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We investigate the phenomenology of the charged Higgs boson within the two-Higgs-doublet type-II seesaw model (2HDMcT type-III) at future μ+μ− colliders. Focusing on 2→2 processes such as μ+μ−→H1+S− (S−=H1−,H2−) and μ+μ−→H1+W−, we incorporate both theoretical and experimental constraints to assess their production prospects. We find that σ(μ+μ−→H1+H1−) can reach or exceed the corresponding e+e− cross section, while σ(μ+μ−→H1+H2−) is roughly 18 times smaller but can be enhanced up to 0.62 fb upon relaxing electroweak precision observables constraints. Moreover, we observe that the cross section for μ+μ−→H1+W− is significantly enhanced due to the large tanβ amplification characteristic of the type-III scenario. Furthermore, we conduct a signal-background analysis and determine the discovery (5σ) regions at a 3 TeV muon collider for the μ+μ−→H1+H1−, μ+μ−→H1+H2−, and μ+μ−→W±H1∓ processes.

"}],"arxiv_eprints":[{"categories":["hep-ph","hep-th"],"value":["10.1103/3dj6-zg7v","2508.04493"]}],"authors":[{"affiliations":[{"country":"-","organization":"","value":", Faculty of Science Semlalia, LPHEAG, P.O.B. 2390 Marrakech 40000, Morocco Cadi Ayyad University"}],"email":null,"full_name":null,"given_names":"Brahim","surname":"Ait-Ouazghour"},{"affiliations":[{"country":"-","organization":"","value":", FST Tanger B.P. 416, Morocco Abdelmalek Essaadi University"},{"country":"-","organization":"","value":"LAPTh, CNRS, Université Savoie Mont-Blanc, 9 Chemin de Bellevue, 74940, Annecy, France"}],"email":null,"full_name":null,"given_names":"Abdesslam","surname":"Arhrib"},{"affiliations":[{"country":"-","organization":"","value":", Faculty of Science Semlalia, LPHEAG, P.O.B. 2390 Marrakech 40000, Morocco Cadi Ayyad University"},{"country":"-","organization":"","value":", National School of Applied Science, P.O.B. 63 Safi 46000, Morocco Cadi Ayyad University"}],"email":null,"full_name":null,"given_names":"Mohamed","surname":"Chabab"},{"affiliations":[{"country":"-","organization":"","value":", Faculty of Science Semlalia, LPHEAG, P.O.B. 2390 Marrakech 40000, Morocco Cadi Ayyad University"}],"email":null,"full_name":null,"given_names":"Khalid","surname":"Goure"}],"collections":[{"primary":"Physical Review D"}],"control_number":106149,"copyright":[{"statement":"Published by the American Physical Society","holder":"","year":2026}],"dois":[{"value":"10.1103/3dj6-zg7v"},{"value":"2508.04493"}],"imprints":[{"date":null,"publisher":"APS"}],"license":[{"license":"CC-BY-4.0","url":"http://creativecommons.org/licenses/by/4.0/"}],"page_nr":[],"publication_info":[{"artid":"","journal_issue":"7","journal_title":"Physical Review D","journal_volume":"113","page_end":"","page_start":"","year":"2026"}],"record_creation_date":"2026-04-06T18:00:15.913239+00:00","titles":[{"source":"APS","title":"Comprehensive study of the charged Higgs boson in the two Higgs doublet type-II seesaw model"}]},"updated":"2026-04-07T00:01:00.414312+00:00","id":106149,"created":"2026-04-06T18:00:15.913239+00:00"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/6myb-c3g1/6myb-c3g1.pdf","key":"6myb-c3g1","filetype":"pdf"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/6myb-c3g1/6myb-c3g1.xml","key":"6myb-c3g1","filetype":"xml"}],"abstracts":[{"source":"APS","value":"

We present the strongest experimental limits to date on the mixing angle, θ, with which a new scalar particle, S, mixes with the Higgs field in the mass range 110 MeV<mS<155 MeV. This result uses the MicroBooNE liquid argon time projection chamber to search for decays of these Higgs-portal scalar particles through the S→e+e− channel with the decays of kaons in the NuMI neutrino beam acting as the source of the scalar particles. The analysis uses an exposure of 2.01×1021 protons on target of NuMI beam data including periods when the beam focusing system was configured to focus positively charged hadrons and separate periods when negatively charged hadrons were focused. The analysis searches for scalar particles produced from kaons decaying in flight in the beam’s decay volume and at rest in the target and absorber. At mS=125 MeV (mS=150 MeV) we set a limit of θ<3.19×10−4 (θ<2.79×10−4) at the 95% confidence level.

