{"count":3939,"next":"https://repo.scoap3.org/api/records/?format=json&page=2&search=higgs","previous":null,"hits":{"hits":[{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/9pv5-qcfv/9pv5-qcfv.pdf","key":"9pv5-qcfv","filetype":"pdf"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/9pv5-qcfv/9pv5-qcfv.xml","key":"9pv5-qcfv","filetype":"xml"}],"abstracts":[{"source":"APS","value":"<p>Extensions of the Standard Model featuring both an enlarged scalar sector and vector-like fermions arise naturally in a wide class of well-motivated theoretical frameworks. In such scenarios, vectorlike quarks (VLQs) can exhibit nonstandard decay modes involving additional Higgs states, giving rise to distinctive collider signatures that remain largely unexplored by existing experimental searches. We investigate the prospects of probing this possibility at the high-luminosity Large Hadron Collider (HL-LHC) through the decay of vector-like top partner (<math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>T</mi></math>) to charged Higgs (<math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msup><mi>H</mi><mo>±</mo></msup></math>) followed by the decay, <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msup><mi>H</mi><mo>±</mo></msup><mo stretchy=\"false\">→</mo><mi>τ</mi><mi>ν</mi></math>, producing a final state containing two tau leptons, two <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>b</mi></math> jets, and missing transverse energy. A model-independent collider analysis is performed using global kinematic observables constructed from visible objects and the missing transverse momentum vector to suppress the dominant backgrounds. Polarization-sensitive observables built from the hadronic <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>τ</mi></math> decay products are also examined as complementary probes of the spin-0 origin of the <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>τ</mi></math> leptons. The expected discovery sensitivity is evaluated using the Asimov significance for an integrated luminosity of <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mn>3</mn><mtext> </mtext><mtext> </mtext><msup><mi>ab</mi><mrow><mo>−</mo><mn>1</mn></mrow></msup></math> at <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msqrt><mi>s</mi></msqrt><mo>=</mo><mn>14</mn><mtext> </mtext><mtext> </mtext><mi>TeV</mi></math>. Our results demonstrate that the <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mn>2</mn><mi>τ</mi><mo>+</mo><mn>2</mn><mi>b</mi><mo>+</mo><msub><menclose notation=\"updiagonalstrike\" other=\"updiag1\"><mi>E</mi></menclose><mi>T</mi></msub></math> (where <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msub><menclose notation=\"updiagonalstrike\" other=\"updiag1\"><mi>E</mi></menclose><mi>T</mi></msub></math> is the missing transverse energy) channel provides a promising and largely orthogonal avenue to search for non-standard VLQ decays in extended Higgs sectors, with discovery-level sensitivity achievable for VLQ masses up to approximately 1.9 TeV.</p>"}],"arxiv_eprints":[{"categories":["hep-ph","hep-ex"],"value":["10.1103/9pv5-qcfv","2606.20054"]}],"authors":[{"affiliations":[{"country":"India","organization":"Indian Institute of Science Education and Research Thiruvananthapuram, Vithura, Kerala 695 551, India","value":"<a href=\"https://ror.org/01pe3t004\">Indian Institute of Science Education and Research Thiruvananthapuram</a>, Vithura, Kerala 695 551, India"}],"email":null,"full_name":null,"given_names":"Tanumoy","surname":"Mandal"},{"affiliations":[{"country":"United Kingdom","organization":"School of Physics and Astronomy, University of Southampton, Southampton SO17 1BJ, United Kingdom","value":"School of Physics and Astronomy, <a href=\"https://ror.org/01ryk1543\">University of Southampton</a>, Southampton SO17 1BJ, United Kingdom"},{"country":"Sweden","organization":"Department of Physics and Astronomy, Uppsala University, Box 516, SE-751 20 Uppsala, Sweden","value":"Department of Physics and Astronomy, <a href=\"https://ror.org/048a87296\">Uppsala University</a>, Box 516, SE-751 20 Uppsala, Sweden"}],"email":null,"full_name":null,"given_names":"Stefano","surname":"Moretti"},{"affiliations":[{"country":"India","organization":"Indian Institute of Science Education and Research Thiruvananthapuram, Vithura, Kerala 695 551, India","value":"<a href=\"https://ror.org/01pe3t004\">Indian Institute of Science Education and Research Thiruvananthapuram</a>, Vithura, Kerala 695 551, India"}],"email":null,"full_name":null,"given_names":"Rachit","surname":"Sharma"}],"collections":[{"primary":"Physical Review D"}],"control_number":111660,"copyright":[{"statement":"Published by the American Physical