Dark photon constraints from a 7.139 GHz cavity haloscope experimentThe dark photon is a promising candidate for the dark matter which comprises most of the matter in our visible Universe. Via kinetic mixing with the Standard Model it can also be resonantly converted…Dong He, Jie Fan, Xin Gao et al.·Apr 1, 2024SaveLearn
Experimental status of |Vcd| and |Vcs|The Cabibbo-Kobayashi-Maskawa (CKM) matrix elements |Vcd| and |Vcs| are essential to test the unitary of CKM matrix. Before 2014, many results of |Vcd| and |Vcs| had been reported…Tengjiao Wang·Mar 31, 2024SaveLearn
CP violation in D meson decays at Belle I/IIWe present recent measurements from the Belle and Belle II experiment related to CP violation in decays of charmed mesons via two complementary approaches. We also propose a new algorithm to…Michel Bertemes·Mar 30, 2024SaveLearn
Angular analysis of B K* e+ e- in the low-q2 region with new electron identification at BelleWe perform an angular analysis of the B K* e+ e- decay for the dielectron mass squared, q2, range of 0.0008 to 1.1200 ~GeV2 /c4 using the full Belle data set in the $K*0…Belle Collaboration, D. Ferlewicz, P. Urquijo et al.·Mar 30, 2024SaveLearn
Differentiable nuclear deexcitation simulation for low energy neutrino physicsNeutrino-nucleus interactions play an important role in present and future neutrino experiments. The accurate simulation of these interactions at low energies (<100 MeV) is crucial for the…Pablo Barham Alzás, Radi Radev·Mar 29, 2024SaveLearn
Constraints on the Blazar-Boosted Dark Matter from the CDEX-10 ExperimentWe report new constraints on light dark matter (DM) boosted by blazars using the 205.4 kg day data from the CDEX-10 experiment located at the China Jinping Underground Laboratory. Two representative…R. Xu, L. T. Yang, Q. Yue et al.·Mar 29, 2024SaveLearn
Probing Dark Matter Particles from Evaporating Primordial Black Holes via Electron Scattering in the CDEX-10 ExperimentDark matter (DM) is a major constituent of the Universe. However, no definite evidence of DM particles (denoted as ``") has been found in DM direct detection (DD) experiments to date. There is…Z. H. Zhang, L. T. Yang, Q. Yue et al.·Mar 29, 2024SaveLearn
Search for ZZ and ZH production in the bbbb final state using proton-proton collisions at s = 13 TeVA search for ZZ and ZH production in the bbbb final state is presented, where H is the standard model (SM) Higgs boson. The search uses an event sample of proton-proton…CMS Collaboration·Mar 29, 2024SaveLearn
Measurement of the production cross section of a Higgs boson with large transverse momentum in its decays to a pair of τ leptons in proton-proton collisions at s = 13 TeVA measurement of the production cross section of a Higgs boson with transverse momentum greater than 250 GeV is presented where the Higgs boson decays to a pair of τ leptons. It is based on…CMS Collaboration·Mar 29, 2024SaveLearn
Rare Strange and Charm Decays at LHCbThanks to the large cross-section for the production of strange and charm mesons at the Large Hadron Collider, LHCb has recently performed several new explorations of rare transitions that are highly…Paras Naik·Mar 29, 2024SaveLearn
Direct CP violation in D decays at LHCbThe discovery of CP violation in charm sector in 2019 was a milestone in searches performed over last decades. The ACP measured by LHCb is at the upper end of the Standard Model…Jolanta Brodzicka·Mar 29, 2024SaveLearn
CP violation measurements in three-body charmless B decaysThis study reports CP asymmetry measurements in charmless three-body decays of B mesons, both using the Run II data from proton-proton collisions at a center-of-mass energy of 13…Lucas Falcao·Mar 29, 2024SaveLearn
Handling correlated systematic uncertainties on the CKM angle gammaThe current precision on the CKM angle γ is driven by averages of measurements from multiple final states and multiple experiments. As the next generation of experiments targets a total…Alex Gilman·Mar 29, 2024SaveLearn