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Measurements of electroweak precision observables are also included and provide complementary constraints to those from the CMS experiment. The CMS measurements, using LHC proton-proton collision data at $$\\sqrt{s}=13\\,\\text {Te}\\text {V} $$ , corresponding to integrated luminosities of 36.3 or 138 $$\\,\\text {fb}^{-1}$$ , are chosen to provide sensitivity to a broad set of operators, for which consistent SMEFT predictions can be derived. These are primarily measurements of differential cross sections which are parameterized as functions of the WCs. In measurements targeting $${\\text {t}} (\\bar{\\textrm{t}})\\text {X} $$ production, SMEFT effects are modelled at the detector level. 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In this paper we show that a modification to Holst gravity induces low-frequency torsion waves of torsional frequency $$\\sim {10^{12}Hz}= 1THz$$ as GWs sourced from astrophysical black holes. Of course, since here we use the almost Riemann-flat manifold approximation, there are no Riemannian GWs as in teleparallel spacetime but only torsionful gravitational waves. This result in Holst gravity allows us to determine an upper bound for the Barbero–Immirzi (BI) parameter as $$\\gamma<<<10^{-58}$$ , which agrees with the BI bound obtained by Aliberti and Lambiase by considering matter–anti-matter asymmetry in Holst gravity. Unfortunately, this very interesting result suffers from the usual torsion ambiguity. To remedy this situation, we proceed with the BI parameter promoted to a field ore BI scalarization. Again we find a BI parameter with a bound of $$10^{-58}$$ from a terahertz-frequency torsion wave. The BI parameter is promoted to a field, and with specific approximation one obtains a BI wave equation with a plane wave solution, similar to those obtained by Taveras and Yunes. From this wave equation constant the BI parameter implies zero torsion, and consequently general relativity (GR), but the converse is not true. Higgs field variation is regarded as responsible for massive torsion. This comes from an analogy between the Higgs field and BI scalar."}],"arxiv_eprints":[{"categories":[],"value":["10.1140/epjc/s10052-026-15388-7"]}],"authors":[{"affiliations":[{"country":"Brazil","organization":"IF-UERJ","value":"Departamento de Física Teórica, IF-UERJ, Rua São Francisco Xavier 524, Maracanã, Rio de Janeiro, RJ, 20550, Brazil"},{"country":"Croatia","organization":"Institute of Cosmology and Philosophy of Nature","value":"Institute of Cosmology and Philosophy of Nature, Krizževci, Croatia"},{"country":"China","organization":"Radioastronomy and technology LAB of Tianjin observary","value":"Radioastronomy and technology LAB of Tianjin observary, street of science 1 #150, urumqi city, People’s Republic of China"}],"email":null,"full_name":null,"given_names":"L.","surname":"Andrade"},{"affiliations":[{"country":"China","organization":"Astronomical Observatory of Chinese Academy of Sciences","value":"Astronomical Observatory of Chinese Academy of Sciences, Chaoyang, 100107, China"}],"email":null,"full_name":null,"given_names":"Zhi-fu","surname":"Gao"}],"collections":[{"primary":"European Physical Journal C"}],"control_number":106029,"copyright":[{"statement":"","holder":"The Author(s)","year":2026}],"dois":[{"value":"10.1140/epjc/s10052-026-15388-7"}],"imprints":[{"date":null,"publisher":"Springer"}],"license":[{"license":"CC-BY-4.0","url":"http://creativecommons.org/licenses/by/4.0/"}],"page_nr":[8],"publication_info":[{"artid":"s10052-026-15388-7","journal_issue":"3","journal_title":"European Physical Journal C","journal_volume":"86","page_end":"8","page_start":"1","year":"2026"}],"record_creation_date":"2026-03-31T18:55:44.336152","titles":[{"source":"Springer","title":"Torsion mass generation induced by Einstein–Cartan gravity with a Barbero–Immirzi