Society","holder":"","year":2026}],"dois":[{"value":"10.1103/9pv5-qcfv"},{"value":"2606.20054"}],"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":"114","page_end":"","page_start":"","year":"2026"}],"record_creation_date":"2026-10-02T18:00:19.338039+00:00","titles":[{"source":"APS","title":"Nonstandard decays of vectorlike top partners in a two-Higgs-doublet model at the HL-LHC"}]},"updated":"2026-10-03T00:00:38.599775+00:00","id":111660,"created":"2026-10-02T18:00:19.338039+00:00"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1140/epjc/s10052-026-16295-7/10052_2026_Article_16295.xml.Meta.xml","key":"10052_2026_Article_16295.xml.Meta","filetype":"xml"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1140/epjc/s10052-026-16295-7/10052_2026_Article_16295_a.pdf","key":"10052_2026_Article_16295_a","filetype":"pdf"}],"abstracts":[{"source":"Springer","value":"Models of Dark Matter must contend with the fact that the presence of electroweak symmetry breaking along the thermal evolution of the Universe modifies the masses, interactions and, thus, the thermally averaged cross sections. We study in detail the impact of taking (not taking) the presence of the electroweak symmetry breaking into account in the calculations of the Dark Matter relic density in Higgs portal models, providing a model-independent measure of such differences. By focusing on a particular model, we show that ignoring this effect can lead to the inclusion (exclusion) of wrong (viable) regions of parameter space."}],"arxiv_eprints":[{"categories":["hep-ph"],"value":["10.1140/epjc/s10052-026-16295-7","2505.07946"]}],"authors":[{"affiliations":[{"country":"United Kingdom","organization":"Durham University","value":"Department of Physics, Institute for Particle Physics Phenomenology, Durham University, Durham, DH1 3LE, UK"}],"email":null,"full_name":null,"given_names":"Sreemanti","surname":"Chakraborti"},{"affiliations":[{"country":"Portugal","organization":"Universidade de Lisboa","value":"Instituto Superior Técnico, Universidade de Lisboa, Avenida Rovisco Pais 1, Lisbon, 1049-001, Portugal"}],"email":null,"full_name":null,"given_names":"André","surname":"Milagre"},{"affiliations":[{"country":"Portugal","organization":"Universidade de Lisboa","value":"Faculdade de Ciências, Centro de Física Téorica e Computacional, Universidade de Lisboa, Campo Grande, Edifício C8, Lisbon, 1749-016, Portugal"},{"country":"Portugal","organization":"ISEL-Instituto Politécnico de Lisboa","value":"ISEL-Instituto Politécnico de Lisboa, Lisbon, 1959-007, Portugal"}],"email":null,"full_name":null,"given_names":"Rui","surname":"Santos"},{"affiliations":[{"country":"Portugal","organization":"Universidade de Lisboa","value":"Instituto Superior Técnico, Universidade de Lisboa, Avenida Rovisco Pais 1, Lisbon, 1049-001, Portugal"}],"email":null,"full_name":null,"given_names":"João","surname":"Silva"}],"collections":[{"primary":"European Physical Journal C"}],"control_number":111519,"copyright":[{"statement":"","holder":"The Author(s)","year":2026}],"dois":[{"value":"10.1140/epjc/s10052-026-16295-7"},{"value":"2505.07946"}],"imprints":[{"date":null,"publisher":"Springer"}],"license":[{"license":"CC-BY-4.0","url":"http://creativecommons.org/licenses/by/4.0/"}],"page_nr":[13],"publication_info":[{"artid":"s10052-026-16295-7","journal_issue":"9","journal_title":"European Physical Journal C","journal_volume":"86","page_end":"13","page_start":"1","year":"2026"}],"record_creation_date":"2026-09-28T06:55:59.953784+00:00","titles":[{"source":"Springer","title":"Interplay between electroweak symmetry breaking and Higgs portal dark matter"}]},"updated":"2026-09-28T18:56:17.153502+00:00","id":111519,"created":"2026-09-28T06:55:59.953784+00:00"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/l8qz-q978/l8qz-q978.pdf","key":"l8qz-q978","filetype":"pdf"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/l8qz-q978/l8qz-q978.xml","key":"l8qz-q978","filetype":"xml"}],"abstracts":[{"source":"APS","value":"<p>We study flavor-violating decays of the SM-like Higgs boson and rare top decays in the type 1B realization of the flavorful two-Higgs-doublet model with a twist, focusing on <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>h</mi><mo stretchy=\"false\">→</mo><mi>s</mi><mi>b</mi></math>, <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>h</mi><mo stretchy=\"false\">→</mo><mi>d</mi><mi>b</mi></math>, <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>h</mi><mo stretchy=\"false\">→</mo><mi>u</mi><mi>c</mi></math>, <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>h</mi><mo stretchy=\"false\">→</mo><mi>μ</mi><mi>τ</mi></math>, <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>h</mi><mo stretchy=\"false\">→</mo><mi>e</mi><mi>τ</mi></math>, <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>h</mi><mo stretchy=\"false\">→</mo><mi>e</mi><mi>μ</mi></math>, <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>t</mi><mo stretchy=\"false\">→</mo><mi>c</mi><mi>h</mi></math>, and <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>t</mi><mo stretchy=\"false\">→</mo><mi>u</mi><mi>h</mi></math>. We present the relevant amplitude and branching-ratio formulae, include one-loop vertex corrections, and impose constraints from Higgs signal-strength measurements, electroweak precision tests, meson mixing, <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>B</mi><mo stretchy=\"false\">→</mo><msub><mi>X</mi><mi>s</mi></msub><mi>γ</mi></math>, direct HFV searches, and CLFV constraints, including <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>μ</mi><mo>−</mo><mi>e</mi></math> conversion. The surviving parameter space favors <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>BR</mi><mo stretchy=\"false\">(</mo><mi>h</mi><mo stretchy=\"false\">→</mo><mi>s</mi><mi>b</mi><mo stretchy=\"false\">)</mo><mo>≫</mo><mspace linebreak=\"goodbreak\"></mspace><mi>BR</mi><mo stretchy=\"false\">(</mo><mi>h</mi><mo stretchy=\"false\">→</mo><mi>d</mi><mi>b</mi><mo stretchy=\"false\">)</mo></math>, <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>BR</mi><mo stretchy=\"false\">(</mo><mi>t</mi><mo stretchy=\"false\">→</mo><mi>c</mi><mi>h</mi><mo stretchy=\"false\">)</mo><mo>≫</mo><mi>BR</mi><mo stretchy=\"false\">(</mo><mi>t</mi><mo stretchy=\"false\">→</mo><mi>u</mi><mi>h</mi><mo stretchy=\"false\">)</mo></math>, and <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>BR</mi><mo stretchy=\"false\">(</mo><mi>h</mi><mo stretchy=\"false\">→</mo><mi>μ</mi><mi>τ</mi><mo stretchy=\"false\">)</mo><mo>≫</mo><mi>BR</mi><mo stretchy=\"false\">(</mo><mi>h</mi><mo stretchy=\"false\">→</mo><mi>e</mi><mi>τ</mi><mo stretchy=\"false\">)</mo><mo>∼</mo><mi>BR</mi><mo stretchy=\"false\">(</mo><mi>h</mi><mo stretchy=\"false\">→</mo><mi>e</mi><mi>μ</mi><mo stretchy=\"false\">)</mo></math> in the lepton sector. One-loop effects usually preserve these hierarchies, but can modify individual channels through different mechanisms: sizable destructive tree-loop interference can reduce <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>h</mi><mo stretchy=\"false\">→</mo><mi>s</mi><mi>b</mi></math> enough to yield rare <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msub><mi>BR</mi><mrow><mn>1</mn><mi mathvariant=\"normal\">L</mi></mrow></msub><mo stretchy=\"false\">(</mo><mi>h</mi><mo stretchy=\"false\">→</mo><mi>d</mi><mi>b</mi><mo stretchy=\"false\">)</mo><mo>&gt;</mo><msub><mi>BR</mi><mrow><mn>1</mn><mi mathvariant=\"normal\">L</mi></mrow></msub><mo stretchy=\"false\">(</mo><mi>h</mi><mo stretchy=\"false\">→</mo><mi>s</mi><mi>b</mi><mo stretchy=\"false\">)</mo></math> points, whereas the large relative corrections found in rare top decays mainly reflect strong SM-like alignment suppressing the tree-level amplitudes.</p>"}],"arxiv_eprints":[{"categories":["hep-ph"],"value":["10.1103/l8qz-q978","2609.00692"]}],"authors":[{"affiliations":[{"country":"China","organization":"Department of Physics, Hebei University, Baoding 071002, China","value":"Department of Physics, <a href=\"https://ror.org/01p884a79\">Hebei University</a>, Baoding 071002, China"},{"country":"China","organization":"Hebei Key Laboratory of High-precision Computation and Application of Quantum Field Theory, Baoding 071002, China","value":"<a href=\"https://ror.org/01p884a79\">Hebei Key Laboratory of High-precision Computation and Application of Quantum Field Theory</a>, Baoding 071002, China"},{"country":"China","organization":"Hebei Research Center of the Basic Discipline for Computational Physics, Baoding 071002, China","value":"<a href=\"https://ror.org/01p884a79\">Hebei Research Center of the Basic Discipline for Computational Physics</a>, Baoding 071002, China"}],"email":null,"full_name":null,"given_names":"Ti-Bin","surname":"Hou"},{"affiliations":[{"country":"China","organization":"Department of Physics, Hebei University, Baoding 071002, China","value":"Department of Physics, <a href=\"https://ror.org/01p884a79\">Hebei University</a>, Baoding 071002, China"},{"country":"China","organization":"Hebei Key Laboratory of High-precision Computation and Application of Quantum Field Theory, Baoding 071002, China","value":"<a href=\"https://ror.org/01p884a79\">Hebei Key Laboratory of High-precision Computation and Application of Quantum Field Theory</a>, Baoding 071002, China"},{"country":"China","organization":"Hebei Research Center of the Basic Discipline for Computational Physics, Baoding 071002, China","value":"<a href=\"https://ror.org/01p884a79\">Hebei Research Center of the Basic Discipline for Computational Physics</a>, Baoding 071002, China"}],"email":null,"full_name":null,"given_names":"Zheng","surname":"Li"},{"affiliations":[{"country":"China","organization":"Department of Physics, Hebei University, Baoding 071002, China","value":"Department of Physics, <a href=\"https://ror.org/01p884a79\">Hebei University</a>, Baoding 