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(LJ212410165019)","acceptance_date":null,"doi":"10.1088/1674-1137/aea108","countries":["CN"],"authors":[{"first_name":"Yi-Qi","last_name":"Mu","name":"Yi-Qi Mu","affiliations":[{"value":"School of Physics and Electronic Technology, Liaoning Normal University, China","organization":"School of Physics and Electronic Technology, Liaoning Normal University","country":{"code":"CN","name":"China"}}]},{"first_name":"Peng-Wen","last_name":"Xu","name":"Peng-Wen Xu","affiliations":[{"value":"School of Physics and Electronic Technology, Liaoning Normal University, China","organization":"School of Physics and Electronic Technology, Liaoning Normal University","country":{"code":"CN","name":"China"}}]},{"first_name":"Si-Tong","last_name":"Chen","name":"Si-Tong Chen","affiliations":[{"value":"School of Physics and Electronic Technology, Liaoning Normal University, China","organization":"School of Physics and Electronic Technology, Liaoning Normal University","country":{"code":"CN","name":"China"}}]},{"first_name":"Yi-Tong","last_name":"Wei","name":"Yi-Tong Wei","affiliations":[{"value":"School of Physics and Electronic Technology, Liaoning Normal University, China","organization":"School of Physics and Electronic Technology, Liaoning Normal University","country":{"code":"CN","name":"China"}}]},{"first_name":"Ge-Jia","last_name":"Zhang","name":"Ge-Jia Zhang","affiliations":[{"value":"School of Physics and Electronic Technology, Liaoning Normal University, China","organization":"School of Physics and Electronic Technology, Liaoning Normal University","country":{"code":"CN","name":"China"}}]},{"first_name":"Bing-Dong","last_name":"Wan","name":"Bing-Dong Wan","affiliations":[{"value":"Center for Theoretical and Experimental High Energy Physics, Liaoning Normal University, China","organization":"Center for Theoretical and Experimental High Energy Physics, Liaoning Normal University","country":{"code":"CN","name":"China"}},{"value":"School of Physics and Electronic Technology, Liaoning Normal University, China","organization":"School of Physics and Electronic Technology, Liaoning Normal University","country":{"code":"CN","name":"China"}}]}],"publication_info":[{"journal_volume":"51","journal_issue":"1","journal_title":"Chinese Physics C","material":"article","page_start":"","page_end":"","artid":"013105","volume_year":"2027","journal_issue_date":null,"publisher":"IOP"}],"subtitle":"","related_materials":[],"abstract":"The nature of the recently observed $K(1690)$ state, reported by the COMPASS Collaboration as a candidate strange crypto-exotic meson with $J^P=0^-$ , remains unclear. In this work, we investigate whether it can be described by local meson-meson currents within the framework of QCD sum rules. We construct a set of independent local color-singlet meson-meson interpolating currents with $J^P=0^-$ and analyze their QCD sum rules. For the currents that admit reliable Borel windows, the extracted effective mass scales are consistently in the range of $2.0-2.3\\;\\mathrm{GeV}$ , significantly above the experimental mass of the $K(1690)$ . Within the standard pole-plus-continuum framework, none of the selected local currents yields a separately resolved low-lying pole compatible with the COMPASS signal. These results indicate that the selected local color-singlet meson-meson currents do not isolate the $K(1690)$ signal within the present framework, while leaving open the possibility of more extended molecular dynamics and other configurations beyond the present analysis.","reception_date":null,"_created_at":"2026-11-13T00:27:12.994899","_updated_at":"2026-11-13T00:27:18.875934+00:00","publication_date":"2027-01-01","id":112995,"copyright":[{"statement":"© 2027 Chinese Physical Society and the Institute of High Energy Physics of the Chinese Academy of Sciences and the Institute of Modern Physics of the Chinese Academy of Sciences and IOP Publishing Ltd","year":2027,"holder":""}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/aea108/cpc_51_1_013105.pdf","created":"2026-11-13T00:27:18.757848+00:00","updated":"2026-11-13T00:27:18.757857+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/aea108/cpc_51_1_013105.xml","created":"2026-11-13T00:27:18.762226+00:00","updated":"2026-11-13T00:27:18.762235+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/3.0/","name":"CC-BY-3.0"}],"article_arxiv_category":[{"category":"hep-ph","primary":true}],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1088/1674-1137/aea108"},{"identifier_type":"arXiv","identifier_value":"2604.20439"}]},{"first_online_date":null,"title":"Measurement of $ \\Xi^-/\\bar{\\Xi}^{+} $ production in jets from $\\textit{Z}$ boson decays using DELPHI open data * Supported by the National Natural Science Foundation of China (12342502). This paper is also supported by the Xiejialin Fund (E65461U2), the Innovation Fund of IHEP (E65451U8) and the Start-up Fund of IHEP (E55156U1)","acceptance_date":null,"doi":"10.1088/1674-1137/aea82b","countries":["CN"],"authors":[{"first_name":"Zhouyue","last_name":"Fan","name":"Zhouyue Fan","affiliations":[{"value":"Institute of High Energy Physics, Chinese Academy of Sciences, China","organization":"Institute of High Energy Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"University of Chinese Academy of Sciences, Chinese Academy of Sciences, China","organization":"University of Chinese Academy of Sciences, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}}]},{"first_name":"Yuzhi","last_name":"Che","name":"Yuzhi Che","affiliations":[{"value":"Institute of High Energy Physics, Chinese Academy of Sciences, China","organization":"Institute of High Energy Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"China Center of