{"count":82368,"next":"https://repo.scoap3.org/api/records/?page=2&q=higgs","previous":null,"hits":{"hits":[{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/ae3dc0/cpc_50_5_053103.pdf","key":"cpc_50_5_053103","filetype":"pdf"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/ae3dc0/cpc_50_5_053103.xml","key":"cpc_50_5_053103","filetype":"xml"}],"abstracts":[{"source":"IOP","value":"The Schwinger effect, a non-perturbative mechanism for particle production in strong fields, plays a crucial role in understanding quantum vacuum decay and high-energy phenomena, including heavy-ion collisions (HIC). Although holographic quantum chromodynamics (QCD) models have been widely used to study this effect, most treatments assume isotropy or consider only a single type of anisotropy, neglecting the interplay between spatial and magnetic anisotropies that arise in realistic HIC scenarios. A unified framework accounting for both anisotropies is needed to accurately model particle production. We investigate the Schwinger effect in a twice anisotropic holographic QCD model incorporating both spatial and magnetic anisotropies. Using the anti-de Sitter/conformal field theory correspondence, we compute the total potential of a particle-antiparticle pair to quantify how these anisotropies influence pair production. Our results show that the magnetic field (parameterized by $c_B$ and $q_3$ ) enhances the Schwinger effect by lowering and narrowing the potential barrier, while increasing spatial anisotropy (controlled by $\\nu$ ) suppresses the process by raising and widening the barrier. These findings demonstrate that magnetic and spatial anisotropies exert competing effects on particle production, emphasizing the necessity of treating both concurrently in holographic models. This work advances the theoretical description of the Schwinger effect in anisotropic environments, with implications for understanding non-equilibrium dynamics in HIC and other strongly coupled systems."}],"arxiv_eprints":[{"categories":["hep-ph"],"value":["10.1088/1674-1137/ae3dc0","2506.16245"]}],"authors":[{"affiliations":[{"country":"China","organization":"College of Intelligent Systems Science and Engineering, Hubei Minzu University","value":"College of Intelligent Systems Science and Engineering, Hubei Minzu University, China"}],"email":null,"full_name":null,"given_names":"Wen-Bin","surname":"Chang"},{"affiliations":[{"country":"China","organization":"Institute of Particle Physics and Key Laboratory of Quark and Lepton Physics (MOS), Central China Normal University","value":"Institute of Particle Physics and Key Laboratory of Quark and Lepton Physics (MOS), Central China Normal University, China"}],"email":null,"full_name":null,"given_names":"Defu","surname":"Hou"}],"collections":[{"primary":"Chinese Physics C"}],"control_number":106073,"copyright":[{"statement":"© 2026 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","holder":"","year":2026}],"dois":[{"value":"10.1088/1674-1137/ae3dc0"},{"value":"2506.16245"}],"imprints":[{"date":null,"publisher":"IOP"}],"license":[{"license":"CC-BY-3.0","url":"http://creativecommons.org/licenses/by/3.0/"}],"page_nr":[],"publication_info":[{"artid":"053103","journal_issue":"5","journal_title":"Chinese Physics C","journal_volume":"50","page_end":"","page_start":"","year":"2026"}],"record_creation_date":"2026-04-02T12:25:39.013153","titles":[{"source":"IOP","title":"Schwinger effect in a twice anisotropic holographic model * Defu Hou's research is supported in part by the National Key Research and Development Program of China (2022YFA1604900). Additionally, Defu Hou receives partial support from the National Natural Science Foundation of China (NSFC) (12435009, 12275104). Wen-Bin Chang is supported by the Ph.D. Research Startup Project at Hubei Minzu University (RZ2500000857)"}]},"updated":"2026-04-02T12:25:45.161388+00:00","id":106073,"created":"2026-04-02T12:25:39.013153"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/ae3f0b/cpc_50_5_053105.pdf","key":"cpc_50_5_053105","filetype":"pdf"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/ae3f0b/cpc_50_5_053105.xml","key":"cpc_50_5_053105","filetype":"xml"}],"abstracts":[{"source":"IOP","value":"Motivated by the observation of the doubly charmed tetraquark $ T_{cc}(3875)^+ $ , we present a systematic study of doubly heavy tetraquarks ( $ T_{QQ'\\bar{q}\\bar{q}'} $ ) using heavy antiquark-diquark symmetry (HADS) within a constituent quark model. By calibrating model parameters to known hadron spectra and incorporating the effective mass formula, we predict the masses for 38 ground-state tetraquarks with $ cc $ , $ bb $ , and $ bc $ heavy quark pairs, including the non-strange, single-strange, and double-strange configurations with quantum numbers $ J^P = 0^+, 1^+ $ and $ 2^+ $ . Notably, we identify several stable states below the relevant meson-meson thresholds, particularly in the $ bb\\bar{q}\\bar{q}' $ sector. The explicit connection between the doubly heavy tetraquark and the heavy baryon spectra through HADS reduces model dependence and reveals the fundamental systematics in the heavy-quark hadron landscape."