071002, China"},{"country":"China","organization":"Hebei Key Laboratory of High-precision Computation and Application of Quantum Field Theory, Baoding 071002, China","value":"<a href=\"https://ror.org/01p884a79\">Hebei Key Laboratory of High-precision Computation and Application of Quantum Field Theory</a>, Baoding 071002, China"},{"country":"China","organization":"Hebei Research Center of the Basic Discipline for Computational Physics, Baoding 071002, China","value":"<a href=\"https://ror.org/01p884a79\">Hebei Research Center of the Basic Discipline for Computational Physics</a>, Baoding 071002, China"}],"email":null,"full_name":null,"given_names":"Yu-Ju","surname":"Peng"},{"affiliations":[{"country":"China","organization":"Department of Physics, Hebei University, Baoding 071002, China","value":"Department of Physics, <a href=\"https://ror.org/01p884a79\">Hebei University</a>, Baoding 071002, China"},{"country":"China","organization":"Hebei Key Laboratory of High-precision Computation and Application of Quantum Field Theory, Baoding 071002, China","value":"<a href=\"https://ror.org/01p884a79\">Hebei Key Laboratory of High-precision Computation and Application of Quantum Field Theory</a>, Baoding 071002, China"},{"country":"China","organization":"Hebei Research Center of the Basic Discipline for Computational Physics, Baoding 071002, China","value":"<a href=\"https://ror.org/01p884a79\">Hebei Research Center of the Basic Discipline for Computational Physics</a>, Baoding 071002, China"}],"email":null,"full_name":null,"given_names":"Jin-Lei","surname":"Yang"},{"affiliations":[{"country":"China","organization":"Department of Physics, Hebei University, Baoding 071002, China","value":"Department of Physics, <a href=\"https://ror.org/01p884a79\">Hebei University</a>, Baoding 071002, China"},{"country":"China","organization":"Hebei Key Laboratory of High-precision Computation and Application of Quantum Field Theory, Baoding 071002, China","value":"<a href=\"https://ror.org/01p884a79\">Hebei Key Laboratory of High-precision Computation and Application of Quantum Field Theory</a>, Baoding 071002, China"},{"country":"China","organization":"Hebei Research Center of the Basic Discipline for Computational Physics, Baoding 071002, China","value":"<a href=\"https://ror.org/01p884a79\">Hebei Research Center of the Basic Discipline for Computational Physics</a>, Baoding 071002, China"}],"email":null,"full_name":null,"given_names":"Hao-Ran","surname":"Ma"},{"affiliations":[{"country":"China","organization":"Department of Physics, Hebei University, Baoding 071002, China","value":"Department of Physics, <a href=\"https://ror.org/01p884a79\">Hebei University</a>, Baoding 071002, China"},{"country":"China","organization":"Department of Physics, Chongqing University, Chongqing 401331, China","value":"Department of Physics, <a href=\"https://ror.org/023rhb549\">Chongqing University</a>, Chongqing 401331, China"},{"country":"China","organization":"Hebei Key Laboratory of High-precision Computation and Application of Quantum Field Theory, Baoding 071002, China","value":"<a href=\"https://ror.org/01p884a79\">Hebei Key Laboratory of High-precision Computation and Application of Quantum Field Theory</a>, Baoding 071002, China"},{"country":"China","organization":"Hebei Research Center of the Basic Discipline for Computational Physics, Baoding 071002, China","value":"<a href=\"https://ror.org/01p884a79\">Hebei Research Center of the Basic Discipline for Computational Physics</a>, Baoding 071002, China"}],"email":null,"full_name":null,"given_names":"Tai-Fu","surname":"Feng"}],"collections":[{"primary":"Physical Review D"}],"control_number":111483,"copyright":[{"statement":"Published by the American Physical Society","holder":"","year":2026}],"dois":[{"value":"10.1103/l8qz-q978"},{"value":"2609.00692"}],"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":"114","page_end":"","page_start":"","year":"2026"}],"record_creation_date":"2026-09-25T18:00:20.356307+00:00","titles":[{"source":"APS","title":"Flavor-violating Higgs and top decays in the type 1B flavorful two-Higgs-doublet model with a twist"}]},"updated":"2026-09-26T00:00:33.462576+00:00","id":111483,"created":"2026-09-25T18:00:20.356307+00:00"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP09(2026)267/13130_2026_Article_30150.xml.scoap.xml","key":"13130_2026_Article_30150.xml.scoap","filetype":"xml"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP09(2026)267/13130_2026_Article_30150_a.pdf","key":"13130_2026_Article_30150_a","filetype":"pdf"}],"abstracts":[{"source":"Springer","value":"We study the angular distribution of the Higgs boson decay $$ h\\to \\ell {\\overline{\\nu}}_{\\ell }{\\overline{\\ell}}^{\\prime }{\\nu}_{\\ell^{\\prime }} $$ with $\\textit{ℓ}$ ≠ $\\textit{ℓ}$ . Due to the presence of two undetected neutrinos, a complete angular