Advanced Science and Technology, China","organization":"China Center of Advanced Science and Technology","country":{"code":"CN","name":"China"}}]},{"first_name":"Xinchou","last_name":"Lou","name":"Xinchou Lou","affiliations":[{"value":"Institute of High Energy Physics, Chinese Academy of Sciences, China","organization":"Institute of High Energy Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"Nanjing University, China","organization":"Nanjing University","country":{"code":"CN","name":"China"}},{"value":"University of Chinese Academy of Sciences, Chinese Academy of Sciences, China","organization":"University of Chinese Academy of Sciences, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}}]},{"first_name":"Zhaoru","last_name":"Zhang","name":"Zhaoru Zhang","affiliations":[{"value":"Institute of High Energy Physics, Chinese Academy of Sciences, China","organization":"Institute of High Energy Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}}]},{"first_name":"Jinfei","last_name":"Wu","name":"Jinfei Wu","affiliations":[{"value":"Institute of High Energy Physics, Chinese Academy of Sciences, China","organization":"Institute of High Energy Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}}]},{"first_name":"Gengyuan","last_name":"Zhang","name":"Gengyuan Zhang","affiliations":[{"value":"Institute of High Energy Physics, Chinese Academy of Sciences, China","organization":"Institute of High Energy Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"University of Chinese Academy of Sciences, Chinese Academy of Sciences, China","organization":"University of Chinese Academy of Sciences, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}}]},{"first_name":"Gang","last_name":"Li","name":"Gang Li","affiliations":[{"value":"Institute of High Energy Physics, Chinese Academy of Sciences, China","organization":"Institute of High Energy Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"University of Chinese Academy of Sciences, Chinese Academy of Sciences, China","organization":"University of Chinese Academy of Sciences, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}}]},{"first_name":"Yanping","last_name":"Huang","name":"Yanping Huang","affiliations":[{"value":"Institute of High Energy Physics, Chinese Academy of Sciences, China","organization":"Institute of High Energy Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"University of Chinese Academy of Sciences, Chinese Academy of Sciences, China","organization":"University of Chinese Academy of Sciences, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}}]},{"first_name":"Manqi","last_name":"Ruan","name":"Manqi Ruan","affiliations":[{"value":"Institute of High Energy Physics, Chinese Academy of Sciences, China","organization":"Institute of High Energy Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"University of Chinese Academy of Sciences, Chinese Academy of Sciences, China","organization":"University of Chinese Academy of Sciences, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}}]}],"publication_info":[{"journal_volume":"51","journal_issue":"1","journal_title":"Chinese Physics C","material":"article","page_start":"","page_end":"","artid":"013002","volume_year":"2027","journal_issue_date":null,"publisher":"IOP"}],"subtitle":"","related_materials":[],"abstract":"The production rates of $ \\Xi^{-}/\\bar{\\Xi}^{+} $ baryons in energy-ranked jets produced from $ Z\\to{\\rm{hadrons}} $ decays are measured using $ 3.2 $ million hadronic $\\textit{Z}$ decay events recorded by the DELPHI experiment. Jets are reconstructed using the Durham algorithm with $ y_{{\\rm{cut}}}=0.005 $ . Quark- and gluon-enriched jet samples are obtained by ranking the jet energies in three-jet events. The softest jet is found to produce fewer $ \\Xi^{-}/\\bar{\\Xi}^{+} $ and less energetic baryons than the other jets. The ratio of $ \\Xi^{-}/\\bar{\\Xi}^{+} $ production rates in gluon and quark jets, each normalized to the corresponding mean charged-particle multiplicity, is measured to be $ 1.21 \\pm 0.18\\; {\\rm{(stat.)}} \\pm 0.26\\; {\\rm{(syst.)}} $ . This result is consistent with the JETSET expectation and the OPAL measurements of $ K_S^0 $ and Λ productions in $\\textit{Z}$ decays. This study presents the first measurement of the gluon-to-quark production ratio for baryons containing two $\\textit{s}$ quarks, providing new insights into strange-quark production and hadronization. Future $ e^{+}e^{-} $ colliders such as CEPC and FCCee will provide much larger $\\textit{Z}$-boson samples and enable far more precise studies of the subject.","reception_date":null,"_created_at":"2026-11-13T00:27:03.310135","_updated_at":"2026-11-13T00:27:09.725125+00:00","publication_date":"2027-01-01","id":112993,"copyright":[{"statement":"© 2027 Chinese Physical Society and the Institute of High Energy Physics of the Chinese Academy of Sciences and the Institute of Modern Physics of the Chinese Academy of Sciences and IOP Publishing Ltd","year":2027,"holder":""}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/aea82b/cpc_51_1_013002.pdf","created":"2026-11-13T00:27:09.472712+00:00","updated":"2026-11-13T00:27:09.472723+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/aea82b/cpc_51_1_013002.xml","created":"2026-11-13T00:27:09.475348+00:00","updated":"2026-11-13T00:27:09.475358+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/3.0/","name":"CC-BY-3.0"}],"article_arxiv_category":[{"category":"hep-ex","primary":true}],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1088/1674-1137/aea82b"},{"identifier_type":"arXiv","identifier_value":"2607.13804"}]},{"first_online_date":null,"title":"Flux estimates and detection prospects for lunar antineutrinos * Supported in part by the National Natural Science Foundation of China (NSFC) (12205018, 12375098, U2541290), the National Key Laboratory of Reliability and Environmental Engineering Technology (WDZC61420040202), and the Strategic Priority Research Program of the Chinese Academy of Sciences (XDA10010100)","acceptance_date":null,"doi":"10.1088/1674-1137/aea82c","countries":["CN"],"authors":[{"first_name":"Hang","last_name":"Hu","name":"Hang Hu","affiliations":[{"value":"Guangdong Ocean University, China","organization":"Guangdong Ocean University","country":{"code":"CN","name":"China"}}]},{"first_name":"Ya-Ping","last_name":"Cheng","name":"Ya-Ping Cheng","affiliations":[{"value":"Beijing Institute of Spacecraft Environment Engineering, China","organization":"Beijing Institute of Spacecraft Environment Engineering","country":{"code":"CN","name":"China"}}]},{"first_name":"Wan-Lei","last_name":"Guo","name":"Wan-Lei Guo","affiliations":[{"value":"Institute of High Energy Physics, Chinese Academy of Sciences, China","organization":"Institute of High Energy Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}}]}],"publication_info":[{"journal_volume":"51","journal_issue":"1","journal_title":"Chinese Physics C","material":"article","page_start":"","page_end":"","artid":"013001","volume_year":"2027","journal_issue_date":null,"publisher":"IOP"}],"subtitle":"","related_materials":[],"abstract":"The distribution of heat-producing elements (U, Th, K) within the Moon is critical for understanding its thermal evolution and formation history. Based on a refined lunar interior model, we calculate the lunar antineutrino fluxes from radioactive decays of these elements at two representative detector locations that bracket the expected signal intensity. The maximum flux is found to be slightly lower than the geoneutrino flux for the KamLAND site on Earth, while the minimum flux is approximately a factor of 9 lower than this maximum value. We also compute the expected event rates for lunar antineutrinos using three detection channels.","reception_date":null,"_created_at":"2026-11-13T00:27:03.103542","_updated_at":"2026-11-13T00:27:09.668410+00:00","publication_date":"2027-01-01","id":112990,"copyright":[{"statement":"© 2027 Chinese Physical Society and the Institute of High Energy Physics of the Chinese Academy of Sciences and the Institute of Modern Physics of the Chinese Academy of Sciences and IOP Publishing Ltd","year":2027,"holder":""}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/aea82c/cpc_51_1_013001.pdf","created":"2026-11-13T00:27:09.315649+00:00","updated":"2026-11-13T00:27:09.315661+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/aea82c/cpc_51_1_013001.xml","created":"2026-11-13T00:27:09.319992+00:00","updated":"2026-11-13T00:27:09.320001+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/3.0/","name":"CC-BY-3.0"}],"article_arxiv_category":[{"category":"hep-ph","primary":true}],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1088/1674-1137/aea82c"},{"identifier_type":"arXiv","identifier_value":"2603.01678"}]},{"first_online_date":null,"title":"Interpreting the 95 GeV di-photon and di-tau excesses in the Georgi–Machacek model * Supported by the National Natural Science Foundation of China (12447167, 12275067), the Joint Fund of Henan Province Science and Technology R&D Program (225200810030, 225200810092 and 225200810014), the Startup Research Fund of Henan Academy of Sciences (231820011), the Basic Research Fund of Henan Academy of Sciences (240620006), the Graduate Innovation Fund of Henan Academy of Sciences (243320031), the National Key R&D Program of China (2023YFA1606000) and the Science and Technology Innovation Leading Talent Support Program of Henan Province (254000510039). PZ is supported by the ARC Discovery Project DP220100007 and the Centre for the Subatomic Structure of Matter (CSSM)","acceptance_date":null,"doi":"10.1088/1674-1137/ae9f36","countries":["AU","CN"],"authors":[{"first_name":"Qin","last_name":"Chang","name":"Qin Chang","affiliations":[{"value":"Center for High Energy Physics, Henan Academy of Sciences, China","organization":"Center for High Energy Physics, Henan Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"Institute of Physics, Henan Academy of Sciences, China","organization":"Institute of Physics, Henan Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"Centre for Theoretical Physics, Henan Normal University, China","organization":"Centre for Theoretical Physics, Henan Normal University","country":{"code":"CN","name":"China"}}]},{"first_name":"Xiaokang","last_name":"Du","name":"Xiaokang Du","affiliations":[{"value":"Institute of Physics, Henan Academy of Sciences, China","organization":"Institute of Physics, Henan Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"Centre for Theoretical Physics, Henan Normal University, China","organization":"Centre for Theoretical Physics, Henan Normal University","country":{"code":"CN","name":"China"}}]},{"first_name":"Pengxuan","last_name":"Zhu","name":"Pengxuan Zhu","affiliations":[{"value":"ARC Centre of Excellence for Dark Matter Particle Physics & CSSM, Department of Physics, Adelaide University, Adelaide, Australia","organization":"ARC Centre of Excellence for Dark Matter Particle Physics & CSSM, Department of Physics, Adelaide University, Adelaide","country":{"code":"AU","name":"Australia"}}]}],"publication_info":[{"journal_volume":"51","journal_issue":"1","journal_title":"Chinese Physics C","material":"article","page_start":"","page_end":"","artid":"013103","volume_year":"2027","journal_issue_date":null,"publisher":"IOP"}],"subtitle":"","related_materials":[],"abstract":"We revisit the 95 GeV $\\gamma\\gamma$ and $\\tau\\tau$ excesses in the Georgi–Machacek model using a combined fit to a single light $\\rm CP$ -even custodial singlet $\\textit{H}$. By