}],"arxiv_eprints":[{"categories":["hep-ph"],"value":["10.1088/1674-1137/ae3f0b","2508.07236"]}],"authors":[{"affiliations":[{"country":"China","organization":"School of Science, Shenzhen Campus of Sun Yat-sen University","value":"School of Science, Shenzhen Campus of Sun Yat-sen University, China"}],"email":null,"full_name":null,"given_names":"Liu-Yu","surname":"Zhang"},{"affiliations":[{"country":"China","organization":"School of Science, Shenzhen Campus of Sun Yat-sen University","value":"School of Science, Shenzhen Campus of Sun Yat-sen University, China"}],"email":null,"full_name":null,"given_names":"Tian-Wei","surname":"Wu"},{"affiliations":[{"country":"China","organization":"School of Frontier Sciences, Nanjing University","value":"School of Frontier Sciences, Nanjing University, China"}],"email":null,"full_name":null,"given_names":"Yong-Liang","surname":"Ma"}],"collections":[{"primary":"Chinese Physics C"}],"control_number":106072,"copyright":[{"statement":"© 2026 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","holder":"","year":2026}],"dois":[{"value":"10.1088/1674-1137/ae3f0b"},{"value":"2508.07236"}],"imprints":[{"date":null,"publisher":"IOP"}],"license":[{"license":"CC-BY-3.0","url":"http://creativecommons.org/licenses/by/3.0/"}],"page_nr":[],"publication_info":[{"artid":"053105","journal_issue":"5","journal_title":"Chinese Physics C","journal_volume":"50","page_end":"","page_start":"","year":"2026"}],"record_creation_date":"2026-04-02T12:25:38.734999","titles":[{"source":"IOP","title":"Bridging doubly heavy tetraquark mass spectrum with heavy baryons utilizing heavy antiquark-diquark symmetry * The work of Tian-Wei Wu is supported by the National Natural Science Foundation of China (12405108). Yong-Liang Ma is supported in part by the National Science Foundation of China (NSFC) (12347103) and Gusu Talent Innovation Program (ZXL2024363)"}]},"updated":"2026-04-02T12:25:45.169085+00:00","id":106072,"created":"2026-04-02T12:25:38.734999"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/ae39cc/cpc_50_5_053102.pdf","key":"cpc_50_5_053102","filetype":"pdf"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/ae39cc/cpc_50_5_053102.xml","key":"cpc_50_5_053102","filetype":"xml"}],"abstracts":[{"source":"IOP","value":"The interference between amplitudes corresponding to different intermediate resonances plays an important role in generating large CP asymmetries in the phase space in multi-body decays of bottom and charmed mesons. In this study, we examine the CP violation in the decay channel $ {\\overline{B}}^{0}\\rightarrow K^{-}\\pi^{+}\\pi^{0} $ in the phase-space region where the intermediate resonances $ \\overline{K}^{*}(892)^{0} $ and $ {\\overline{K}^{*}_{0}(700)} $ dominate. In particular, the forward-backward asymmetry (FBA) and the CP asymmetry induced by FBA (FB-CPA), which are closely related to the interference effects between the two aforementioned resonances, are investigated. The nontrivial correlation between FBA and FB-CPA is analyzed. The analysis indicates that FB-CPAs around the resonance $ \\overline{K}^{*}(892)^{0} $ can be as large as approximately 35%, which can be potentially accessible by Belle and Belle-II collaborations in the near future."}],"arxiv_eprints":[{"categories":["hep-ph","hep-ex"],"value":["10.1088/1674-1137/ae39cc","2410.08539"]}],"authors":[{"affiliations":[{"country":"China","organization":"School of Nuclear Science and Technology, University of South China","value":"School of Nuclear Science and Technology, University of South China, China"}],"email":null,"full_name":null,"given_names":"Jian-Yu","surname":"Yang"},{"affiliations":[{"country":"China","organization":"School of Nuclear Science and Technology, University of South China","value":"School of Nuclear Science and Technology, University of South China, China"}],"email":null,"full_name":null,"given_names":"Yu-Jie","surname":"Zhao"},{"affiliations":[{"country":"China","organization":"College of Information and Intelligence Engineering, Zhejiang Wanli University","value":"College of Information and Intelligence Engineering, Zhejiang Wanli University, China"}],"email":null,"full_name":null,"given_names":"Jing-Juan","surname":"Qi"},{"affiliations":[{"country":"China","organization":"School of Nuclear Science and Technology, University of South China","value":"School of Nuclear Science and Technology, University of South China, China"}],"email":null,"full_name":null,"given_names":"Zhen-Hua","surname":"Zhang"}],"collections":[{"primary":"Chinese Physics C"}],"control_number":106074,"copyright":[{"statement":"© 2026 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","holder":"","year":2026}],"dois":[{"value":"10.1088/1674-1137/ae39cc"},{"value":"2410.08539"}],"imprints":[{"date":null,"publisher":"IOP"}],"license":[{"license":"CC-BY-3.0","url":"http://creativecommons.org/licenses/by/3.0/"}],"page_nr":[],"publication_info":[{"artid":"053102","journal_issue":"5","journal_title":"Chinese Physics C","journal_volume":"50","page_end":"","page_start":"","year":"2026"}],"record_creation_date":"2026-04-02T12:25:38.731756","titles":[{"source":"IOP","title":"The forward-backward asymmetry induced CP asymmetry in ${{\\overline{B}}^{0}\\rightarrow K^{-}\\pi^{+}\\pi^{0}}$ in phase space around the resonances ${{\\overline{K}}^{*}(892)^{0}}$ and ${{\\overline{K}}^{*}_{0}(700)}$ * Supported by National Natural Science Foundation of China (12475096, 12405115, 12192261) and Scientific Research Fund of Hunan Provincial Education Department (22A0319)"}]},"updated":"2026-04-02T12:25:45.239515+00:00","id":106074,"created":"2026-04-02T12:25:38.731756"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/ae4325/cpc_50_5_051001.pdf","key":"cpc_50_5_051001","filetype":"pdf"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/ae4325/cpc_50_5_051001.xml","key":"cpc_50_5_051001","filetype":"xml"}],"abstracts":[{"source":"IOP","value":"We investigate the Wigner distributions of gluons at non-zero skewness using light-front wave functions within the dressed quark model, where the target state is a quark dressed with a gluon in the leading-order Fock space expansion. The analyses focus on the configurations wherein the gluon and/or the target are transversely polarized. Subsequently, we derive analytical expressions for the Wigner distributions in the boost-invariant longitudinal space ($\\textit{σ}$) for transversely polarized configurations. Resultantly, a diffraction-like oscillatory pattern is yielded in $\\textit{σ}$-space, which is analogous to that reported previously for unpolarized and longitudinally polarized gluons."