New insights into strange-quark hadronization measuring multiple (multi-)strange hadron production in small collision systems with ALICEAmong the most important results from the Run-1 and Run-2 of the LHC is the observation of an enhanced production of (multi-)strange to non-strange hadron yields, gradually rising from…Sara Pucillo·Sep 11, 2024SaveLearn
Measurements of the CP-even fractions of D0π+π-π0 and D0 K+K-π0 at BESIIIThe CP-even fractions (F+) of the decays D0π+π-π0 and D0 K+K-π0 are measured with a quantum-correlated (3770) DD data sample collected by…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Sep 11, 2024SaveLearn
Experimental Summary of the Moriond 2024 conference -- Electroweak Interaction & Unified TheoriesThe proceeding gives a summary of the experimental results presented at the Moriond 2024 conference (electroweak interactions and unified theory session), focussing on the latest measurements. A…Barbara Clerbaux·Sep 11, 2024SaveLearn
LHC beam monitoring via real-time hit reconstruction in the LHCb VELO pixel detectorThe increasing computing power and bandwidth of programmable digital devices opens new possibilities in the field of real-time processing of HEP data. The LHCb collaboration is exploiting these…Daniele Passaro, Giulio Cordova, Federico Lazzari et al.·Sep 10, 2024SaveLearn
Measurement of inclusive and differential cross sections of single top quark production in association with a W boson in proton-proton collisions at s = 13.6 TeVThe first measurement of the inclusive and normalised differential cross sections of single top quark production in association with a W boson in proton-proton collisions at a centre-of-mass energy…CMS Collaboration·Sep 10, 2024SaveLearn
A universal implementation of radiative effects in neutrino event generatorsDue to the similarities between electron-nucleus (eA) and neutrino-nucleus scattering ( A), eA data can contribute key information to improve cross-section modeling in eA and hence in $…Julia Tena Vidal, Adi Ashkenazi, Larry B. Weinstein et al.·Sep 9, 2024SaveLearn
First determination of the spin-parity of c(3055)+,0 baryonsThe b0(-)c(3055)+(0)( D+(0))π- decay chains are observed, and the spin-parity of c(3055)+(0) baryons is determined for the first time.…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Sep 9, 2024SaveLearn
Germanium and Silicon Detectors for WIMP Searches: Key Experimental InsightsDark matter plays a crucial role in our comprehension of the universe, but its mysterious nature poses challenges for direct detection. A primary obstacle in detecting dark matter is distinguishing…M. Mirzakhani, S. Maludze·Sep 9, 2024SaveLearn
Dual-Baseline Search for Active-to-Sterile Neutrino Oscillations in NOvAWe report a search for neutrino oscillations to sterile neutrinos under a model with three active and one sterile neutrinos (3+1 model). This analysis uses the NOvA detectors exposed to the NuMI…The NOvA Collaboration·Sep 6, 2024SaveLearn
Study of the decay D0→ (770)-e+eWe present a study of the semileptonic decay D0→ π-π0e+e using an e+e- annihilation data sample of 7.93~fb-1 collected at the center-of-mass energy of…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Sep 6, 2024SaveLearn
Study of neutron production for 360 GeV cosmic muonsThe China Jinping underground Laboratory (CJPL) is an excellent location for studying solar, terrestrial, and supernova neutrinos due to its 2400-meter vertical rock overburden. Its unparalleled…Xinshun Zhang, Jinjing Li, Shaomin Chen et al.·Sep 6, 2024SaveLearn
Multiplicity dependent J/ and (2S) production at forward and backward rapidity in p+p collisions at s=200 GeVThe J/ and (2S) charmonium states, composed of cc quark pairs and known since the 1970s, are widely believed to serve as ideal probes to test quantum chromodynamics in high-energy…PHENIX Collaboration, N. J. Abdulameer, U. Acharya et al.·Sep 5, 2024SaveLearn