Higgs field analogue"}]},"updated":"2026-03-31T18:55:50.469503+00:00","id":106029,"created":"2026-03-31T18:55:44.336152"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP03(2026)261/13130_2026_Article_28568.xml.scoap.xml","key":"13130_2026_Article_28568.xml.scoap","filetype":"xml"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP03(2026)261/13130_2026_Article_28568_a.pdf","key":"13130_2026_Article_28568_a","filetype":"pdf"}],"abstracts":[{"source":"Springer","value":"Using two benchmark models containing extended scalar sectors beyond the Standard Model, we study deep learning techniques to enhance the sensitivity of resonant triple Higgs boson searches in the fully hadronic 6$\\textit{b}$ channel, which suffers from the combinatorial challenge of reconstructing the Higgs bosons correctly from the multiple $\\textit{b}$-jets. More specifically, we employ the framework of Symmetry Preserving Attention Network (S -N ), which takes into account the permutational symmetry when a correct pairing of $\\textit{b}$-jets is achieved, to tackle both jet pairing and event classification. Significantly improved efficiency is achieved in signal and background discrimination. When comparing with the conventional Dense Neural Networks, S -N results in up to 40% more stringent limits on resonant production cross-sections. These results highlight the potential of using advanced machine learning techniques to significantly improve the sensitivity of triple Higgs boson searches in the fully hadronic channel."}],"arxiv_eprints":[{"categories":["hep-ph","hep-ex"],"value":["10.1007/JHEP03(2026)261","2510.01672"]}],"authors":[{"affiliations":[{"country":"Taiwan","organization":"National Taiwan University","value":"Department of Physics, National Taiwan University, Taipei, 10617, Taiwan"},{"country":"Taiwan","organization":"Physics Division, National Center for Theoretical Sciences","value":"Physics Division, National Center for Theoretical Sciences, Taipei, 10617, Taiwan"}],"email":null,"full_name":null,"given_names":"Cheng-Wei","surname":"Chiang"},{"affiliations":[{"country":"Taiwan","organization":"National Taiwan University","value":"Department of Physics, National Taiwan University, Taipei, 10617, Taiwan"}],"email":null,"full_name":null,"given_names":"Feng-Yang","surname":"Hsieh"},{"affiliations":[{"country":"United States","organization":"University of Washington","value":"Department of Physics, University of Washington, Seattle, WA, 98195, USA"}],"email":null,"full_name":null,"given_names":"Shih-Chieh","surname":"Hsu"},{"affiliations":[{"country":"United States","organization":"Northwestern University","value":"Department of Physics and Astronomy, Northwestern University, Evanston, IL, 60208, USA"}],"email":null,"full_name":null,"given_names":"Zhi-Zhong","surname":"Li"},{"affiliations":[{"country":"United States","organization":"Northwestern University","value":"Department of Physics and Astronomy, Northwestern University, Evanston, IL, 60208, USA"},{"country":"United States","organization":"Argonne National Laboratory","value":"High Energy Physics Division, Argonne National Laboratory, Lemont, IL, 60439, USA"}],"email":null,"full_name":null,"given_names":"Ian","surname":"Low"}],"collections":[{"primary":"Journal of High Energy Physics"}],"control_number":105970,"copyright":[{"statement":"","holder":"The Author(s)","year":2026}],"dois":[{"value":"10.1007/JHEP03(2026)261"},{"value":"2510.01672"}],"imprints":[{"date":null,"publisher":"Springer"}],"license":[{"license":"CC-BY-4.0","url":"http://creativecommons.org/licenses/by/4.0/"}],"page_nr":[21],"publication_info":[{"artid":"JHEP03(2026)261","journal_issue":"3","journal_title":"Journal of High Energy Physics","journal_volume":"2026","page_end":"21","page_start":"1","year":"2026"}],"record_creation_date":"2026-03-28T00:55:41.733875","titles":[{"source":"Springer","title":"Enhancing