combining the one-loop renormalization group-improved effective potential and positive-definiteness conditions for vacuum stability with perturbative unitarity, electroweak precision tests, $\\textit{B}$-physics, and Higgs data, we identify a narrow but viable parameter region. In the allowed region, $\\mu_{\\gamma\\gamma}$ approaches the experimental central value, whereas $\\mu_{\\tau\\tau}$ reaches only $\\sim0.5$ (about $1.4\\sigma$ below the CMS central value) and remains within the $2\\sigma$ interval—providing a good description of the di-photon excess but only a partial accommodation of the di-tau excess. The scenario predicts characteristic patterns in the singlet mixing and triplet vacuum expectation values and is highly testable at the HL-LHC and future lepton colliders through precision $\\kappa_V$ measurements and direct exotic searches.","reception_date":null,"_created_at":"2026-11-13T00:27:02.555595","_updated_at":"2026-11-13T00:27:09.562432+00:00","publication_date":"2027-01-01","id":112992,"copyright":[{"statement":"© 2027 Chinese Physical Society and the Institute of High Energy Physics of the Chinese Academy of Sciences and the Institute of Modern Physics of the Chinese Academy of Sciences and IOP Publishing Ltd","year":2027,"holder":""}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/ae9f36/cpc_51_1_013103.pdf","created":"2026-11-13T00:27:09.477996+00:00","updated":"2026-11-13T00:27:09.478005+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/ae9f36/cpc_51_1_013103.xml","created":"2026-11-13T00:27:09.481190+00:00","updated":"2026-11-13T00:27:09.481200+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/3.0/","name":"CC-BY-3.0"}],"article_arxiv_category":[{"category":"hep-ph","primary":true}],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1088/1674-1137/ae9f36"},{"identifier_type":"arXiv","identifier_value":"2509.26155"}]},{"first_online_date":null,"title":"Production rate of the glueball-like $\\textit{X}$(2370) in $\\textit{J}$/$\\textit{ψ}$ radiative decay * Supported by the National Natural Science Foundation of China (NSFC) (12293060, 12293065, 12175063, 12675103). WS and GL are also supported by the Chinese Academy of Sciences (YSBR-101). GL is also supported by the China Postdoctoral Science Foundation (2025M773362)","acceptance_date":null,"doi":"10.1088/1674-1137/aeaa0f","countries":["CN"],"authors":[{"first_name":"Ying","last_name":"Chen","name":"Ying Chen","affiliations":[{"value":"Institute of High Energy Physics, Chinese Academy of Sciences, China","organization":"Institute of High Energy Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"School of Physical Sciences, University of Chinese Academy of Sciences, China","organization":"School of Physical Sciences, University of Chinese Academy of Sciences","country":{"code":"CN","name":"China"}}]},{"first_name":"Long-Cheng","last_name":"Gui","name":"Long-Cheng Gui","affiliations":[{"value":"Department of Physics, Hunan Normal University, and Key Laboratory of Low-Dimensional Quantum Structures and Quantum Control of Ministry of Education, China","organization":"Department of Physics, Hunan Normal University, and Key Laboratory of Low-Dimensional Quantum Structures and Quantum Control of Ministry of Education","country":{"code":"CN","name":"China"}},{"value":"Synergetic Innovation Center for Quantum Effects and Applications (SICQEA), Hunan Normal University, China","organization":"Synergetic Innovation Center for Quantum Effects and Applications (SICQEA), Hunan Normal University","country":{"code":"CN","name":"China"}}]},{"first_name":"Geng","last_name":"Li","name":"Geng Li","affiliations":[{"value":"Institute of High Energy Physics, Chinese Academy of Sciences, China","organization":"Institute of High Energy Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}}]},{"first_name":"Wei","last_name":"Sun","name":"Wei Sun","affiliations":[{"value":"Institute of High Energy Physics, Chinese Academy of Sciences, China","organization":"Institute of High Energy Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}}]}],"publication_info":[{"journal_volume":"51","journal_issue":"1","journal_title":"Chinese Physics C","material":"article","page_start":"","page_end":"","artid":"011001","volume_year":"2027","journal_issue_date":null,"publisher":"IOP"}],"subtitle":"","related_materials":[],"abstract":"$ X(2370) $ lies in the mass region of the lowest pseudoscalar glueball predicted by lattice quantum chromodynamics (QCD) studies, and its decay properties are similar to those of $ \\eta_c $ . A previous lattice QCD study clearly shows that the pseudoscalar glueball ( $ G_{0^-} $ ) and lowest pseudoscalar charmonium state ( $ c\\bar{c}(0^-) $ ) can mix with a small mixing angle $\\textit{θ}$. Therefore, $ X(2370) $ and $ \\eta_c $ could be admixtures of $ G_{0^-} $ and $ c\\bar{c}(0^-) $ . Although $ {\\rm{Br}}(J/\\psi\\to\\gamma\\eta_c) $ is insensitive to small values of $ \\sin\\theta $ , $ {\\rm{Br}}(J/\\psi\\to \\gamma X(2370)) $ can be greatly enhanced by mixing because of the considerably larger kinematic factor for $ J/\\psi\\to \\gamma X(2370) $ and the substantially larger transition form factor for $ J/\\psi\\to \\gamma (c\\bar{c}(0^{-})) $ . Based on the value of $ \\sin\\theta $ , $ {\\rm{Br}}(J/\\psi\\to \\gamma X(2370)) $ can be considerably larger than the branching fraction for a pure pseudoscalar glueball, namely, $ 2.3(8)\\times 10^{-4} $ , as predicted by a quenched lattice QCD calculation. This amplification mechanism helps explain the large production rate of $ X(2370) $ in $ J/\\psi $ radiative decay, and the BESIII Collaboration results favor a small mixing angle of $ {\\cal{O}}(1^\\circ) $ if the mixing picture applies