First constraints on the coherent elastic scattering of reactor antineutrinos off xenon nucleiRED-100 is a two-phase emission detector with an active volume containing 126~kg of liquid xenon. The detector was exposed to the antineutrino flux of about 1.4 · 1013~cm-2s-1 at a…D. Yu. Akimov, I. S. Alexandrov, V. A. Belov et al.·Nov 25, 2024SaveLearn
Search for Higgs boson decays into a Z boson and a light hadronically decaying resonance in pp collisions at s=13 TeV with the ATLAS detectorA search for decays of the Higgs boson into a Z boson and a light resonance, with a mass of 0.5-3.5 GeV, is performed using the full 140 fb-1 dataset of 13 TeV proton-proton collisions…ATLAS Collaboration·Nov 25, 2024SaveLearn
Averages of b-hadron, c-hadron, and τ-lepton properties as of 2023This paper reports world averages of measurements of b-hadron, c-hadron, and τ-lepton properties obtained by the Heavy Flavour Averaging Group using results available before October 2023. In…Sw. Banerjee, E. Ben-Haim, F. Bernlochner et al.·Nov 25, 2024SaveLearn
Measurement of cross sections of e+e- K0S K0S (3686) from s= 4.682 to 4.951 GeVThe process e+e- K0S K0S (3686) is studied by analyzing e+e- collision data samples collected at eight center-of-mass energies ranging from 4.682 to 4.951 GeV with the BESIII…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Nov 24, 2024SaveLearn
New test on contact interactions in the data at s 130-207GeV by Bhabha scattering process e+e- e+e-We used data mainly collected by OPAL experiment to test the signal significance of a parameter , which is equal to zero in SM. For total cross sections, we obtained no derivation of…Zhikun Xi, Minghui Liu, Jürgen Ulbricht·Nov 24, 2024SaveLearn
Study of b0 and b0 decays to h+h'- and evidence for CP violation in b0 K+K- decaysA study of b0 and b0 decays to h+ h - (h()=π, K) is performed using pp collision data collected by the…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Nov 23, 2024SaveLearn
Search for Light Dark Matter in Low-Energy Ionization Signals from XENONnTWe report on a blinded search for dark matter with single- and few-electron signals in the first science run of XENONnT relying on a novel detector response framework that is physics-model-dependent.…E. Aprile, J. Aalbers, K. Abe et al.·Nov 22, 2024SaveLearn
Study of collective phenomena via the production of heavy quarks and quarkonia in hadronic collisionsOpen heavy flavor and quarkonia have long been identified as ideal probes for understanding the quark-gluon plasma (QGP). Heavy quarks are produced in the early stage of the heavy-ion collisions.…Victor Valencia Torres·Nov 22, 2024SaveLearn
Search for rare decays of the Z and Higgs bosons to a J/ or (2S) meson and a photon in proton-proton collisions at s = 13 TeVA search is presented for rare decays of the Z and Higgs bosons to a photon and a J/ or a (2S) meson, with the charmonium state subsequentially decaying to a pair of muons. The data set…CMS Collaboration·Nov 22, 2024SaveLearn
Measurements of inclusive and differential cross-sections of ttγ production in pp collisions at s=13 TeV with the ATLAS detectorCross-section measurements of the associated production of a top quark pair and a photon (ttγ) are performed with an integrated luminosity of 140 fb-1 of proton-proton collisions at…Carmen Diez Pardos·Nov 22, 2024SaveLearn
Direct-photon production in inelastic and high-multiplicity proton-proton collisions at s = 13 TeVIn this letter, we present the first measurement of direct photons at the transverse momentum of 1 < p T < 6 GeV/c at midrapidity |η| < 0.8 in inelastic and high-multiplicity…ALICE Collaboration·Nov 21, 2024SaveLearn
Physics Performance and Detector Requirements at an Asymmetric Higgs FactoryThe Hybrid Asymmetric Linear Higgs Factory (HALHF) proposes a shorter and cheaper design for a future Higgs factory. It reaches a s = 250 GeV using a 500 GeV electron beam accelerated by an…Antoine Laudrain, Ties Behnke, Carl Mikael Berggren et al.·Nov 21, 2024SaveLearn