the sensitivity for triple Higgs boson searches with deep learning techniques"}]},"updated":"2026-03-28T00:55:48.036821+00:00","id":105970,"created":"2026-03-28T00:55:41.733875"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP03(2026)260/13130_2026_Article_28567.xml.scoap.xml","key":"13130_2026_Article_28567.xml.scoap","filetype":"xml"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP03(2026)260/13130_2026_Article_28567_a.pdf","key":"13130_2026_Article_28567_a","filetype":"pdf"}],"abstracts":[{"source":"Springer","value":"In this paper, we propose two novel signatures of Higgs decays to search for electron-muon flavor violation. These signatures arise from the presence of a light pseudoscalar into which the 125-GeV Higgs boson decays. The pseudoscalar subsequently decays into an electron-muon pair, leading to multilepton final states, which are relatively clean signatures to search for at the LHC. As a benchmark, we consider the type-III Two-Higgs-doublet-model. We analyze both low-energy and collider constraints on the model and identify regions of parameter space where the light pseudoscalar is viable. Our proposed signatures yield stronger constraints on the lepton flavor violating couplings than current low-energy precision measurements. Taken together, our findings suggest that collider-based probes of exotic Higgs decays provide a powerful complement to precision experiments in the quest to uncover new physics."}],"arxiv_eprints":[{"categories":["hep-ph"],"value":["10.1007/JHEP03(2026)260","2508.20932"]}],"authors":[{"affiliations":[{"country":"Thailand","organization":"Srinakharinwirot University","value":"Department of Physics, Srinakharinwirot University, 114 Sukhumvit 23rd Rd., Wattana, Bangkok, 10110, Thailand"}],"email":null,"full_name":null,"given_names":"P.","surname":"Uttayarat"},{"affiliations":[{"country":"Indonesia","organization":"National Research and Innovation Agency","value":"National Research and Innovation Agency, KST B. J. Habibie, South Tangerang, 15314, Indonesia"}],"email":null,"full_name":null,"given_names":"J.","surname":"Julio"},{"affiliations":[{"country":"Indonesia","organization":"Parahyangan Catholic University","value":"Center for Theoretical Physics, Department of Physics, Parahyangan Catholic University, Jl. Ciumbuleuit 94, Bandung, 40141, Indonesia"}],"email":null,"full_name":null,"given_names":"R.","surname":"Primulando"}],"collections":[{"primary":"Journal of High Energy Physics"}],"control_number":105975,"copyright":[{"statement":"","holder":"The Author(s)","year":2026}],"dois":[{"value":"10.1007/JHEP03(2026)260"},{"value":"2508.20932"}],"imprints":[{"date":null,"publisher":"Springer"}],"license":[{"license":"CC-BY-4.0","url":"http://creativecommons.org/licenses/by/4.0/"}],"page_nr":[21],"publication_info":[{"artid":"JHEP03(2026)260","journal_issue":"3","journal_title":"Journal of High Energy Physics","journal_volume":"2026","page_end":"21","page_start":"1","year":"2026"}],"record_creation_date":"2026-03-28T00:55:41.511826","titles":[{"source":"Springer","title":"Novel probes for electron-muon flavor violation from exotic Higgs decays"}]},"updated":"2026-03-28T00:55:48.206774+00:00","id":105975,"created":"2026-03-28T00:55:41.511826"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/5ssz-3nh7/5ssz-3nh7.pdf","key":"5ssz-3nh7","filetype":"pdf"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/5ssz-3nh7/5ssz-3nh7.xml","key":"5ssz-3nh7","filetype":"xml"}],"abstracts":[{"source":"APS","value":"

In this Letter, I quantify the effects of varying the top Yukawa coupling in the process of the production of three Higgs bosons at the LHC. Modifications of the coupling within experimentally observed ranges have a sizeable impact on the total cross section, but they do not have large effects on the distributions of the invariant mass of the three-Higgs system and other global observables.