here.","reception_date":null,"_created_at":"2026-11-13T00:27:03.139997","_updated_at":"2026-11-13T00:27:09.350857+00:00","publication_date":"2027-01-01","id":112989,"copyright":[{"statement":"© 2027 Chinese Physical Society and the Institute of High Energy Physics of the Chinese Academy of Sciences and the Institute of Modern Physics of the Chinese Academy of Sciences and IOP Publishing Ltd","year":2027,"holder":""}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/aeaa0f/cpc_51_1_011001.pdf","created":"2026-11-13T00:27:09.238627+00:00","updated":"2026-11-13T00:27:09.238636+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/aeaa0f/cpc_51_1_011001.xml","created":"2026-11-13T00:27:09.242164+00:00","updated":"2026-11-13T00:27:09.242172+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/3.0/","name":"CC-BY-3.0"}],"article_arxiv_category":[{"category":"hep-ph","primary":true},{"category":"hep-lat","primary":false}],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1088/1674-1137/aeaa0f"},{"identifier_type":"arXiv","identifier_value":"2605.01757"}]},{"first_online_date":null,"title":"Flavor tomography of long-lived neutrino-mass mediators: probing the neutrino mass ordering at the HL-LHC * Supported by the Internal Research Fund of the Institute of High Energy Physics, Chinese Academy of Sciences","acceptance_date":null,"doi":"10.1088/1674-1137/aea53f","countries":["CN"],"authors":[{"first_name":"Renjie","last_name":"Wang","name":"Renjie Wang","affiliations":[{"value":"Institute of High Energy Physics, Chinese Academy of Sciences, China","organization":"Institute of High Energy Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}}]}],"publication_info":[{"journal_volume":"51","journal_issue":"1","journal_title":"Chinese Physics C","material":"article","page_start":"","page_end":"","artid":"011002","volume_year":"2027","journal_issue_date":null,"publisher":"IOP"}],"subtitle":"","related_materials":[],"abstract":"The neutrino mass ordering remains unresolved because long-baseline oscillation measurements are entangled with the unknown CP phase $ \\delta_{\\rm CP} $ ; a collider probe free from this degeneracy would provide a qualitatively distinct and complementary test. We show that, when the long-lived charged particle producing a displaced-lepton signal at the High-Luminosity LHC is also the mediator responsible for Majorana neutrino masses—the $\\textit{shared-coupling condition}$—the Casas–Ibarra parametrization determines the lepton flavor ratio $ N_e/N_\\mu $ of time-delayed leptons solely in terms of Pontecorvo–Maki–Nakagawa–Sakata (PMNS) mixing parameters. Within the resulting $\\textit{shared-coupling class}$ of models, the ratio is fixed by oscillation data and is independent of all beyond-Standard-Model mass and coupling parameters, up to calculable corrections bounded by charged-lepton-flavor-violation data, yielding $ N_e/N_\\mu = 0.140 $ for the Normal and 2.11 for the Inverted Hierarchy—a separation of more than an order of magnitude between the two predictions. This prediction holds identically across the Scotogenic model, the Type-III seesaw, the inverse and linear seesaw, and lepton-portal dark matter, and it is stable against oscillation-parameter uncertainties and detector-efficiency variations, which cancel in the ratio. A single efficiency-corrected decision criterion identifies the hierarchy, and explicit signal-yield estimates combined with an exact Poisson test show that $ {\\cal{O}}(25) $ displaced-lepton events suffice for a $ 3\\sigma $ discrimination with the timing infrastructure already under construction at CMS and ATLAS—so that a positive long-lived-particle signal would simultaneously resolve the mass ordering, with no dependence on $ \\delta_{\\rm CP} $ .","reception_date":null,"_created_at":"2026-11-13T00:27:02.774171","_updated_at":"2026-11-13T00:27:09.234188+00:00","publication_date":"2027-01-01","id":112988,"copyright":[{"statement":"© 2027 Chinese Physical Society and the Institute of High Energy Physics of the Chinese Academy of Sciences and the Institute of Modern Physics of the Chinese Academy of Sciences and IOP Publishing Ltd","year":2027,"holder":""}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/aea53f/cpc_51_1_011002.pdf","created":"2026-11-13T00:27:09.198268+00:00","updated":"2026-11-13T00:27:09.198277+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/aea53f/cpc_51_1_011002.xml","created":"2026-11-13T00:27:09.201508+00:00","updated":"2026-11-13T00:27:09.201516+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/3.0/","name":"CC-BY-3.0"}],"article_arxiv_category":[],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1088/1674-1137/aea53f"}]},{"first_online_date":null,"title":"A high performance partial wave analysis framework for hadron spectroscopy * Supported in part by the National Key R&D Program of China (2025YFA1613900), the National Natural Science Foundation of China (NSFC) (12225509, 12235017), and the Strategic Priority Research Program of the Chinese Academy of Sciences (XDA0480600)","acceptance_date":null,"doi":"10.1088/1674-1137/aeb254","countries":["CN"],"authors":[{"first_name":"Benhou","last_name":"Xiang","name":"Benhou Xiang","affiliations":[{"value":"Institute of High Energy Physics, Chinese Academy of Sciences, China","organization":"Institute of High Energy Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"University of Chinese Academy of Sciences, China","organization":"University of Chinese Academy of Sciences","country":{"code":"CN","name":"China"}}]},{"first_name":"Shuangshi","last_name":"Fang","name":"Shuangshi Fang","affiliations":[{"value":"Institute of High Energy Physics, Chinese Academy of Sciences, China","organization":"Institute of High Energy Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"University