Jet Energy Scale and Resolution Measurements in CMSMeasurements of jet energy scale (JES) and resolution (JER) are presented, based on the legacy reconstruction of 13 TeV proton-proton collision data collected by the CMS experiment during the LHC Run…Garvita Agarwal·Jan 5, 2023SaveLearn
Transverse-spin-dependent azimuthal asymmetries of pion and kaon pairs produced in muon-proton and muon-deuteron semi-inclusive deep inelastic scatteringA set of measurements of azimuthal asymmetries in the production of pairs of identified hadrons in deep-inelastic scattering of muons on transversely polarised 6LiD (deuteron) and NH3 (proton)…The COMPASS Collaboration·Jan 5, 2023SaveLearn
An Improved Method of Estimating the Uncertainty of Air-Shower Size at Ultra-High EnergiesThe collection of a statistically significant number detected of cosmic rays with energy above 1017 to 1018 eV requires widely-spaced particle detectors at the ground level to detect the…Alan Coleman, Pierre Billoir, Oliver Deligny·Jan 4, 2023SaveLearn
Heavy-flavour production at the LHCHeavy flavour production measurements in pp collisions are a crucial test of QCD. The LHC experiments ALICE, ATLAS, CMS and LHCb, provide complementary abilities to measure many aspects of…Jaime Norman·Jan 2, 2023SaveLearn
Quarkonia production in ultra-peripheral PbPb collisions at LHCbMeasurements of coherent charmonium production cross sections together with their ratio in ultra-peripheral PbPb collisions are studied at a nucleon-nucleon centre-of-mass energy of…Xiaolin Wang·Dec 31, 2022SaveLearn
Neutron capture-induced nuclear recoils as background for CE~measurements at reactorsNuclear reactors represent a promising neutrino source for CE (coherent-elastic neutrino-nucleus scattering) searches. However, reactor sites also come with high ambient neutron flux. Neutron…A. J. Biffl, A. Gevorgian, K. Harris et al.·Dec 29, 2022SaveLearn
Dark matter searches and energy accumulation and release in materialsEfforts to identify dark matter by detecting nuclear recoils produced by dark matter particles reveal low-energy backgrounds of unknown origin in different types of detectors. In many cases, energy…Sergey Pereverzev·Dec 28, 2022SaveLearn
Measurement of branching fraction of D*+s D+s π0 relative to D*+s D+s γBased on 7.33 fb-1 of e+e- collision data taken at center-of-mass energies between 4.128 and 4.226 GeV with the BESIII detector, we measure the branching fraction of D*+s D+sπ0…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Dec 27, 2022SaveLearn
Performance of the 1-ton Prototype Neutrino Detector at CJPL-IChina Jinping Underground Laboratory provides an ideal site for solar, geo-, and supernova neutrino studies. With a prototype neutrino detector running since 2017, containing 1-ton liquid…Yiyang Wu, Jinjing Li, Shaomin Chen et al.·Dec 26, 2022SaveLearn
Measurement of the absolute branching fraction of the inclusive decay Ds+ π+π+π- XUsing an e+ e- collision data sample with a total integrated luminosity of 3.19 fb-1 collected with the BESIII detector at a center-of-mass energy of 4.178 GeV, the branching fraction of…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Dec 26, 2022SaveLearn
Search for effective Lorentz and CPT violation using ZEUS dataLorentz and CPT symmetry in the quark sector of the Standard Model are studied in the context of an effective field theory using ZEUS e p data. Symmetry-violating effects can lead to…ZEUS collaboration, I. Abt, R. Aggarwal et al.·Dec 24, 2022SaveLearn
Measurement of production in pp collisions at s=5 \ TeVThe production cross-sections of mesons, namely (1S), (2S) and (3S), in pp collisions at s=5 \ TeV are measured with a data sample…LHCb collaboration·Dec 24, 2022SaveLearn
Search for new physics in the τ lepton plus missing transverse momentum final state in proton-proton collisions at s = 13 TeVA search for physics beyond the standard model (SM) in the final state with a hadronically decaying tau lepton and a neutrino is presented. This analysis is based on data recorded by the CMS…CMS Collaboration·Dec 23, 2022SaveLearn