"}],"arxiv_eprints":[{"categories":["hep-ph"],"value":["10.1103/5ssz-3nh7","2512.03003"]}],"authors":[{"affiliations":[{"country":"Italy","organization":"Dipartimento di Fisica, Università della Calabria, I-87036 Arcavacata di Rende, Cosenza, Italy and INFN-Cosenza, I-87036 Arcavacata di Rende, Cosenza, Italy","value":"Dipartimento di Fisica, Università della Calabria, I-87036 Arcavacata di Rende, Cosenza, Italy and INFN-Cosenza, I-87036 Arcavacata di Rende, Cosenza, Italy"}],"email":null,"full_name":null,"given_names":"Luca","surname":"Panizzi"}],"collections":[{"primary":"Physical Review D"}],"control_number":105890,"copyright":[{"statement":"Published by the American Physical Society","holder":"","year":2026}],"dois":[{"value":"10.1103/5ssz-3nh7"},{"value":"2512.03003"}],"imprints":[{"date":null,"publisher":"APS"}],"license":[{"license":"CC-BY-4.0","url":"http://creativecommons.org/licenses/by/4.0/"}],"page_nr":[],"publication_info":[{"artid":"","journal_issue":"5","journal_title":"Physical Review D","journal_volume":"113","page_end":"","page_start":"","year":"2026"}],"record_creation_date":"2026-03-25T18:00:50.644093+00:00","titles":[{"source":"APS","title":"Role of the top Yukawa coupling in triple Higgs production at the LHC"}]},"updated":"2026-03-26T00:12:12.107531+00:00","id":105890,"created":"2026-03-25T18:00:50.644093+00:00"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/t865-lq98/t865-lq98.pdf","key":"t865-lq98","filetype":"pdf"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/t865-lq98/t865-lq98.xml","key":"t865-lq98","filetype":"xml"}],"abstracts":[{"source":"APS","value":"

This study investigates the excesses observed around 95 GeV in diphoton and bb¯ experiments within the framework of the left-right supersymmetric model (LRSSM). Considering the one- and two-loop effective potential corrections to the Higgs masses, the model is able to describe the experimentally observed μ(h95)γγ and μ(h95)bb¯ signal strengths. In addition, we also present the impacts of the LRSSM-specific parameters tanβR, vR, and vS on the theoretical predictions of the signal strengths for the 95 and 125 GeV neutral Higgs bosons.

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We take the axion-like particle of gravitational origin to be approximately massless in the early Universe and show how inflation with the Higgs field materializes."}],"arxiv_eprints":[{"categories":[],"value":["10.1016/j.physletb.2026.140376"]}],"authors":[{"affiliations":[{"country":"Germany","organization":"Max-Planck-Institut für Physik, Boltzmannstraße 8","value":"Max-Planck-Institut für Physik, Boltzmannstraße 8, Garching b. München, 85748, Germany"},{"country":"Germany","organization":"Arnold Sommerfeld Center, Ludwig-Maximilians-Universität München Theresienstraße 37","value":"Arnold Sommerfeld Center, Ludwig-Maximilians-Universität München Theresienstraße 37, München, 80333, Germany"}],"email":null,"full_name":null,"given_names":"Georgios K.","surname":"Karananas"},{"affiliations":[{"country":"Switzerland","organization":"Institute of Physics, École Polytechnique Fédérale de Lausanne (EPFL)","value":"Institute of Physics, École Polytechnique Fédérale de Lausanne (EPFL), Lausanne, CH-1015, Switzerland"}],"email":null,"full_name":null,"given_names":"Mikhail","surname":"Shaposhnikov"}],"collections":[{"primary":"Physics Letters B"}],"control_number":106051,"copyright":[{"statement":"The Authors","holder":"The Authors","year":2026}],"dois":[{"value":"10.1016/j.physletb.2026.140376"}],"imprints":[{"date":null,"publisher":"Elsevier"}],"license":[{"license":"CC-BY-3.0","url":"http://creativecommons.org/licenses/by/3.0/"}],"page_nr":[],"publication_info":[{"artid":"140376","journal_issue":"","journal_title":"Physics Letters B","journal_volume":"1026 C","page_end":"","page_start":"","year":"2026"}],"record_creation_date":"2026-04-02T00:07:24.673485+00:00","titles":[{"source":"Elsevier","title":"Higgs inflation in Weyl-invariant Einstein-Cartan gravity"}]},"updated":"2026-04-08T00:16:38.385752+00:00","id":106051,"created":"2026-04-02T00:07:24.673485+00:00"}]}}