of Chinese Academy of Sciences, China","organization":"University of Chinese Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"School of Physics, Henan Normal University, China","organization":"School of Physics, Henan Normal University","country":{"code":"CN","name":"China"}}]},{"first_name":"Beijiang","last_name":"Liu","name":"Beijiang Liu","affiliations":[{"value":"Institute of High Energy Physics, Chinese Academy of Sciences, China","organization":"Institute of High Energy Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"University of Chinese Academy of Sciences, China","organization":"University of Chinese Academy of Sciences","country":{"code":"CN","name":"China"}}]}],"publication_info":[{"journal_volume":"51","journal_issue":"1","journal_title":"Chinese Physics C","material":"article","page_start":"","page_end":"","artid":"013003","volume_year":"2027","journal_issue_date":null,"publisher":"IOP"}],"subtitle":"","related_materials":[],"abstract":"Partial wave analysis (PWA) is a key method in hadron physics for extracting the properties of hadronic resonances. As experimental statistics increase, conventional implementations face substantial challenges in memory usage and computational speed. We present $\\mathrm{CTPWA} $ , a high-performance PWA framework based on the covariant tensor formalism. This framework incorporates extensive precomputation and caching mechanisms, together with fully GPU-based likelihood computation and minimization. These optimizations accelerate fitting by two orders of magnitude relative to autograd-based GPU PWA programs, making high-statistics partial wave analyses feasible in high-precision experiments such as BESIII.","reception_date":null,"_created_at":"2026-11-13T00:27:02.360626","_updated_at":"2026-11-13T00:27:07.699591+00:00","publication_date":"2027-01-01","id":112987,"copyright":[{"statement":"© 2027 Chinese Physical Society and the Institute of High Energy Physics of the Chinese Academy of Sciences and the Institute of Modern Physics of the Chinese Academy of Sciences and IOP Publishing Ltd","year":2027,"holder":""}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/aeb254/cpc_51_1_013003.pdf","created":"2026-11-13T00:27:07.489641+00:00","updated":"2026-11-13T00:27:07.489652+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/aeb254/cpc_51_1_013003.xml","created":"2026-11-13T00:27:07.492829+00:00","updated":"2026-11-13T00:27:07.492838+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/3.0/","name":"CC-BY-3.0"}],"article_arxiv_category":[{"category":"hep-ex","primary":true}],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1088/1674-1137/aeb254"},{"identifier_type":"arXiv","identifier_value":"2608.25963"}]},{"first_online_date":null,"title":"Probing proton structure via physics-guided neural networks in holographic QCD * Supported by the National Natural Science Foundation of China (12547118), the Research Program of State Key Laboratory of Heavy Ion Science and Technology, Institute of Modern Physics, Chinese Academy of Sciences (HIST2025CS08), and the National Key R&D Program of China (2024YFE0109800, 2024YFE0109802)","acceptance_date":null,"doi":"10.1088/1674-1137/aea284","countries":["CN"],"authors":[{"first_name":"Wei","last_name":"Kou","name":"Wei Kou","affiliations":[{"value":"Institute of Modern Physics, Chinese Academy of Sciences, China","organization":"Institute of Modern Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"School of Nuclear Science and Technology, University of Chinese Academy of Sciences, China","organization":"School of Nuclear Science and Technology, University of Chinese Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"State Key Laboratory of Heavy Ion Science and Technology, Institute of Modern Physics, Chinese Academy of Sciences, China","organization":"State Key Laboratory of Heavy Ion Science and Technology, Institute of Modern Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"Southern Center for Nuclear Science Theory (SCNT), Institute of Modern Physics, Chinese Academy of Sciences, China","organization":"Southern Center for Nuclear Science Theory (SCNT), Institute of Modern Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}}]},{"first_name":"Xurong","last_name":"Chen","name":"Xurong Chen","affiliations":[{"value":"Institute of Modern Physics, Chinese Academy of Sciences, China","organization":"Institute of Modern Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"School of Nuclear Science and Technology, University of Chinese Academy of Sciences, China","organization":"School of Nuclear Science and Technology, University of Chinese Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"State Key Laboratory of Heavy Ion Science and Technology, Institute of Modern Physics, Chinese Academy of Sciences, China","organization":"State Key Laboratory of Heavy Ion Science and Technology, Institute of Modern Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}},{"value":"Southern Center for Nuclear Science Theory (SCNT), Institute of Modern Physics, Chinese Academy of Sciences, China","organization":"Southern Center for Nuclear Science Theory (SCNT), Institute of Modern Physics, Chinese Academy of Sciences","country":{"code":"CN","name":"China"}}]}],"publication_info":[{"journal_volume":"51","journal_issue":"1","journal_title":"Chinese Physics C","material":"article","page_start":"","page_end":"","artid":"013104","volume_year":"2027","journal_issue_date":null,"publisher":"IOP"}],"subtitle":"","related_materials":[],"abstract":"Describing the proton structure function $ F_2(x,Q^2) $ across the nonperturbative and transition regimes of quantum chromodynamics remains a significant theoretical challenge. We construct a physics-guided phenomenological representation