analysis is not experimentally feasible. To overcome this, we reorganize the kinematics from the conventional lepton-neutrino pairs into a charged-lepton pair and a neutrino pair, i.e. $$ \\ell {\\overline{\\ell}}^{\\prime } $$ and $$ {\\overline{\\nu}}_{\\ell }{\\nu}_{\\ell^{\\prime }} $$ . This allows us to express the differential decay rate in terms of experimentally accessible variables, including the invariant mass squared of the neutrino pair. Using the effective field theory framework, we derive this rate and integrate over the neutrino-associated angles. This parametrization provides a clean and measurable angular distribution, offering a new probe of the $\\textit{hWW}$ coupling and possible beyond-the-Standard-Model contributions."}],"arxiv_eprints":[{"categories":["hep-ph"],"value":["10.1007/JHEP09(2026)267","2606.05061"]}],"authors":[{"affiliations":[{"country":"China","organization":"Zhengzhou University","value":"School of Physics, Zhengzhou University, Zhengzhou, Henan, 450001, China"}],"email":null,"full_name":null,"given_names":"Han","surname":"Zhang"},{"affiliations":[{"country":"China","organization":"Zhengzhou University","value":"School of Physics, Zhengzhou University, Zhengzhou, Henan, 450001, China"}],"email":null,"full_name":null,"given_names":"Bai-Cian","surname":"Ke"},{"affiliations":[{"country":"China","organization":"Chongqing University of Posts & Telecommunications","value":"Chongqing University of Posts & Telecommunications, Chongqing, 400065, China"},{"country":"China","organization":"Chongqing University","value":"Department of Physics and Chongqing Key Laboratory for Strongly Coupled Physics, Chongqing University, Chongqing, 401331, China"}],"email":null,"full_name":null,"given_names":"Yao","surname":"Yu"},{"affiliations":[{"country":"China","organization":"Chongqing University of Posts & Telecommunications","value":"Chongqing University of Posts & Telecommunications, Chongqing, 400065, China"}],"email":null,"full_name":null,"given_names":"Yi-Rong","surname":"Ma"},{"affiliations":[{"country":"China","organization":"Chongqing University of Science and Technology","value":"Department of Physics, Chongqing University of Science and Technology, Chongqing, 401331, China"}],"email":null,"full_name":null,"given_names":"Jia-Wei","surname":"Zhang"}],"collections":[{"primary":"Journal of High Energy Physics"}],"control_number":111502,"copyright":[{"statement":"","holder":"The Author(s)","year":2026}],"dois":[{"value":"10.1007/JHEP09(2026)267"},{"value":"2606.05061"}],"imprints":[{"date":null,"publisher":"Springer"}],"license":[{"license":"CC-BY-4.0","url":"http://creativecommons.org/licenses/by/4.0/"}],"page_nr":[15],"publication_info":[{"artid":"JHEP09(2026)267","journal_issue":"9","journal_title":"Journal of High Energy Physics","journal_volume":"2026","page_end":"15","page_start":"1","year":"2026"}],"record_creation_date":"2026-09-26T06:55:43.569848","titles":[{"source":"Springer","title":"Angular and invariant-mass observables in the four-body Higgs decay $$ h\\to \\ell {\\overline{\\nu}}_{\\ell }{\\overline{\\ell}}^{\\prime }{\\nu}_{\\ell^{\\prime }} $$"}]},"updated":"2026-09-26T06:55:49.346297+00:00","id":111502,"created":"2026-09-26T06:55:43.569848"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/27s7-2frt/27s7-2frt.pdf","key":"27s7-2frt","filetype":"pdf"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/27s7-2frt/27s7-2frt.xml","key":"27s7-2frt","filetype":"xml"}],"abstracts":[{"source":"APS","value":"<p>This Letter presents a combination of searches for Higgs boson pair (<math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>H</mi><mi>H</mi></math>) production performed by the ATLAS and CMS Collaborations using proton-proton collision datasets recorded 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> during the Large Hadron Collider Run 2, corresponding to integrated luminosities ranging between 126 and <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mn>140</mn><mtext> </mtext><mtext> </mtext><msup><mi>fb</mi><mrow><mo>−</mo><mn>1</mn></mrow></msup></math>. The upper limit at the 95% confidence level on the total <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>H</mi><mi>H</mi></math> signal strength, defined as the ratio of the measured cross section to the standard model (SM) prediction, corresponds to 2.5, with an expected value of 1.7 (2.8) assuming the absence (presence) of the SM <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>H</mi><mi>H</mi></math> signal. The strength of the <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>H</mi><mi>H</mi></math> signal is measured to be <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msubsup><mn>0.8</mn><mrow><mo>−</mo><mn>0.7</mn></mrow><mrow><mo>+</mo><mn>0.9</mn></mrow></msubsup></math> relative to the SM prediction. The observed significance is found to be 1.1 