Measurement of the electroweak production of Wγ in association with two jets in proton-proton collisions at s = 13 TeVA measurement is presented for the electroweak production of a W boson, a photon (γ), and two jets (j) in proton-proton collisions. The leptonic decay of the W boson is selected by requiring…CMS Collaboration·Dec 23, 2022SaveLearn
First observation and branching fraction measurement of the b0 Ds- p decayThe first observation of the b0 Ds- p decay is presented using proton-proton collision data collected by the LHCb experiment at a centre-of-mass energy of $s=13…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Dec 23, 2022SaveLearn
Observation of (3770)η J/The Born cross section of the process e+e-η J/ at a center-of-mass energy s=3.773 ~GeV is measured to be (8.890.880.42)~pb, using a data sample…BESIII Collaboration·Dec 23, 2022SaveLearn
Towards a possible discovery of dark photons with a multi-cathode counterThe main points of experiment on the search of dark photons using multy-cathode counter are outlined. The evidence base to prove that the observed effect is really from dark photons is formulated.…A. Kopylov, I. Orekhov, V. Petukhov·Dec 22, 2022SaveLearn
Proposal for the search for exotic spin-spin interactions at the micrometer scale using functionalized cantilever force sensorsSpin-dependent exotic interactions can be generated by exchanging hypothetical bosons, which were introduced to solve some puzzles in physics. Many precision experiments have been performed to search…Qian Wang, Ze Ouyang, Yu Lu et al.·Dec 22, 2022SaveLearn
Measurement of natPb(e,Xn) production with a stopped-pion neutrino sourceUsing neutrinos produced at the Spallation Neutron Source (SNS) at Oak Ridge National Laboratory (ORNL), the COHERENT collaboration has studied the Pb(e,Xn) process with a lead…COHERENT Collaboration, P. An, C. Awe et al.·Dec 21, 2022SaveLearn
Search for rare decays of D0 mesons into two muonsA search for the very rare D0 μ+μ- decay is performed using data collected by the LHCb experiment in proton-proton collisions at s = 7, 8 and 13~TeV, corresponding to an…LHCb collaboration·Dec 21, 2022SaveLearn
Graph Clustering: a graph-based clustering algorithm for the electromagnetic calorimeter in LHCbThe recent upgrade of the LHCb experiment pushes data processing rates up to 40 Tbit/s. Out of the whole reconstruction sequence, one of the most time consuming algorithms is the calorimeter…Núria Valls Canudas, Míriam Calvo Gómez, Xavier Vilasís-Cardona et al.·Dec 21, 2022SaveLearn
Recent results from DANSSDANSS is a solid state scintillator neutrino spectrometer placed at a small distance from the commercial nuclear reactor of Kalininskaya NPP. The distance from the detector to the center of the…Igor Alekseev·Dec 21, 2022SaveLearn
Outreach Modules for New Particle Searches Using the ATLAS Forward Proton Detector and for Higgs Boson PhysicsWe present two modules as part of the Czech Particle Physics Project (CPPP). These modules are intended as learning tools in masterclasses aimed at high-school students (aged 15 to 18). The first…Andre Sopczak·Dec 21, 2022SaveLearn
Search for Light Neutral Bosons in the TREK/E36 Experiment at J-PARCThe Standard Model (SM) represents our best description of the subatomic world and it has been very successful in explaining how elementary particles interact under the influence of the fundamental…Dongwi H. Dongwi·Dec 21, 2022SaveLearn
Measurement of the cosmogenic neutron yield in Super-Kamiokande with gadolinium loaded waterCosmic-ray muons that enter the Super-Kamiokande detector cause hadronic showers due to spallation in water, producing neutrons and radioactive isotopes. Those are a major background source for…Kamiokande Collaboration, M. Shinoki, K. Abe et al.·Dec 21, 2022SaveLearn