}],"arxiv_eprints":[{"categories":[],"value":["10.1088/1674-1137/ae4325"]}],"authors":[{"affiliations":[{"country":"India","organization":"Department of Physics, Sardar Vallabhbhai National Institute of Technology, Surat, 395 007","value":"Department of Physics, Sardar Vallabhbhai National Institute of Technology, Surat, 395 007, India"}],"email":null,"full_name":null,"given_names":"Sujit","surname":"Jana"},{"affiliations":[{"country":"India","organization":"Department of Physics, Sardar Vallabhbhai National Institute of Technology, Surat, 395 007","value":"Department of Physics, Sardar Vallabhbhai National Institute of Technology, Surat, 395 007, India"}],"email":null,"full_name":null,"given_names":"Kenil","surname":"Solanki"},{"affiliations":[{"country":"India","organization":"Department of Physics, Sardar Vallabhbhai National Institute of Technology, Surat, 395 007","value":"Department of Physics, Sardar Vallabhbhai National Institute of Technology, Surat, 395 007, India"}],"email":null,"full_name":null,"given_names":"Vikash","surname":"Kumar Ojha"}],"collections":[{"primary":"Chinese Physics C"}],"control_number":106075,"copyright":[{"statement":"© 2026 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","holder":"","year":2026}],"dois":[{"value":"10.1088/1674-1137/ae4325"}],"imprints":[{"date":null,"publisher":"IOP"}],"license":[{"license":"CC-BY-3.0","url":"http://creativecommons.org/licenses/by/3.0/"}],"page_nr":[],"publication_info":[{"artid":"051001","journal_issue":"5","journal_title":"Chinese Physics C","journal_volume":"50","page_end":"","page_start":"","year":"2026"}],"record_creation_date":"2026-04-02T12:25:39.013213","titles":[{"source":"IOP","title":"Gluon Wigner distributions under transverse polarization at non-zero skewness"}]},"updated":"2026-04-02T12:25:45.413610+00:00","id":106075,"created":"2026-04-02T12:25:39.013213"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/ae3be1/cpc_50_5_053104.pdf","key":"cpc_50_5_053104","filetype":"pdf"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/ae3be1/cpc_50_5_053104.xml","key":"cpc_50_5_053104","filetype":"xml"}],"abstracts":[{"source":"IOP","value":"Investigating the electromagnetic characteristics of unconventional states may offer new insights into their internal structures. In particular, the magnetic moment attributes may serve as a crucial physical observable for differentiating exotic states with disparate configurations or spin-parity quantum numbers. As a promising avenue for research, encompassing both opportunities and challenges, an in-depth examination of the electromagnetic properties of exotic states is crucial for advancing our understanding of unconventional states. Motivated by this, in this study, the magnetic moments of ${I(J^{P})} = 1(1^{+})$ $ Z_{\\bar{b} c} $ tetraquark states are analyzed in the framework of QCD light-cone sum rules by considering the diquark-antidiquark approximation, designated as type $ 3_c \\otimes \\bar{3}_c $ . Although the tetraquark states examined in this study have nearly identical masses, their magnetic moment results exhibit noticeable discrepancies. This may facilitate the differentiation between quantum numbers associated with states with identical quark content. The results show that heavy quarks overcoming light quarks can determine both the sign and magnitude of the magnetic moments of these tetraquark states. The numerical results obtained in this study suggest that the magnetic moments of $ Z_{\\bar{b} c} $ tetraquark states may reveal aspects of their underlying structure, which could distinguish between their spin-parity quantum numbers and internal structure. The results obtained regarding the magnetic moments of the $ Z_{\\bar{b} c} $ tetraquark states may be checked within the context of different phenomenological approaches."}],"arxiv_eprints":[{"categories":["hep-ph","hep-ex","hep-lat"],"value":["10.1088/1674-1137/ae3be1","2411.15508"]}],"authors":[{"affiliations":[],"email":null,"full_name":null,"given_names":"Ulaş","surname":"Özdem"}],"collections":[{"primary":"Chinese Physics C"}],"control_number":106183,"copyright":[{"statement":"© 2026 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","holder":"","year":2026}],"dois":[{"value":"10.1088/1674-1137/ae3be1"},{"value":"2411.15508"}],"imprints":[{"date":null,"publisher":"IOP"}],"license":[{"license":"CC-BY-3.0","url":"http://creativecommons.org/licenses/by/3.0/"}],"page_nr":[],"publication_info":[{"artid":"053104","journal_issue":"5","journal_title":"Chinese Physics C","journal_volume":"50","page_end":"","page_start":"","year":"2026"}],"record_creation_date":"2026-04-07T12:25:29.958231","titles":[{"source":"IOP","title":"Elucidating the nature of axial-vector charm-antibottom tetraquark states"}]},"updated":"2026-04-07T12:25:35.146998+00:00","id":106183,"created":"2026-04-07T12:25:29.958231"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/ae4579/cpc_50_5_053107.pdf","key":"cpc_50_5_053107","filetype":"pdf"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/ae4579/cpc_50_5_053107.xml","key":"cpc_50_5_053107","filetype":"xml"}],"abstracts":[{"source":"IOP","value":"In brane-world scenarios, the effective action of a massless bulk $U(1)$ gauge field preserves gauge invariance via couplings between massive vector Kaluza-Klein (KK) and scalar KK modes. In this study, we extend this framework by introducing the term $(\\nabla^M X_M)^2$ into the massless bulk $U(1)$ gauge action. This modification explicitly breaks full gauge redundancy while preserving residual gauge symmetry both in the bulk and on the brane. In this setup, scalar KK modes can acquire masses from the background geometry. We find that, on the five-dimensional brane, these scalar KK modes are lighter than the vector KK modes. On the six-dimensional brane, two types of scalar modes emerge, and mixed interactions between them give rise to oscillations among these scalar modes."