standard deviations whereas 1.3 are expected for the SM <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>H</mi><mi>H</mi></math> signal. Constraints are set on the Higgs boson trilinear self-coupling and on the couplings of two Higgs bosons to two vector bosons, both normalized to the SM predictions and denoted as <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msub><mi>κ</mi><mi>λ</mi></msub></math> and <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><msub><mi>κ</mi><mrow><mn>2</mn><mi>V</mi></mrow></msub></math>, respectively. The observed individual constraints at the 95% confidence level are <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mrow><mo>−</mo><mn>0.71</mn><mo>&lt;</mo><msub><mrow><mi>κ</mi></mrow><mrow><mi>λ</mi></mrow></msub><mo>&lt;</mo><mn>6.1</mn></mrow></math> and <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mn>0.73</mn><mo>&lt;</mo><msub><mi>κ</mi><mrow><mn>2</mn><mi>V</mi></mrow></msub><mo>&lt;</mo><mn>1.3</mn></math>, while the expected constraints assuming the presence of the SM <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mi>H</mi><mi>H</mi></math> signal are <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mo>−</mo><mn>1.3</mn><mo>&lt;</mo><msub><mi>κ</mi><mi>λ</mi></msub><mo>&lt;</mo><mn>6.7</mn></math> and <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mn>0.66</mn><mo>&lt;</mo><msub><mi>κ</mi><mrow><mn>2</mn><mi>V</mi></mrow></msub><mo>&lt;</mo><mn>1.4</mn></math>.</p>"}],"arxiv_eprints":[{"categories":["hep-ex"],"value":["10.1103/27s7-2frt","2602.23991"]}],"authors":[{"affiliations":[{"country":"France","organization":"CPPM, Aix-Marseille Université, CNRS/IN2P3, Marseille, France","value":"CPPM, Aix-Marseille Université, CNRS/IN2P3, Marseille, France"}],"email":null,"full_name":null,"given_names":"G.","surname":"Aad"},{"affiliations":[{"country":"Norway","organization":"Department for Physics and Technology, University of Bergen, Bergen, Norway","value":"Department for Physics and Technology, University of Bergen, Bergen, Norway"}],"email":null,"full_name":null,"given_names":"E.","surname":"Aakvaag"},{"affiliations":[{"country":"United States","organization":"Homer L. 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The latter describe the nearly collinear emission of a Higgs boson from a top-quark and reproduce the leading mass dependence of the exact next-to-leading-order (NLO) calculation. Although the NLO fragmentation functions have been calculated a few years ago, it has not been possible up to now to demonstrate the applicability of the approximation in a realistic setup. At NLO, we analyse two different ways of treating the top-quark mass, called the zero-mass-top-quark (ZMTQ) and the hybrid prescription. We show that the method yields reliable results at LHC center-of-mass (cms) energies in the hybrid prescription. In the ZMTQ prescription, the results at LHC cms energies are only reliable in the quark-anti-quark channel, but become viable for the full $$ pp\\to t\\overline{t}H $$ process at a 100 TeV hadron collider. In addition, we discuss some subtleties and complications arising when extending the formalism to next-to-next-to-leading-order (NNLO) and beyond."}],"arxiv_eprints":[{"categories":["hep-ph"],"value":["10.1007/JHEP09(2026)255","2605.05880"]}],"authors":[{"affiliations":[{"country":"Italy","organization":"Università di Torino, and INFN, Sezione di Torino","value":"Dipartimento di Fisica and Arnold-Regge Center, Università di Torino, and INFN, Sezione di Torino, Via P. Giuria 1, Torino, I-10125, Italy"}],"email":null,"full_name":null,"given_names":"Colomba","surname":"Brancaccio"},{"affiliations":[{"country":"Germany","organization":"RWTH Aachen University","value":"Institut für Theoretische Teilchenphysik und Kosmologie, RWTH Aachen University, Aachen, D-52056, Germany"}],"email":null,"full_name":null,"given_names":"Michał","surname":"Czakon"},{"affiliations":[{"country":"United Kingdom","organization":"University of Cambridge","value":"Cavendish Laboratory, University of Cambridge, Cambridge, CB3 0HE, U.K."}],"email":null,"full_name":null,"given_names":"Terry","surname":"Generet"},{"affiliations":[{"country":"Germany","organization":"RWTH Aachen University","value":"Institut für Theoretische Teilchenphysik und Kosmologie, RWTH Aachen University, Aachen, D-52056, Germany"}],"email":null,"full_name":null,"given_names":"Benedikt","surname":"Gurdon"}],"collections":[{"primary":"Journal of High Energy Physics"}],"control_number":111489,"copyright":[{"statement":"","holder":"The Author(s)","year":2026}],"dois":[{"value":"10.1007/JHEP09(2026)255"},{"value":"2605.05880"}],"imprints":[{"date":null,"publisher":"Springer"}],"license":[{"license":"CC-BY-4.0","url":"http://creativecommons.org/licenses/by/4.0/"}],"page_nr":[34],"publication_info":[{"artid":"JHEP09(2026)255","journal_issue":"9","journal_title":"Journal