Searching for new physics in WW and single-W eventsPair-production and single-production of W bosons provide many opportunities to look for new physics via precision measurements, for instance via scrutinising the involved triple-gauge vertices or…Jenny List, Ulrich Einhaus, Andre Filipe Silva et al.·Oct 19, 2024SaveLearn
Dark matter searches at BESIIIDark matter (DM) is a new type of invisible matter introduced to explain various features of recent astrophysical observations, including galaxy rotation curves and other fundamental characteristics…Vindhyawasini Prasad·Oct 19, 2024SaveLearn
The application of Hough transform for fast interaction vertex position estimation in heavy-ion collisionsCharged particle track reconstruction in silicon detectors of collider experiments in high-multiplicity events, such as heavy-ion collisions at LHC, is a difficult and resource-demanding process. The…Petr Balek, Tomasz Bold, Michal Naworyta·Oct 18, 2024SaveLearn
Exploring jets: substructure and flavour tagging in CMS and ATLASThe identification and characterization of jets are crucial tasks for effectively probing fundamental particle interactions. The ATLAS and CMS experiments have developed cutting-edge techniques to…Andrea Malara·Oct 18, 2024SaveLearn
Test of lepton flavour universality with Bs0 → φ +- decaysLepton flavour universality in rare b→ s transitions is tested for the first time using Bs0 meson decays. The measurements are performed using pp collision data collected by the…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Oct 17, 2024SaveLearn
Signal partitioning in superfluid 4He: a Monte Carlo approachSuperfluid 4He is an ideal candidate for the direct detection of light dark matter via nuclear recoils thanks to its low nuclear mass and the possibility to reach a low detection energy…Francesco Toschi, Axel Brunold, Lea Burmeister et al.·Oct 17, 2024SaveLearn
Observation of a rare beta decay of the charmed baryon with a Graph Neural NetworkThe beta decay of the lightest charmed baryon c+ provides unique insights into the fundamental mechanism of strong and electro-weak interactions, serving as a testbed for investigating…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Oct 17, 2024SaveLearn
Observation of c0+-η and evidence for c1,2+-ηUsing (27.12 0.14)×108 (3686) events collected with the BESIII detector, the decay c0+-η is observed for the first time with a statistical…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Oct 17, 2024SaveLearn
Observation of the Singly Cabibbo-Suppressed Decay c+ pπ0Utilizing 4.5~fb-1 of e+e- annihilation data collected with the BESIII detector at the BEPCII collider at center-of-mass energies between 4.600 and 4.699 GeV, the first observation of…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Oct 17, 2024SaveLearn
Measurement of attenuation length of the muon content in extensive air showers from 0.3 to 30 PeV with LHAASOThe attenuation length of the muon content in extensive air showers provides important information regarding the generation and development of air showers. This information can be used not only to…The LHAASO Collaboration, Zhen Cao, F. Aharonian et al.·Oct 17, 2024SaveLearn
Search for e+e- φ c0 and φηc2(1D) at center-of-mass energies from 4.47 to 4.95 GeVUtilizing a data set of 6.7 fb-1 from electron-positron collisions recorded by the BESIII detector at the BEPCII storage ring, a search is conducted for the processes $e+e- φ…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Oct 16, 2024SaveLearn
Multiplicities of positive and negative pions, kaons and unidentified hadrons from deep-inelastic scattering of muons off a liquid hydrogen targetThe multiplicities of positive and negative pions, kaons and unidentified hadrons produced in deep-inelastic scattering are measured in bins of the Bjorken scaling variable x, the relative…G. D. Alexeev, M. G. Alexeev, C. Alice et al.·Oct 15, 2024SaveLearn
Observation of cJ p p K0S K- π+ + c.c.By analyzing (27.120.14)×108 (3686) events collected with the BESIII detector operating at the BEPCII collider, the decays of $cJ p p K0S K- π+ +c.c.(J=0, 1,…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Oct 15, 2024SaveLearn