Measurement of exclusive J/ and (2S) production at s=13 TeVMeasurements are presented of the cross-section for the central exclusive production of J/μ+μ- and (2S)μ+μ- processes in proton-proton collisions at s = 13 TeV…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Sep 5, 2024SaveLearn
Measurement of CP violation in B0→D+D- and B0s→D+sD-s decaysA time-dependent, flavour-tagged measurement of CP violation is performed with B0→D+D- and B0s→D+sD-s decays, using data collected by the…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Sep 4, 2024SaveLearn
Measurement of b0, c+ and decay parameters using b0 c+ h- decaysA comprehensive study of the angular distributions in the bottom-baryon decays 0bc+ h-(h=π, K), followed by c+ h+ with…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Sep 4, 2024SaveLearn
Search for the massless dark photon with D0ωγ' and D0γγ'Using 7.9~fb-1 of e+e- collision data collected at s=3.773 GeV with the BESIII detector at the BEPCII collider, we search for the massless dark photon with the flavor-changing…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Sep 4, 2024SaveLearn
Search for sub-eV axion-like particles in a quasi-parallel stimulated resonant photon-photon collider with "coronagraphy"Axion-like particles (ALPs) have been searched for with a quasi-parallel stimulated resonant photon-photon collider sensitive to the sub-eV mass range by focusing two-color near-infrared pulse lasers…Yuri Kirita, Airi Kodama, Kensuke Homma et al.·Sep 3, 2024SaveLearn
First search for K+π0πμ e decaysThe first search for the lepton number violating decay K+π0π-μ+e+ and lepton flavour violating decays K+π0π+μ-e+, K+π0π+μ+e- has been performed using a…NA62 collaboration·Sep 3, 2024SaveLearn
A novel machine learning method to detect double- hypernuclear events in nuclear emulsionsA novel method was developed to detect double- hypernuclear events in nuclear emulsions using machine learning techniques. The object detection model, the Mask R-CNN, was trained using…Yan He, Vasyl Drozd, Hiroyuki Ekawa et al.·Sep 3, 2024SaveLearn
Study of D+ KS0K*(892)+ in D+ KS0 KS0 π+Using a data sample of e+e- collisions corresponding to an integrated luminosity of 7.93 fb-1 collected with the BESIII detector at the center-of-mass energy 3.773~GeV, we perform the…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Sep 2, 2024SaveLearn
Measurement of C\!P violation observables in D+→ K-K+π+ decaysA search for violation of the charge-parity C\!P symmetry in the D+→ K-K+π+ decay is presented, with proton-proton collision data corresponding to an integrated luminosity of 5.4…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Sep 2, 2024SaveLearn
First Measurement of Missing Energy Due to Nuclear Effects in Monoenergetic Neutrino Charged Current InteractionsWe present the first measurement of the missing energy due to nuclear effects in monoenergetic, muon neutrino charged-current interactions on carbon, originating from K+ → μ+ μ…E. Marzec, S. Ajimura, A. Antonakis et al.·Sep 2, 2024SaveLearn
Pseudorapidity distributions of charged hadrons in lead-lead collisions at sNN = 5.36 TeVThe pseudorapidity (η) distributions of charged hadrons are measured using data collected at the highest ever nucleon-nucleon center-of-mass energy of sNN = 5.36 TeV for…CMS Collaboration·Sep 1, 2024SaveLearn
Search for MeV-Scale Axionlike Particles and Dark Photons with PandaX-4TAxionlike particles (ALPs) and dark photons (DPs) are viable dark matter particle candidates. We have searched for possible ALP/DP signals in the PandaX-4T liquid xenon detector using 440 kg·yr…PandaX Collaboration, Tao Li, Zihao Bo et al.·Sep 1, 2024SaveLearn
Measurement of Born cross sections of e+e-00 and search for charmonium(-like) states at s = 3.51-4.95 GeVUsing e+e- collision data collected by the BESIII detector at BEPCII corresponding to an integrated luminosity of 30 fb-1, we measure Born cross sections and effective form factors for…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Aug 31, 2024SaveLearn