that combines fermion-resonance and Pomeron-like AdS/QCD basis functions with a neural parametrization. The fermion-resonance sector is constrained by the AdS eigenvalue problem and the physical proton mass, while the neural parametrization describes the effective kinematic mixing, the Pomeron normalization, and a regularized log-space correction. For 187 selected SLAC measurements, a fixed training–test partition containing 153 and 34 points, respectively, yields the point-normalized diagnostics $ \\chi^2/N_{{\\rm{train}}}=0.542 $ , $ \\chi^2/N_{{\\rm{test}}}=1.990 $ , and $ \\chi^2/N_{{\\rm{all}}}=0.805 $ . Conditional on the chosen holographic basis, the fitted channel fractions show a continuous transition from Pomeron-like dominance at the lower end of the measured $\\textit{x}$ range to fermion-resonance dominance at larger $\\textit{x}$. The midpoint of the mixing function occurs at $ x\\simeq0.187 $ , whereas equality of the final channel fractions occurs at $ x\\simeq0.226 $ . These two definitions identify a transition region of approximately $ x\\simeq0.19 $ – $ 0.23 $ , rather than a unique physical boundary. Although $ \\alpha_0\\simeq1.08 $ is compatible with the data, fixed- $ \\alpha_0 $ refits show that it is not separately identifiable from the flexible Pomeron normalization. The $\\textit{x}$-dependent holographic coordinates and associated effective excited scales should therefore be interpreted as basis-dependent effective quantities rather than direct measurements of an $\\textit{x}$-dependent proton spectrum. A comparison with a data-only neural baseline does not establish a predictive advantage for the holographic basis on the present dataset. The resulting framework thus provides a basis-conditioned phenomenological decomposition of the data, rather than a model-independent extraction of the underlying proton dynamics.","reception_date":null,"_created_at":"2026-11-13T00:27:02.011895","_updated_at":"2026-11-13T00:27:07.605603+00:00","publication_date":"2027-01-01","id":112986,"copyright":[{"statement":"© 2027 Chinese Physical Society and the Institute of High Energy Physics of the Chinese Academy of Sciences and the Institute of Modern Physics of the Chinese Academy of Sciences and IOP Publishing Ltd","year":2027,"holder":""}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/aea284/cpc_51_1_013104.pdf","created":"2026-11-13T00:27:07.475361+00:00","updated":"2026-11-13T00:27:07.475372+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/aea284/cpc_51_1_013104.xml","created":"2026-11-13T00:27:07.478446+00:00","updated":"2026-11-13T00:27:07.478455+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/3.0/","name":"CC-BY-3.0"}],"article_arxiv_category":[{"category":"hep-ph","primary":true},{"category":"hep-th","primary":false}],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1088/1674-1137/aea284"},{"identifier_type":"arXiv","identifier_value":"2604.02906"}]},{"first_online_date":null,"title":"Quasinormal frequencies and greybody factors for axial perturbations of dilaton–Euler–Heisenberg de Sitter black holes * This research was supported by the National Natural Science Foundation of China (NNSFC) (12365009), the Natural Science Basic Research Program of Shaanxi Province (2026JC-YBMS-0083), and the Jiangxi Provincial Natural Science Foundation (20262BAC240347)","acceptance_date":null,"doi":"10.1088/1674-1137/ae9e9c","countries":["CN"],"authors":[{"first_name":"Ming","last_name":"Zhang","name":"Ming Zhang","affiliations":[]},{"first_name":"Guo-Xin","last_name":"Chen","name":"Guo-Xin Chen","affiliations":[]},{"first_name":"Xufen","last_name":"Zhang","name":"Xufen Zhang","affiliations":[{"value":"Key Laboratory of Low Dimensional Quantum Structures and Quantum Control of Ministry of Education, Synergetic Innovation Center for Quantum Effects and Applications, and Department of Physics, Hunan Normal University, China","organization":"Key Laboratory of Low Dimensional Quantum Structures and Quantum Control of Ministry of Education, Synergetic Innovation Center for Quantum Effects and Applications, and Department of Physics, Hunan Normal University","country":{"code":"CN","name":"China"}}]},{"first_name":"Cheng-Fu","last_name":"Feng","name":"Cheng-Fu Feng","affiliations":[{"value":"Center for Gravitation and Cosmology, College of Physical Science and Technology, Yangzhou University, China","organization":"Center for Gravitation and Cosmology, College of Physical Science and Technology, Yangzhou University","country":{"code":"CN","name":"China"}}]},{"first_name":"Sheng-Yuan","last_name":"Li","name":"Sheng-Yuan Li","affiliations":[{"value":"Center for Gravitation and Cosmology, College of Physical Science and Technology, Yangzhou University, China","organization":"Center for Gravitation and Cosmology, College of Physical Science and Technology, Yangzhou University","country":{"code":"CN","name":"China"}}]},{"first_name":"Rui-Hong","last_name":"Yue","name":"Rui-Hong Yue","affiliations":[{"value":"Center for Gravitation and Cosmology, College of Physical Science and Technology, Yangzhou University, China","organization":"Center for Gravitation and Cosmology, College of Physical Science and Technology, Yangzhou University","country":{"code":"CN","name":"China"}}]},{"first_name":"De-Cheng","last_name":"Zou","name":"De-Cheng Zou","affiliations":[{"value":"School of Physics, Jiangxi Normal University, China","organization":"School of Physics, Jiangxi Normal University","country":{"code":"CN","name":"China"}}]}],"publication_info":[{"journal_volume":"51","journal_issue":"1","journal_title":"Chinese Physics C","material":"article","page_start":"","page_end":"","artid":"013107","volume_year":"2027","journal_issue_date":null,"publisher":"IOP"}],"subtitle":"","related_materials":[],"abstract":"We