of High Energy Physics","journal_volume":"2026","page_end":"34","page_start":"1","year":"2026"}],"record_creation_date":"2026-09-25T18:55:31.937913","titles":[{"source":"Springer","title":"Top-associated Higgs-boson production using perturbative fragmentation functions at next-to-leading-order"}]},"updated":"2026-09-25T18:55:37.065477+00:00","id":111489,"created":"2026-09-25T18:55:31.937913"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP09(2026)243/13130_2026_Article_30126.xml.scoap.xml","key":"13130_2026_Article_30126.xml.scoap","filetype":"xml"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1007/JHEP09(2026)243/13130_2026_Article_30126_a.pdf","key":"13130_2026_Article_30126_a","filetype":"pdf"}],"abstracts":[{"source":"Springer","value":"We study the Higgs branch and associated vertex operator algebra (VOA) of 4d $$ \\mathcal{N} $$ = 2 superconformal field theories (SCFTs) from the geometric engineering of IIB superstring on canonical threefold singularities. For terminal singularities, we explain how to derive the 4d Higgs branch from their small resolution. We also investigate singularities with compact 4-cycles in their crepant resolution, and discuss different ways to compute their Higgs branch. Using a symplectic duality argument, we propose the first examples of 4d $$ \\mathcal{N} $$ = 2 SCFTs with the E-type Kleinian singularities as their Higgs branches, and conjecture their associated VOA to be affine E-type W-algebra. Many new VOAs with no known W-algebra descriptions are found, with conjectured associated varieties. We investigate the singularities associated with lisse VOAs and propose predictions for the BPS quivers of $$ {D}_N^N\\left[k\\right] $$ and $$ {E}_7^{14}\\left[k\\right] $$ from the perspective of deformed singularities. As an application, we show directly that the $$ {D}_N^N\\left[1\\right] $$ theory is equivalent to the ($\\textit{A}$ , $\\textit{A}$ ) Argyres-Douglas theory, and illustrate, in a general setting, how the Schur index is determined by the BPS quiver."}],"arxiv_eprints":[{"categories":["hep-th","math.RT"],"value":["10.1007/JHEP09(2026)243","2603.01742"]}],"authors":[{"affiliations":[{"country":"China","organization":"Peking University","value":"Center for High Energy Physics, Peking University, Beijing, 100871, China"},{"country":"China","organization":"Peking University","value":"School of Physics, Peking University, Beijing, 100871, China"}],"email":null,"full_name":null,"given_names":"Yi-Nan","surname":"Wang"},{"affiliations":[{"country":"China","organization":"Tsinghua University","value":"Yau Mathematical Sciences Center, Tsinghua University, Beijing, 100084, China"}],"email":null,"full_name":null,"given_names":"Wenbin","surname":"Yan"},{"affiliations":[{"country":"China","organization":"Peking University","value":"Center for High Energy Physics, Peking University, Beijing, 100871, China"}],"email":null,"full_name":null,"given_names":"Peihe","surname":"Yang"}],"collections":[{"primary":"Journal of High Energy Physics"}],"control_number":111597,"copyright":[{"statement":"","holder":"The Author(s)","year":2026}],"dois":[{"value":"10.1007/JHEP09(2026)243"},{"value":"2603.01742"}],"imprints":[{"date":null,"publisher":"Springer"}],"license":[{"license":"CC-BY-4.0","url":"http://creativecommons.org/licenses/by/4.0/"}],"page_nr":[76],"publication_info":[{"artid":"JHEP09(2026)243","journal_issue":"9","journal_title":"Journal of High Energy Physics","journal_volume":"2026","page_end":"76","page_start":"1","year":"2026"}],"record_creation_date":"2026-09-29T18:55:54.586239","titles":[{"source":"Springer","title":"Higgs branch and VOA of 4d $$ \\mathcal{N} $$ = 2 SCFTs from IIB"}]},"updated":"2026-09-29T18:56:00.342528+00:00","id":111597,"created":"2026-09-29T18:55:54.586239"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1016/j.nuclphysb.2026.117671/main.pdf","key":"main","filetype":"pdf"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1016/j.nuclphysb.2026.117671/main.xml","key":"main","filetype":"xml"}],"abstracts":[{"source":"Elsevier","value":"We study a dark photon dark matter scenario associated with a gauged <italic>U</italic>(1) <inf><italic>X</italic></inf> symmetry, stabilized by a dark parity that forbids kinetic mixing with the Standard Model. The leading interactions between the dark photon dark matter and the Standard Model arise from dimension-six Higgs-portal operators. In previous work, we found that for the parity-violating operator, the dark matter annihilation process is <italic>p</italic>-wave suppressed, naturally evading stringent direct-detection constraints while reproducing the observed relic abundance through thermal freeze-out. For a cutoff scale of 1&#8201;TeV, a dark matter mass of around 400&#8201;GeV is favored to realize the observed relic abundance. This scenario predicts