Application of Particle Transformer to quark flavor tagging in the ILC projectInternational Linear Collider (ILC) is a next-generation e+e- linear collider to explore Beyond-Standard-Models by precise measurements of Higgs bosons. Jet flavor tagging plays a vital role in…Risako Tagami, Taikan Suehara, Masaya Ishino·Oct 15, 2024SaveLearn
A Proposal for the Lohengrin Experiment to Search for Dark Sector Particles at the ELSA AcceleratorWe present a proposal for a future light dark matter search experiment at the Electron Stretcher Accelerator ELSA in Bonn: Lohengrin. It employs the fixed-target missing momentum based technique for…Philip Bechtle, Christian Bespin, Dominique Breton et al.·Oct 14, 2024SaveLearn
Top quark properties measurements and searches at ATLAS and CMSTheoretical predictions for processes involving top quarks, such as top quark-antiquark pair production, depend on fundamental standard model (SM) parameters like the top quark mass or potentially…Sebastian Wuchterl·Oct 14, 2024SaveLearn
Shining Light on the Dark Sector: Search for Axion-like Particles and Other New Physics in Photonic Final States with FASERThe first FASER search for a light, long-lived particle decaying into a pair of photons is reported. The search uses LHC proton-proton collision data at s=13.6~TeV collected in 2022…FASER collaboration, Roshan Mammen Abraham, Xiaocong Ai et al.·Oct 14, 2024SaveLearn
Development and commissioning of a new readout system for the gas flow of the Belle II KL0 and muon detectorWe have designed and commissioned a new readout board to detect photosensor signals from gas-bubbler panels to continuously monitor the gas flow through the resistive plate chambers of the KL0…Travis Applegate, Noah Brenny, Chunhui Chen et al.·Oct 14, 2024SaveLearn
Measurement of the double-differential cross section of muon-neutrino charged-current interactions with low hadronic energy in the NOvA Near DetectorThe NOvA collaboration reports cross-section measurements for μ charged-current interactions with low hadronic energy (maximum kinetic energy of 250 MeV for protons and 175 MeV for pions)…M. A. Acero, B. Acharya, P. Adamson et al.·Oct 14, 2024SaveLearn
Search for heavy long-lived charged particles with large ionization energy loss in proton-proton collisions at s = 13 TeVA search for heavy, long-lived, charged particles with large ionization energy loss within the silicon tracker of the CMS experiment is presented. A data set of proton-proton collisions at a center…CMS Collaboration·Oct 11, 2024SaveLearn
Observation of time-dependent CP violation and measurement of the branching fraction of B0 J/ π0 decaysWe present a measurement of the branching fraction and time-dependent charge-parity (CP) decay-rate asymmetries in B0 J/ π0 decays. The data sample was collected with the Belle~II…Belle II Collaboration, I. Adachi, L. Aggarwal et al.·Oct 11, 2024SaveLearn
Observation of D+ημ+μ and First Study of D+ η + Decay DynamicsUsing 20.3\, fb-1 of e+e- collision data collected at the center-of-mass energy 3.773\,GeV with the BESIII detector, we report the first observation of the semileptonic decay $D+…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Oct 11, 2024SaveLearn
DUNE's low energy physics searchesThe Deep Underground Neutrino Experiment (DUNE) is a long-baseline neutrino experiment that will precisely measure neutrino oscillation parameters, observe astrophysical neutrinos, and search for…Sergio Manthey Corchado·Oct 10, 2024SaveLearn
New measurement of transverse spin effects in (di-)hadron production from muon-deuteron semi-inclusive DIS at COMPASSThe COMPASS experiment is a fixed-target high-energy physics experiment that has been collecting data for 20 years (2002 to 2022) at the M2 beamline (SPS, North Area) at CERN. One of the goals of the…Siranush Asatryan·Oct 10, 2024SaveLearn
Precision Measurement of the Branching Fraction of D+ μ+μUsing 20.3~fb-1 of e+e- collision data collected at a center-of-mass energy of E c.m.=3.773 GeV with the BESIII detector operating at the BEPCII collider, we determine the…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Oct 10, 2024SaveLearn