investigate the quasinormal modes (QNMs) and greybody factors of dilaton–Euler–Heisenberg (dEH) de Sitter (dS) black holes in string-inspired Euler–Heisenberg gravity. Since the axial gravitational and electromagnetic perturbations decouple, we analyze them independently. By applying the asymptotic iteration method (AIM) together with a sixth-order WKB approximation, we compute the quasinormal frequencies and find excellent agreement between the two methods. We also find that the QNM spectra depend sensitively on the magnetic charge $Q_{\\text{m}}$ , cosmological constant Λ, and nonlinear coupling $\\epsilon$ , with a notable topological anomaly appearing in the electromagnetic frequency trajectories. Additionally, larger values of $Q_{\\text{m}}$ or the multipole number $\\textit{l}$ generally suppress wave transmission, while the electromagnetic sector with $\\epsilon=1$ exhibits an anomalous response.","reception_date":null,"_created_at":"2026-10-27T18:25:40.343073","_updated_at":"2026-10-27T18:25:46.267405+00:00","publication_date":"2027-01-01","id":112536,"copyright":[{"statement":"© 2027 Chinese Physical Society and the Institute of High Energy Physics of the Chinese Academy of Sciences and the Institute of Modern Physics of the Chinese Academy of Sciences and IOP Publishing Ltd","year":2027,"holder":""}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/ae9e9c/cpc_51_1_013107.pdf","created":"2026-10-27T18:25:46.176865+00:00","updated":"2026-10-27T18:25:46.176875+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/ae9e9c/cpc_51_1_013107.xml","created":"2026-10-27T18:25:46.179640+00:00","updated":"2026-10-27T18:25:46.179648+00:00"}],"related_licenses":[{"url":"http://creativecommons.org/licenses/by/3.0/","name":"CC-BY-3.0"}],"article_arxiv_category":[{"category":"hep-th","primary":true},{"category":"gr-qc","primary":false}],"article_identifiers":[{"identifier_type":"DOI","identifier_value":"10.1088/1674-1137/ae9e9c"},{"identifier_type":"arXiv","identifier_value":"2608.15111"}]},{"first_online_date":null,"title":"Perturbative Nicolai-map diagrammatics: application to Poincaré supergravity","acceptance_date":null,"doi":"10.1007/JHEP11(2026)144","countries":["KR","JP"],"authors":[{"first_name":"Ji-Seong","last_name":"Chae","name":"Ji-Seong Chae","affiliations":[{"value":"Department of Physics, Hanyang University, Seoul, 04763, South Korea","organization":"Hanyang University","country":{"code":"KR","name":"South Korea"},"ror":"046865y68"}],"orcid":"0000-0002-1890-496X"},{"first_name":"Hun","last_name":"Jang","name":"Hun Jang","affiliations":[{"value":"Yukawa Institute for Theoretical Physics (YITP), Kyoto University, Kyoto, 606-8502, Japan","organization":"Kyoto University","country":{"code":"JP","name":"Japan"},"ror":"02kpeqv85"},{"value":"Center for Quantum Spacetime (CQUeST), Sogang University, Seoul, 04107, South Korea","organization":"Sogang University","country":{"code":"KR","name":"South Korea"},"ror":"056tn4839"}],"orcid":"0000-0002-9966-0775"},{"first_name":"Junhyeok","last_name":"Lee","name":"Junhyeok Lee","affiliations":[{"value":"Department of Physics, Hanyang University, Seoul, 04763, South Korea","organization":"Hanyang University","country":{"code":"KR","name":"South Korea"},"ror":"046865y68"}],"orcid":"0009-0003-3765-637X"}],"publication_info":[{"journal_volume":"2026","journal_issue":"11","journal_title":"Journal of High Energy Physics","material":"article","page_start":"1","page_end":"77","artid":"JHEP11(2026)144","volume_year":"2026","journal_issue_date":null,"publisher":"Springer"}],"subtitle":"","related_materials":[],"abstract":"We develop a perturbative, diagrammatic framework for constructing Nicolai maps and apply it to four-dimensional $$ \\mathcal{N} $$ = 1 Poincaré supergravity expanded around flat Minkowski space. It provides an alternative to the coupling-flow-operator construction, which faces several obstructions when extended to local supersymmetry. Expanding the bosonic effective action and the Nicolai map jointly in the gravitational coupling $\\textit{κ}$ and the loop-counting parameter ℏ, we derive the Nicolai-map defining conditions, i.e. the free-action and determinant-matching conditions, order by order. The diagrammatics enumerates all admissible local terms in the Nicolai-map ansatz from the effective-action diagrams and reduces the construction to a finite system of nonlinear polynomial equations. Carried through order $\\textit{κ}$ , the resulting constraints are found to be independent of the detailed bosonic input and hierarchical, order-$\\textit{κ}$ consistency further restricting the order-$\\textit{κ}$ data. A consistent Nicolai-map construction for the Einstein-Hilbert graviton sector is found to require the Rarita-Schwinger gravitino already at this order: Einstein gravity admits a Nicolai map only through its $$ \\mathcal{N} $$ = 1 supersymmetric completion, Poincaré supergravity, supporting Nicolai’s characterization of supersymmetry.","reception_date":null,"_created_at":"2026-11-14T12:55:32.387736","_updated_at":"2026-11-14T12:55:38.147318+00:00","publication_date":"2026-11-13","id":113096,"copyright":[{"statement":"","year":2026,"holder":"The Author(s)"}],"related_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP11(2026)144/13130_2026_Article_30588.xml.scoap.xml","created":"2026-11-14T12:55:37.604848+00:00","updated":"2026-11-14T12:55:37.604860+00:00"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP11(2026)144/13130_2026_Article_30588_a.pdf","created":"2026-11-14T12:55:37.617501+00:00","updated":"2026-11-14T12:55:37.617510+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/JHEP11(2026)144"},{"identifier_type":"arXiv","identifier_value":"2605.29990"}]}]}