}],"arxiv_eprints":[{"categories":["hep-th"],"value":["10.1088/1674-1137/ae4579","2601.02626"]}],"authors":[{"affiliations":[{"country":"China","organization":"Institute of Modern Physics, Department of Modern Physics and Astronomy, School of Physics, Xi'an Jiaotong University","value":"Institute of Modern Physics, Department of Modern Physics and Astronomy, School of Physics, Xi'an Jiaotong University, China"}],"email":null,"full_name":null,"given_names":"Ye-Hao","surname":"Yang"},{"affiliations":[{"country":"China","organization":"Institute of Modern Physics, Department of Modern Physics and Astronomy, School of Physics, Xi'an Jiaotong University","value":"Institute of Modern Physics, Department of Modern Physics and Astronomy, School of Physics, Xi'an Jiaotong University, China"}],"email":null,"full_name":null,"given_names":"Wen-Xuan","surname":"Ma"},{"affiliations":[{"country":"China","organization":"Institute of Modern Physics, Department of Modern Physics and Astronomy, School of Physics, Xi'an Jiaotong University","value":"Institute of Modern Physics, Department of Modern Physics and Astronomy, School of Physics, Xi'an Jiaotong University, China"}],"email":null,"full_name":null,"given_names":"Chun-E","surname":"Fu"}],"collections":[{"primary":"Chinese Physics C"}],"control_number":106184,"copyright":[{"statement":"© 2026 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","holder":"","year":2026}],"dois":[{"value":"10.1088/1674-1137/ae4579"},{"value":"2601.02626"}],"imprints":[{"date":null,"publisher":"IOP"}],"license":[{"license":"CC-BY-3.0","url":"http://creativecommons.org/licenses/by/3.0/"}],"page_nr":[],"publication_info":[{"artid":"053107","journal_issue":"5","journal_title":"Chinese Physics C","journal_volume":"50","page_end":"","page_start":"","year":"2026"}],"record_creation_date":"2026-04-07T12:25:29.738795","titles":[{"source":"IOP","title":"Massive $\\textit{U}$(1) gauge fields and their accompanying scalars in brane world"}]},"updated":"2026-04-07T12:25:35.189280+00:00","id":106184,"created":"2026-04-07T12:25:29.738795"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/ae4583/cpc_50_5_053106.pdf","key":"cpc_50_5_053106","filetype":"pdf"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1088/1674-1137/ae4583/cpc_50_5_053106.xml","key":"cpc_50_5_053106","filetype":"xml"}],"abstracts":[{"source":"IOP","value":"Within the framework of Dyson-Schwinger equations (DSEs) and by means of the Multiple Reflection Expansion approximation, we study the finite volume effects on the constituent quark mass in a strong external magnetic field. Since the magnetic field influences the coupling constant, which controls the strength of strong interactions in QCD, we adopt the magnetic-field-dependent running coupling constant in our simulations. The results show that, in addition to the magnetic field, the masses of constituent quarks also have a significant dependence on the volume and the running coupling constant. The model behaves closely to the infinite volume limit for large sizes, but the effect of the finite volume is significant when the system size $\\textit{R}$ is about $ 2-6 $ fm. The finite volume effects and the magnetic-field-dependent running coupling constant have considerable influence on the phase transition."}],"arxiv_eprints":[{"categories":["hep-ph"],"value":["10.1088/1674-1137/ae4583","2508.11968"]}],"authors":[{"affiliations":[{"country":"China","organization":"Liuzhou Polytechnic University","value":"Liuzhou Polytechnic University, China"},{"country":"China","organization":"School of Science, Guangxi University of Science and Technology","value":"School of Science, Guangxi University of Science and Technology, China"}],"email":null,"full_name":null,"given_names":"Li-Juan","surname":"Zhou"},{"affiliations":[{"country":"China","organization":"School of Science, Guangxi University of Science and Technology","value":"School of Science, Guangxi University of Science and Technology, China"}],"email":null,"full_name":null,"given_names":"De-Xian","surname":"Wei"},{"affiliations":[{"country":"China","organization":"School of Mathematical Sciences and Statistics, Baise University","value":"School of Mathematical Sciences and Statistics, Baise University, China"}],"email":null,"full_name":null,"given_names":"Zhong-Yi","surname":"Liu"},{"affiliations":[{"country":"China","organization":"School of Science, Guangxi University of Science and Technology","value":"School of Science, Guangxi University of Science and Technology, China"}],"email":null,"full_name":null,"given_names":"Hong-Wei","surname":"Zhong"}],"collections":[{"primary":"Chinese Physics C"}],"control_number":106185,"copyright":[{"statement":"© 2026 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","holder":"","year":2026}],"dois":[{"value":"10.1088/1674-1137/ae4583"},{"value":"2508.11968"}],"imprints":[{"date":null,"publisher":"IOP"}],"license":[{"license":"CC-BY-3.0","url":"http://creativecommons.org/licenses/by/3.0/"}],"page_nr":[],"publication_info":[{"artid":"053106","journal_issue":"5","journal_title":"Chinese Physics C","journal_volume":"50","page_end":"","page_start":"","year":"2026"}],"record_creation_date":"2026-04-07T12:25:29.985351","titles":[{"source":"IOP","title":"Dynamical quark mass and finite volume effects in the Dyson-Schwinger equations * Li-Juan Zhou has been supported by the National Natural Science Foundation of China (11865005), the Natural Science Foundation of Guangxi (China) (2025GXNSFAA069552). De-Xian Wei has been supported by the National Natural Science Foundation of China (12105057), the Natural Science Foundation of Guangxi (China) (2023GXNSFAA026020)"}]},"updated":"2026-04-07T12:25:35.383326+00:00","id":106185,"created":"2026-04-07T12:25:29.985351"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1140/epjc/s10052-026-15606-2/10052_2026_Article_15606.xml.Meta.xml","key":"10052_2026_Article_15606.xml.Meta","filetype":"xml"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1140/epjc/s10052-026-15606-2/10052_2026_Article_15606_a.pdf","key":"10052_2026_Article_15606_a","filetype":"pdf"}],"abstracts":[{"source":"Springer","value":"The $$\\gamma $$ -metric, also known as Zipoy–Voorhees spacetime, is a static, axially symmetric vacuum solution to Einstein’s field equations characterized by two parameters: mass and the deformation parameter $$\\gamma $$ . It reduces to the Schwarzschild metric when $$\\gamma = 1$$ . In this paper, we explore potential signatures of the $$\\gamma $$ -metric on periodic orbits and their gravitational-wave radiation. Periodic orbits are classified by a rotational number specified by three topological numbers ($\\textit{z}$, $\\textit{w}$, $\\textit{v}$), each triple corresponding to characteristic zoom-whirl behavior. We show that deviations from $$\\gamma =1$$ alter the radii and angular momentum of bound orbits and thereby shift the ($\\textit{z}$, $\\textit{w}$, $\\textit{v}$) taxonomy. We also compute representative gravitational waveforms for certain periodic orbits and demonstrate that $$\\gamma \\ne 1$$ can induce phase shifts and amplitude modulations correlated with changes in the zoom–whirl structure. In particular, larger zoom numbers lead to increasingly complex substructures in the waveforms, and finite deviations from $$\\gamma =1$$ can significantly modify these features. Our results indicate that precise measurements of waveform morphology from extreme-mass-ratio inspirals may constrain deviations from spherical symmetry encoded in $$\\gamma $$ ."}],"arxiv_eprints":[{"categories":[],"value":["10.1140/epjc/s10052-026-15606-2"]}],"authors":[{"affiliations":[{"country":"China","organization":"China University of Petroleum-Beijing","value":"Beijing Key Laboratory of Optical Detection Technology for Oil and Gas, China University of Petroleum-Beijing, Beijing, 102249, China"},{"country":"China","organization":"China University of Petroleum-Beijing","value":"Basic Research Center for Energy Interdisciplinary, College of Science, China University of Petroleum-Beijing, Beijing, 102249, China"}],"email":null,"full_name":null,"given_names":"Chao","surname":"Zhang"},{"affiliations":[{"country":"China","organization":"Zhejiang University of Technology","value":"Institute for Theoretical Physics and Cosmology, Zhejiang University of Technology, Hangzhou, 310032, China"},{"country":"China","organization":"Zhejiang University of Technology","value":"United Center for Gravitational Wave Physics (UCGWP), Zhejiang University of Technology, Hangzhou, 310032, China"}],"email":null,"full_name":null,"given_names":"Tao","surname":"Zhu"}],"collections":[{"primary":"European Physical Journal C"}],"control_number":106178,"copyright":[{"statement":"","holder":"The Author(s)","year":2026}],"dois":[{"value":"10.1140/epjc/s10052-026-15606-2"}],"imprints":[{"date":null,"publisher":"Springer"}],"license":[{"license":"CC-BY-4.0","url":"http://creativecommons.org/licenses/by/4.0/"}],"page_nr":[19],"publication_info":[{"artid":"s10052-026-15606-2","journal_issue":"4","journal_title":"European Physical Journal C","journal_volume":"86","page_end":"19","page_start":"1","year":"2026"}],"record_creation_date":"2026-04-07T06:55:36.335902","titles":[{"source":"Springer","title":"Periodic orbits and their gravitational wave radiations in $$\\gamma $$ -metric"}]},"updated":"2026-04-07T06:55:42.685260+00:00","id":106178,"created":"2026-04-07T06:55:36.335902"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1140/epjc/s10052-026-15576-5/10052_2026_Article_15576.xml.Meta.xml","key":"10052_2026_Article_15576.xml.Meta","filetype":"xml"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1140/epjc/s10052-026-15576-5/10052_2026_Article_15576_a.pdf","key":"10052_2026_Article_15576_a","filetype":"pdf"}],"abstracts":[{"source":"Springer","value":"In recent years, the resistive cylindrical chamber (RCC) has been introduced as a novel gaseous detector, extending the well-established resistive plate chambers (RPCs) to the case of cylindrical electrode geometry. Preliminary experimental studies, although still limited in number and performed under experimental conditions not always fully controlled, have nevertheless highlighted several promising features of this detector configuration, motivating the need for further systematic investigations of its operation. In contrast, from the simulation perspective, detailed studies of the RCC have not been performed yet, despite the fact that the cylindrical geometry introduces new degrees of freedom – such as cylinder electrodes radii and voltage polarity – which lead to asymmetric behaviour of the avalanche development according to the polarity of the applied voltage between the electrodes. In this work we present a standalone simulation program specifically designed to model avalanche growth and signal induction in both RPC and RCC geometries. The code implements a stepwise transport model for electron multiplication, includes approximate space-charge effects, and evaluates the induced signals on an external electrode. The simulation has been validated against experimental data for planar RPCs and subsequently applied to RCC geometries with the primary goal of investigating the underlying physical features of the cylindrical detector configuration. The results show that key observables such as induced charge and efficiency are well reproduced in the planar case, and they highlight the role of the electric-field asymmetry in shaping avalanche dynamics in the cylindrical geometry. A first comparison with available RCC experimental data is also presented, providing an initial assessment of the model performance in realistic operating conditions."