name":"B. 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