Performance of the Scintillation Wall in the BM@N experimentThe performance of the scintillation wall (ScWall) has been studied in the first physics run at the Baryonic Matter at Nuclotron (BM@N) in Xe+CsI reaction at a xenon beam energy of 3.8 and 3.0 AGeV.…V. Volkov, M. Golubeva, F. Guber et al.·Nov 21, 2024SaveLearn
Measurement of the inclusive branching fractions for Bs0 decays into D mesons via hadronic taggingWe report measurements of the absolute branching fractions B(Bs0 Ds X), B(Bs0 D0/D0 X), and B(Bs0 D X), where the latter is…Belle, Belle II Collaborations, : et al.·Nov 21, 2024SaveLearn
Search for flavour-changing neutral current couplings between the top quark and the Higgs boson in multilepton final states with the ATLAS detectorThese proceedings present a search for flavour-changing neutral-current (FCNC) interaction involving the top quark, Higgs boson and either the up or the charm quark, using 140 fb-1 of 13 TeV…Shayma Wahdan, On behalf of the ATLAS collaboration·Nov 21, 2024SaveLearn
An accurate solar axions ray-tracing response of BabyIAXOBabyIAXO is the intermediate stage of the International Axion Observatory (IAXO) to be hosted at DESY. Its primary goal is the detection of solar axions following the axion helioscope technique.…S. Ahyoune, K. Altenmueller, I. Antolin et al.·Nov 21, 2024SaveLearn
Maximizing Quantum Enhancement in Axion Dark Matter ExperimentsWe provide a comprehensive comparison of linear amplifiers and microwave photon-counters in axion dark matter experiments. The study is done assuming a range of realistic operating conditions and…Chao-Lin Kuo, Chelsea L. Bartram, Aaron S. Chou et al.·Nov 21, 2024SaveLearn
Measurement of the t-channel single top-quark production cross section at s=13 TeV with the ATLAS detector and interpretations of the measurementThe t-channel is the dominant production channel for single top-quarks at the LHC. The total cross section of this process is measured by ATLAS in proton-proton collisions at a center-of-mass…Maren Stratmann·Nov 19, 2024SaveLearn
Neutrino Oscillation Tomography of the Earth with the Hyper-Kamiokande DetectorUsing PREM as a reference model for the Earth density distribution we investigate the sensitivity of the Hyper-Kamiokande (HK) detector to deviations of the Earth i) core average density…César Jesús-Valls, Serguey T. Petcov, Junjie Xia·Nov 19, 2024SaveLearn
Production cross sections of light and charmed mesons in e+e- annihilation near 10.58 GeVWe report measurements of production cross sections for +, 0, ω, K*+, K*0, φ, η, KS0, f0(980), D+, D0, Ds+, D*+, D*0, and…Belle Collaboration, R. Seidl, I. Adachi et al.·Nov 19, 2024SaveLearn
First evidence for direct CP violation in beauty to charmonium decaysThe C\!P asymmetry and branching fraction of the CKM-suppressed decay B+\! J -3mu/ -2mu\,π+ are precisely measured relative to the favoured decay $B+\! J…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Nov 19, 2024SaveLearn
Angular analysis of the B0 K*(892)0μ+μ- decay in proton-proton collisions at s = 13 TeVA full set of optimized observables is measured in an angular analysis of the decay B0 K*(892)0μ+μ- using a sample of proton-proton collisions at s = 13 TeV, collected…CMS Collaboration·Nov 18, 2024SaveLearn
Evidence for Two Excited - HyperonsUsing e+e- collision data corresponding to an integrated luminosity of 19,fb-1 collected by the BESIII detector at center-of-mass energies ranging from 4.13 to 4.70,GeV, we report the first…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Nov 18, 2024SaveLearn
Search for the KL π0 Decay at the J-PARC KOTO ExperimentWe performed a search for the KL π0 decay using the data taken in 2021 at the J-PARC KOTO experiment. With newly installed counters and new analysis method, the expected…KOTO Collaboration, J. K. Ahn, M. Farriagton et al.·Nov 18, 2024SaveLearn
Modeling the Differential Rate for Signal Interactions in Coincidence with Noise Fluctuations or Large Rate BackgroundsThe characteristic energy of a relic dark matter interaction with a detector scales strongly with the putative dark matter mass. Consequently, experimental search sensitivity at the lightest masses…Xinran Li, Matt Pyle, Bernard Sadoulet·Nov 16, 2024SaveLearn