cosmic-ray signals, in particular in the <math altimg='si15.svg'><mrow><msup><mi>W</mi><mo>+</mo></msup><msup><mi>W</mi><mo>&#8722;</mo></msup></mrow></math> channel, which can be targeted by indirect-detection experiments. Recently, a halo-like gamma-ray excess has been reported by Totani. Assuming a Navarro&#8211;Frenk&#8211;White <math altimg='si16.svg'><mrow><mo>&#8722;</mo><msup><mi>&#961;</mi><mn>2</mn></msup></mrow></math> morphology for the dark matter distribution, a dark matter mass of 420&#8201;GeV is favored for the <math altimg='si15.svg'><mrow><msup><mi>W</mi><mo>+</mo></msup><msup><mi>W</mi><mo>&#8722;</mo></msup></mrow></math> final state. Motivated by this excess, we consider the present dark photon dark matter framework augmented by a CP-even sub-GeV scalar mediator, which couples to the dark photon mass operator in order to enhance the present-day annihilation rate in the Galactic halo while inducing only an <math altimg='si17.svg'><mrow><mi mathvariant='script'>O</mi><mo>(</mo><mn>1</mn><mo>)</mo></mrow></math> correction at freeze-out. The exchange of this scalar induces a long-range attractive force, leading to Sommerfeld enhancement of the annihilation rate. The enhancement is saturating in dwarf spheroidal galaxies and the annihilation rate is dropping as <italic>p</italic>-wave remaining consistent with constraints from dwarf galaxies and cosmology."}],"arxiv_eprints":[{"categories":[],"value":["10.1016/j.nuclphysb.2026.117671"]}],"authors":[{"affiliations":[{"country":"Japan","organization":"Department of Physics, Ibaraki University","value":"Department of Physics, Ibaraki University, Mito, 310–8512,Japan"}],"email":null,"full_name":null,"given_names":"Kimiko","surname":"Yamashita"}],"collections":[{"primary":"Nuclear Physics B"}],"control_number":111494,"copyright":[{"statement":"The Authors","holder":"The Authors","year":2026}],"dois":[{"value":"10.1016/j.nuclphysb.2026.117671"}],"imprints":[{"date":null,"publisher":"Elsevier"}],"license":[{"license":"CC-BY-3.0","url":"http://creativecommons.org/licenses/by/3.0/"}],"page_nr":[],"publication_info":[{"artid":"117671","journal_issue":"","journal_title":"Nuclear Physics B","journal_volume":"1031 C","page_end":"","page_start":"","year":"2026"}],"record_creation_date":"2026-09-26T00:17:57.960162+00:00","titles":[{"source":"Elsevier","title":"Higgs-portal spin-1 dark matter with parity-violating interaction for a galactic halo gamma ray excess"}]},"updated":"2026-09-30T06:17:49.179780+00:00","id":111494,"created":"2026-09-26T00:17:57.960162+00:00"},{"metadata":{"_files":[{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/qydl-rlp7/qydl-rlp7.pdf","key":"qydl-rlp7","filetype":"pdf"},{"file":"https://scoap3-prod-backend.s3.cern.ch/media/harvested_files/10.1103/qydl-rlp7/qydl-rlp7.xml","key":"qydl-rlp7","filetype":"xml"}],"abstracts":[{"source":"APS","value":"<p>A search is presented for the production of two additional Higgs bosons from an off-shell <i>Z</i> boson, where both additional particles decay to <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mrow><mi>τ</mi></mrow></math> lepton pairs. The search is performed with a data sample collected with the CMS detector from proton-proton collisions at the LHC at <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mrow><msqrt><mrow><mi>s</mi></mrow></msqrt><mo>=</mo><mn>13</mn><mtext> </mtext><mtext> </mtext><mrow><mtext>TeV</mtext></mrow></mrow></math>, corresponding to an integrated luminosity of <math xmlns=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mrow><mn>138</mn><mtext> </mtext><mtext> </mtext><msup><mrow><mi>fb</mi></mrow><mrow><mo>−</mo><mn>1</mn></mrow></msup></mrow></math>. No deviation from the standard model background is observed. Exclusion limits are set on the type-X two-Higgs-doublet model alignment scenario. These results exclude previously unexplored regions of parameter space and provide constraints complementary to those from earlier searches.</p>"}],"arxiv_eprints":[{"categories":["hep-ex"],"value":["10.1103/qydl-rlp7","2605.16655"]}],"authors":[{"affiliations":[{"country":"Armenia","organization":"Yerevan Physics Institute, Yerevan, Armenia","value":"Yerevan Physics Institute, Yerevan, Armenia"}],"email":null,"full_name":null,"given_names":"A.","surname":"Hayrapetyan"},{"affiliations":[{"country":"Armenia","organization":"Yerevan Physics Institute, Yerevan, Armenia","value":"Yerevan Physics Institute, Yerevan, Armenia"}],"email":null,"full_name":null,"given_names":"A.","surname":"Tumasyan"},{"affiliations":[{"country":"Austria","organization":"Institut für Hochenergiephysik, Vienna, Austria","value":"Institut für Hochenergiephysik, Vienna, Austria"}],"email":null,"full_name":null,"given_names":"W.","surname":"Adam"},{"affiliations":[{"country":"Austria","organization":"Institut für 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