}],"arxiv_eprints":[{"categories":[],"value":["10.1140/epjc/s10052-026-15576-5"]}],"authors":[{"affiliations":[{"country":"Italy","organization":"INFN Sezione di Bari","value":"INFN Sezione di Bari, Via E. Orabona 4, Bari, 70125, Italy"},{"country":"Italy","organization":"Università degli studi di Bari","value":"Dipartimento Interateneo di Fisica, Università degli studi di Bari, Via Amendola 173, Bari, 70125, Italy"}],"email":null,"full_name":null,"given_names":"M.","surname":"Abbrescia"},{"affiliations":[{"country":"Italy","organization":"INFN, Laboratori Nazionali di Frascati","value":"INFN, Laboratori Nazionali di Frascati, Frascati, 00044, Italy"},{"country":"United States","organization":"James Madison University (JMU)","value":"James Madison University (JMU), Harrisonburg, VA, 22807, USA"}],"email":null,"full_name":null,"given_names":"S.","surname":"Colafranceschi"},{"affiliations":[{"country":"Italy","organization":"INFN Sezione di Bari","value":"INFN Sezione di Bari, Via E. Orabona 4, Bari, 70125, Italy"},{"country":"Italy","organization":"Università degli studi di Bari","value":"Dipartimento Interateneo di Fisica, Università degli studi di Bari, Via Amendola 173, Bari, 70125, Italy"}],"email":null,"full_name":null,"given_names":"M.","surname":"Serio"},{"affiliations":[{"country":"Italy","organization":"INFN, Sezione di Roma Tor Vergata","value":"INFN, Sezione di Roma Tor Vergata, Via della Ricerca Scientifica 1, Rome, 00133, Italy"}],"email":null,"full_name":null,"given_names":"B.","surname":"Liberti"},{"affiliations":[{"country":"Italy","organization":"INFN, Laboratori Nazionali di Frascati","value":"INFN, Laboratori Nazionali di Frascati, Frascati, 00044, Italy"},{"country":"Italy","organization":"Università degli Studi Guglielmo Marconi","value":"Università degli Studi Guglielmo Marconi, Rome, 00193, Italy"}],"email":null,"full_name":null,"given_names":"S.","surname":"Meola"},{"affiliations":[{"country":"Italy","organization":"INFN, Laboratori Nazionali di Frascati","value":"INFN, Laboratori Nazionali di Frascati, Frascati, 00044, Italy"}],"email":null,"full_name":null,"given_names":"A.","surname":"Paoloni"},{"affiliations":[{"country":"Italy","organization":"INFN Sezione di Bari","value":"INFN Sezione di Bari, Via E. Orabona 4, Bari, 70125, Italy"}],"email":null,"full_name":null,"given_names":"A.","surname":"Pastore"},{"affiliations":[{"country":"Italy","organization":"INFN, Laboratori Nazionali di Frascati","value":"INFN, Laboratori Nazionali di Frascati, Frascati, 00044, Italy"}],"email":null,"full_name":null,"given_names":"D.","surname":"Piccolo"},{"affiliations":[{"country":"Italy","organization":"INFN, Laboratori Nazionali di Frascati","value":"INFN, Laboratori Nazionali di Frascati, Frascati, 00044, Italy"},{"country":"Italy","organization":"INFN, Sezione di Roma Tor Vergata","value":"INFN, Sezione di Roma Tor Vergata, Via della Ricerca Scientifica 1, Rome, 00133, Italy"}],"email":null,"full_name":null,"given_names":"A.","surname":"Rocchi"},{"affiliations":[{"country":"Italy","organization":"INFN, Laboratori Nazionali di Frascati","value":"INFN, Laboratori Nazionali di Frascati, Frascati, 00044, Italy"},{"country":"Italy","organization":"Università di Roma La Sapienza","value":"Dipartimento di Ingegneria Chimica Materiali Ambiente, Università di Roma La Sapienza, Via Eudossiana 18, Rome, 00184, Italy"}],"email":null,"full_name":null,"given_names":"G.","surname":"Saviano"},{"affiliations":[{"country":"Italy","organization":"INFN, Laboratori Nazionali di Frascati","value":"INFN, Laboratori Nazionali di Frascati, Frascati, 00044, Italy"},{"country":"Italy","organization":"Università di Roma La Sapienza","value":"Dipartimento di Ingegneria Chimica Materiali Ambiente, Università di Roma La Sapienza, Via Eudossiana 18, Rome, 00184, Italy"}],"email":null,"full_name":null,"given_names":"C.","surname":"Vendittozzi"}],"collections":[{"primary":"European Physical Journal C"}],"control_number":106186,"copyright":[{"statement":"","holder":"The Author(s)","year":2026}],"dois":[{"value":"10.1140/epjc/s10052-026-15576-5"}],"imprints":[{"date":null,"publisher":"Springer"}],"license":[{"license":"CC-BY-4.0","url":"http://creativecommons.org/licenses/by/4.0/"}],"page_nr":[22],"publication_info":[{"artid":"s10052-026-15576-5","journal_issue":"4","journal_title":"European Physical Journal C","journal_volume":"86","page_end":"22","page_start":"1","year":"2026"}],"record_creation_date":"2026-04-07T12:55:24.581100","titles":[{"source":"Springer","title":"A standalone simulation program for resistive cylindrical chamber (RCC)"}]},"updated":"2026-04-07T12:55:29.395261+00:00","id":106186,"created":"2026-04-07T12:55:24.581100"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/rcfs-ynh2/rcfs-ynh2.pdf","key":"rcfs-ynh2","filetype":"pdf"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/rcfs-ynh2/rcfs-ynh2.xml","key":"rcfs-ynh2","filetype":"xml"}],"abstracts":[{"source":"APS","value":"<p>The first four-dimensional amplitude analysis of the <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msup><mi>B</mi><mo>+</mo></msup><mo stretchy=\"false\">→</mo><mi>ψ</mi><mo stretchy=\"false\">(</mo><mn>2</mn><mi>S</mi><mo stretchy=\"false\">)</mo><msubsup><mi>K</mi><mi mathvariant=\"normal\">S</mi><mn>0</mn></msubsup><msup><mi>π</mi><mo>+</mo></msup></math> decay is performed with proton-proton collision data collected by the LHCb experiment at <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>13</mn><mtext> </mtext><mtext> </mtext><mi>TeV</mi></math>, corresponding to an integrated luminosity of <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mrow><mn>5.4</mn><mtext> </mtext><mtext> </mtext><mrow><mi mathvariant=\"normal\">f</mi><msup><mrow><mi mathvariant=\"normal\">b</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup></mrow></mrow></math>. The data cannot be fully explained by <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msup><mi>B</mi><mo>+</mo></msup><mo stretchy=\"false\">→</mo><mi>ψ</mi><mo stretchy=\"false\">(</mo><mn>2</mn><mi>S</mi><mo stretchy=\"false\">)</mo><msup><mi>K</mi><mrow><mo>*</mo><mo>+</mo></mrow></msup></math> contributions alone. A significantly better description of the data is obtained by adding a <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msubsup><mi>T</mi><mrow><mi>c</mi><mover accent=\"true\"><mi>c</mi><mo stretchy=\"false\">¯</mo></mover></mrow><mo>+</mo></msubsup></math> contribution decaying to <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>ψ</mi><mo stretchy=\"false\">(</mo><mn>2</mn><mi>S</mi><mo stretchy=\"false\">)</mo><msup><mi>π</mi><mo>+</mo></msup></math>. The properties of the <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msubsup><mi>T</mi><mrow><mi>c</mi><mover accent=\"true\"><mi>c</mi><mo stretchy=\"false\">¯</mo></mover></mrow><mo>+</mo></msubsup></math> structure are consistent with the exotic state <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msub><mi>T</mi><mrow><mi>c</mi><mover accent=\"true\"><mi>c</mi><mo stretchy=\"false\">¯</mo></mover><mn>1</mn></mrow></msub><mo stretchy=\"false\">(</mo><mn>4430</mn><msup><mo stretchy=\"false\">)</mo><mo>+</mo></msup></math> reported in the isospin-related <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msup><mover accent=\"true\"><mi>B</mi><mo stretchy=\"false\">¯</mo></mover><mn>0</mn></msup><mo stretchy=\"false\">→</mo><mi>ψ</mi><mo stretchy=\"false\">(</mo><mn>2</mn><mi>S</mi><mo stretchy=\"false\">)</mo><msup><mi>K</mi><mo>−</mo></msup><msup><mi>π</mi><mo>+</mo></msup></math> decay. Effects of a possible <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msub><mi>T</mi><mrow><mi>c</mi><mover accent=\"true\"><mi>c</mi><mo stretchy=\"false\">¯</mo></mover><mn>1</mn></mrow></msub><mo stretchy=\"false\">(</mo><mn>4430</mn><msup><mo stretchy=\"false\">)</mo><mo>+</mo></msup><mo stretchy=\"false\">→</mo><msubsup><mover accent=\"true\"><mi>D</mi><mo stretchy=\"false\">¯</mo></mover><mn>1</mn><mo>*</mo></msubsup><mo stretchy=\"false\">(</mo><mn>2600</mn><msup><mo stretchy=\"false\">)</mo><mn>0</mn></msup><msup><mi>D</mi><mo>+</mo></msup></math> decay mode on the <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msub><mi>T</mi><mrow><mi>c</mi><mover accent=\"true\"><mi>c</mi><mo stretchy=\"false\">¯</mo></mover><mn>1</mn></mrow></msub><mo stretchy=\"false\">(</mo><mn>4430</mn><msup><mo stretchy=\"false\">)</mo><mo>+</mo></msup><mo stretchy=\"false\">→</mo><mi>ψ</mi><mo stretchy=\"false\">(</mo><mn>2</mn><mi>S</mi><mo stretchy=\"false\">)</mo><msup><mi>π</mi><mo>+</mo></msup></math> mass distribution are investigated through a Flatté parametrization, providing constraints on the relative decay strength. A description of the <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msub><mi>T</mi><mrow><mi>c</mi><mover accent=\"true\"><mi>c</mi><mo stretchy=\"false\">¯</mo></mover><mn>1</mn></mrow></msub><mo stretchy=\"false\">(</mo><mn>4430</mn><msup><mo stretchy=\"false\">)</mo><mo>+</mo></msup></math> structure using the triangle singularity mechanism is studied and also found to be consistent with the data.</p>"}],"arxiv_eprints":[{"categories":["hep-ex"],"value":["10.1103/rcfs-ynh2","2511.20428"]}],"authors":[{"affiliations":[{"country":"-","organization":"","value":"Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands"}],"email":null,"full_name":null,"given_names":"R.","surname":"Aaij"},{"affiliations":[{"country":"-","organization":"","value":"Department of Physics, University of Warwick, Coventry, United Kingdom"}],"email":null,"full_name":null,"given_names":"A.S.W.","surname":"Abdelmotteleb"},{"affiliations":[{"country":"-","organization":"","value":"Physik-Institut, Universität Zürich, Zürich, Switzerland"}],"email":null,"full_name":null,"given_names":"C.","surname":"Abellan Beteta"},{"affiliations":[{"country":"-","organization":"","value":"Department of Physics, University of Warwick, Coventry, United Kingdom"}],"email":null,"full_name":null,"given_names":"F.","surname":"Abudinén"},{"affiliations":[{"country":"-","organization":"","value":"Oliver Lodge Laboratory, University of Liverpool, Liverpool, United Kingdom"}],"email":null,"full_name":null,"given_names":"T.","surname":"Ackernley"},{"affiliations":[{"country":"-","organization":"","value":"Syracuse University, Syracuse, New York, USA"}],"email":null,"full_name":null,"given_names":"A.A.","surname":"Adefisoye"},{"affiliations":[{"country":"-","organization":"","value":"Instituto Galego de Física de Altas Enerxías (IGFAE), Universidade de Santiago de Compostela, Santiago de Compostela, Spain"}],"email":null,"full_name":null,"given_names":"B.","surname":"Adeva"},{"affiliations":[{"country":"-","organization":"","value":"H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom"}],"email":null,"full_name":null,"given_names":"M.","surname":"Adinolfi"},{"affiliations":[{"country":"-","organization":"","value":"Department of Physics and Astronomy, Uppsala University, Uppsala, Sweden (associated with School of Physics and Astronomy, University of Glasgow, Glasgow, United Kingdom)"}],"email":null,"full_name":null,"given_names":"P.","surname":"Adlarson"},{"affiliations":[{"country":"-","organization":"","value":"Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France"}],"email":null,"full_name":null,"given_names":"C.","surname":"Agapopoulou"},{"affiliations":[{"country":"-","organization":"","value":"University of Michigan, Ann Arbor, Michigan, USA (associated with Syracuse University, Syracuse, New York, USA)"}],"email":null,"full_name":null,"given_names":"C.A.","surname":"Aidala"},{"affiliations":[{"country":"-","organization":"","value":"Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France"}],"email":null,"full_name":null,"given_names":"Z.","surname":"Ajaltouni"},{"affiliations":[{"country":"-","organization":"","value":"Université