Perspectives of Semi-Inclusive Deep-Inelastic ScatteringThis contribution highlights some topics addressed by current and future experiments in Semi-Inclusive Deep-Inelastic Scattering. We concentrate on the programs at 12 and 22 GeV at Jefferson Lab…Anselm Vossen·Mar 28, 2024SaveLearn
New results of γ measurements in ADS and GLW-like decays at LHCbRecent LHCb measurements of the CKM angle γ in ADS and GLW-like decays are presented. One measurement considers B0 D K*0(892) decays with two- and four-body D-decay final states…Seophine Stanislaus·Mar 28, 2024SaveLearn
Measurement of double-differential cross sections for mesonless charged-current muon neutrino interactions on argon with final-state protons using the MicroBooNE detectorCharged-current neutrino interactions with final states containing zero mesons and at least one proton are of high interest for current and future accelerator-based neutrino oscillation experiments.…MicroBooNE collaboration, P. Abratenko, O. Alterkait et al.·Mar 28, 2024SaveLearn
Measuring Solar Neutrinos in the SNO+ DetectorThe SNO+ experiment is a large multi-purpose neutrino detector, currently filled with liquid scintillator. For the first time in a single experiment, SNO+ is able to measure the neutrino oscillation…Daniel Cookman·Mar 28, 2024SaveLearn
The SNO+ Journey to 0ββSNO+ is a large multipurpose experiment with the ultimate goal of searching for the neutrinoless double beta decay in 130Te. After a commissioning phase with water as the target medium,…A. S. Inácio, W. Parker, B. Tam·Mar 28, 2024SaveLearn
RootInteractive tool for multidimensional statistical analysis, machine learning and analytical model validationThe ALICE experiment at CERN LHC is specifically designed for investigating heavy ion collisions. The upgraded ALICE accommodates a tenfold increase in PbPb luminosity and a two-order of magnitude…Marian Ivanov, Marian Ivanov, Giulio Eulise·Mar 28, 2024SaveLearn
Measurement of absolute branching fractions of Ds+ hadronic decaysUsing e+ e- collision data collected at the BESIII detector at center-of-mass energies between 4.128 and 4.226 GeV, corresponding to an integrated luminosity of 7.33~ fb-1, we determine…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Mar 28, 2024SaveLearn
Observation of the semileptonic decays D0→ KS0π-π0 e+ e and D+→ KS0π+π- e+ eBy analyzing e+e- annihilation data corresponding to an integrated luminosity of 2.93 fb-1 collected at a center-of-mass energy of 3.773 GeV with the BESIII detector, the first…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Mar 28, 2024SaveLearn
New Constraints on Exotic Spin-Spin-Velocity-Dependent Interactions with Solid-State Quantum SensorsWe report new experimental results on exotic spin-spin-velocity-dependent interactions between electron spins. We designed an elaborate setup that is equipped with two nitrogen-vacancy (NV) ensembles…Yue Huang, Hang Liang, Man Jiao et al.·Mar 27, 2024SaveLearn
CPT and Lorentz symmetry tests with hydrogen using a novel in-beam hyperfine spectroscopy method applicable to antihydrogen experimentsWe present a Rabi-type measurement of two ground-state hydrogen hyperfine transitions performed in two opposite external magnetic field directions. This puts first constraints at the level of 2.3…Lilian Nowak, Chloe Malbrunot, Martin C. Simon et al.·Mar 26, 2024SaveLearn
Particle identification with machine learning from incomplete data in the ALICE experimentThe ALICE experiment at the LHC measures properties of the strongly interacting matter formed in ultrarelativistic heavy-ion collisions. Such studies require accurate particle identification (PID).…Maja Karwowska, Łukasz Graczykowski, Kamil Deja et al.·Mar 26, 2024SaveLearn
Searches for Higgs boson production through decays of heavy resonancesThe discovery of the Higgs boson has led to new possible signatures for heavy resonance searches at the LHC. Since then, search channels including at least one Higgs boson plus another particle have…CMS Collaboration·Mar 25, 2024SaveLearn