Clermont Auvergne, CNRS/IN2P3, LPC, Clermont-Ferrand, France"}],"email":null,"full_name":null,"given_names":"S.","surname":"Akar"},{"affiliations":[{"country":"-","organization":"","value":"Nikhef National Institute for Subatomic Physics, Amsterdam, Netherlands"}],"email":null,"full_name":null,"given_names":"K.","surname":"Akiba"},{"affiliations":[{"country":"-","organization":"","value":"AGH - University of Krakow, Faculty of Physics and Applied Computer Science, Kraków, Poland"}],"email":null,"full_name":null,"given_names":"M.","surname":"Akthar"},{"affiliations":[{"country":"-","organization":"","value":"INFN Laboratori Nazionali di Frascati, Frascati, Italy"}],"email":null,"full_name":null,"given_names":"P.","surname":"Albicocco"},{"affiliations":[{"country":"-","organization":"","value":"Fakultät Physik, Technische Universität Dortmund, Dortmund, Germany"}],"email":null,"full_name":null,"given_names":"J.","surname":"Albrecht"},{"affiliations":[{"country":"-","organization":"","value":"Faculty of Physics, Vilnius University, Vilnius, Lithuania (associated with Physikalisches Institut, Albert-Ludwigs-Universität Freiburg, Freiburg, Germany)"}],"email":null,"full_name":null,"given_names":"R.","surname":"Aleksiejunas"},{"affiliations":[{"country":"-","organization":"","value":", Geneva, Switzerland European Organization for Nuclear Research (CERN)"}],"email":null,"full_name":null,"given_names":"F.","surname":"Alessio"},{"affiliations":[{"country":"-","organization":"","value":"Cavendish Laboratory, University of Cambridge, Cambridge, United Kingdom"}],"email":null,"full_name":null,"given_names":"P.","surname":"Alvarez Cartelle"},{"affiliations":[{"country":"-","organization":"","value":"Laboratoire de Physique Nucléaire et de Hautes Énergies (LPNHE), Sorbonne Université, CNRS/IN2P3, F-75005 Paris, France, Paris, France"}],"email":null,"full_name":null,"given_names":"R.","surname":"Amalric"},{"affiliations":[{"country":"-","organization":"","value":"Universidade Federal do Rio de Janeiro (UFRJ), Rio de Janeiro, Brazil"}],"email":null,"full_name":null,"given_names":"S.","surname":"Amato"},{"affiliations":[{"country":"-","organization":"","value":"H.H. Wills Physics Laboratory, University of Bristol, Bristol, United Kingdom"}],"email":null,"full_name":null,"given_names":"J.L.","surname":"Amey"},{"affiliations":[{"country":"-","organization":"","value":"Université Paris-Saclay, CNRS/IN2P3, IJCLab, Orsay, France"}],"email":null,"full_name":null,"given_names":"Y.","surname":"Amhis"},{"affiliations":[{"country":"-","organization":"","value":"School of Physics State Key Laboratory of Nuclear Physics and Technology, Beijing, China Peking University"}],"email":null,"full_name":null,"given_names":"L.","surname":"An"},{"affiliations":[{"country":"-","organization":"","value":"INFN Sezione di Firenze, Firenze, Italy"}],"email":null,"full_name":null,"given_names":"L.","surname":"Anderlini"},{"affiliations":[{"country":"-","organization":"","value":"Physik-Institut, Universität Zürich, Zürich, Switzerland"}],"email":null,"full_name":null,"given_names":"M.","surname":"Andersson"},{"affiliations":[{"country":"-","organization":"","value":"Physik-Institut, Universität Zürich, Zürich, Switzerland"}],"email":null,"full_name":null,"given_names":"P.","surname":"Andreola"},{"affiliations":[{"country":"-","organization":"","value":"INFN Sezione di Ferrara, Ferrara, Italy"}],"email":null,"full_name":null,"given_names":"M.","surname":"Andreotti"},{"affiliations":[{"country":"-","organization":"","value":"Universidade da Coruña, A Coruña, Spain (associated with La Salle, Universitat Ramon Llull, Barcelona, Spain)"}],"email":null,"full_name":null,"given_names":"S.","surname":"Andres Estrada"},{"affiliations":[{"country":"-","organization":"","value":"INFN Sezione di Milano-Bicocca, Milano, Italy"},{"country":"-","organization":"","value":", Geneva, Switzerland European Organization for Nuclear Research (CERN)"}],"email":null,"full_name":null,"given_names":"A.","surname":"Anelli"},{"affiliations":[{"country":"-","organization":"","value":"University of Chinese Academy of Sciences, Beijing, China"}],"email":null,"full_name":null,"given_names":"D.","surname":"Ao"},{"affiliations":[{"country":"-","organization":"","value":"Université Paris-Saclay, Centre d’Etudes de Saclay (CEA), IRFU, Saclay, France, Gif-Sur-Yvette, France"}],"email":null,"full_name":null,"given_names":"C.","surname":"Arata"},{"affiliations":[{"country":"-","organization":"","value":"INFN Sezione di Roma Tor Vergata, Roma, Italy"}],"email":null,"full_name":null,"given_names":"F.","surname":"Archilli"},{"affiliations":[{"country":"-","organization":"","value":"Syracuse University, Syracuse, New York, USA"}],"email":null,"full_name":null,"given_names":"Z.","surname":"Areg"},{"affiliations":[{"country":"-","organization":"","value":"INFN Sezione di Ferrara, Ferrara, Italy"}],"email":null,"full_name":null,"given_names":"M.","surname":"Argenton"},{"affiliations":[{"country":"-","organization":"","value":"Consejo Nacional de Rectores (CONARE), San Jose, Costa Rica"},{"country":"-","organization":"","value":", Geneva, Switzerland European Organization for Nuclear Research (CERN)"}],"email":null,"full_name":null,"given_names":"S.","surname":"Arguedas Cuendis"},{"affiliations":[{"country":"-","organization":"","value":"INFN Sezione di Milano-Bicocca, Milano, Italy"}],"email":null,"full_name":null,"given_names":"L.","surname":"Arnone"},{"affiliations":[{"country":"-","organization":"","value":"Authors affiliated with an institute formerly covered by a cooperation agreement with CERN"}],"email":null,"full_name":null,"given_names":"A.","surname":"Artamonov"},{"affiliations":[{"country":"-","organization":"","value":"Syracuse University, Syracuse, New York, 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