Reconstructing the Kinematics of Deep Inelastic Scattering with Deep LearningWe introduce a method to reconstruct the kinematics of neutral-current deep inelastic scattering (DIS) using a deep neural network (DNN). Unlike traditional methods, it exploits the full kinematic…Miguel Arratia, Daniel Britzger, Owen Long et al.·Oct 11, 2021SaveLearn
Measurement of the energy asymmetry in ttj production at 13 TeV with the ATLAS experiment and interpretation in the SMEFT frameworkA measurement of the energy asymmetry in jet-associated top-quark pair production is presented using 139 fb-1 of data collected by the ATLAS detector at the Large Hadron Collider during…ATLAS Collaboration·Oct 11, 2021SaveLearn
Measurements of inclusive photons at forward rapidities in p-Pb collisions at sNN = 5.02 TeV with ALICEWe present multiplicity and pseudorapidity distributions of inclusive photons at forward rapidity in proton-lead (p-Pb) collisions at sNN = 5.02 TeV using the data obtained from Photon…Abhi Modak·Oct 11, 2021SaveLearn
Precision measurements of jet production at the ATLAS experimentMeasurements of jet production are sensitive to the strong coupling constant, high order perturbative calculations and parton distribution functions. In this talk we present the most recent ATLAS…Francesco Giuli·Oct 11, 2021SaveLearn
Analysis of the CP structure of the Yukawa coupling between the Higgs boson and τ leptons in proton-proton collisions at s = 13 TeVThe first measurement of the CP structure of the Yukawa coupling between the Higgs boson and τ leptons is presented. The measurement is based on data collected in proton-proton collisions at…CMS Collaboration·Oct 10, 2021SaveLearn
Search for long-lived particles decaying to leptons with large impact parameter in proton-proton collisions at s = 13 TeVA search for new long-lived particles decaying to leptons using proton-proton collision data produced by the CERN LHC at s = 13 TeV is presented. Events are selected with two leptons (an…CMS Collaboration·Oct 10, 2021SaveLearn
Measurement of the e+e-Σ0Σ0 cross sections at center-of-mass energies from 2.3864 to 3.0200 GeVThe Born cross sections of e+e- Σ0Σ0 are measured at center-of-mass energies from 2.3864 to 3.0200 GeV using data samples with an integrated luminosity of 328.5 pb-1…M. Ablikim, M. N. Achasov, P. Adlarson et al.·Oct 9, 2021SaveLearn
Observation of two new excited b0 states decaying to b0 K-π+Two narrow resonant states are observed in the b0 K-π+ mass spectrum using a data sample of proton-proton collisions at a center-of-mass energy of 13~ TeV, collected by the…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Oct 9, 2021SaveLearn
Probing gluon helicity with heavy flavor at the EICWe propose a new measurement of the heavy flavor hadron double spin asymmetry in deep-inelastic scattering at a future Electron-Ion Collider (EIC) to constrain the polarized gluon distribution…Daniele Paolo Anderle, Xin Dong, Felix Hekhorn et al.·Oct 9, 2021SaveLearn
Search for the decay B0→ K 0τ+τ- at the Belle experimentThis letter presents a search for the rare flavor-changing neutral current process B0→ K 0τ+τ- using data taken with the Belle detector at the KEKB asymmetric energy…Belle Collaboration, T. V. Dong, T. Luo et al.·Oct 8, 2021SaveLearn
Experimental estimates of the photon background in a potential light-by-light scattering studyHigh power short pulse lasers provide a promising route to study the strong field effects of the quantum vacuum, for example by direct photon-photon scattering in the all-optical regime. Theoretical…Leonard Doyle, Pooyan Khademi, Peter Hilz et al.·Oct 7, 2021SaveLearn
Observation of D0(+) K0Sπ0(+)ω and improved measurement of D0 K-π+ωBy analyzing an e+e- annihilation data sample with an integrated luminosity of 2.93\ fb-1 taken at the center-of-mass energy of 3.773 GeV with the BESIII detector, we determine the…M. Ablikim, M. N. Achasov, P. Adlarson et al.·Oct 7, 2021SaveLearn
Measurement of the B- -> D0 l- nubarl Branching Fraction in 62.8/fb of Belle II dataWe report a measurement of the branching fraction of the semileptonic decay B- -> D0 l- nubarl (and its charge conjugate) using 62.8/fb of Upsilon(4S) -> B Bbar data recorded by the Belle II…Belle II Collaboration·Oct 6, 2021SaveLearn
Modelling the Data at the LHCMeasurements at hadron colliders rely on large scale quantum chromodynamics (QCD) Monte Carlo (MC) production for interpretation of the data. MC simulations allow testing Standard Model (SM) with…Efe Yazgan·Oct 6, 2021SaveLearn
Simultaneous determination of CKM angle γ and charm mixing parametersA combination of measurements sensitive to the CP violation angle γ of the Cabibbo-Kobayashi-Maskawa unitarity triangle and to the charm mixing parameters that describe oscillations between D0…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Oct 5, 2021SaveLearn
Light, Unstable Sterile Neutrinos: Phenomenology, a Search in the IceCube Experiment, and a Global PictureLongstanding anomalies in neutrino oscillation experiments point to the existence of a fourth, hypothetical neutrino: the sterile neutrino. Global fits to a sterile neutrino model find a strong…Marjon H. Moulai·Oct 5, 2021SaveLearn
Muχe -- A Search for Familons in Muon Decay Using HPGe DetectorsA broken lepton family symmetry can lead to muon decay to a Familon \[μ χFamilon + e .\] We propose to search for two body muon decay to a Familon in the mass range from 86 to 105 MeV/c2,…D . Koltick, S. Huang, F. Bergin et al.·Oct 5, 2021SaveLearn
New Constraints on Dark Photon Dark Matter with Superconducting Nanowire Detectors in an Optical HaloscopeUncovering the nature of dark matter is one of the most important goals of particle physics. Light bosonic particles, such as the dark photon, are well-motivated candidates: they are generally…Jeff Chiles, Ilya Charaev, Robert Lasenby et al.·Oct 4, 2021SaveLearn
Thin Film (High Temperature) Superconducting Radiofrequency Cavities for the Search of Axion Dark MatterThe axion is a hypothetical particle which is a candidate for cold dark matter. Haloscope experiments directly search for these particles in strong magnetic fields with RF cavities as detectors. The…J. Golm, S. Arguedas Cuendis, S. Calatroni et al.·Oct 4, 2021SaveLearn
Mixing and C\!P violation in charm decays at LHCbThe LHCb experiment has collected the world's largest sample of charmed hadrons. This sample is used to measure observables related to D0 -D0 mixing, direct C\!P violation and…Federico Betti·Oct 3, 2021SaveLearn
Charm and multi-charm baryon measurements via strangeness tracking with the upgraded ALICE detectorWe present a new method for detection of multiply charmed baryons via their decays into strange baryons, using `strangeness tracking'. This method makes use of the state-of-the-art upgraded…David Dobrigkeit Chinellato·Oct 3, 2021SaveLearn
Improved experimental layout for dipole moment measurements at the LHCThe electric and magnetic dipole moment of charm and bottom baryons can be measured for the first time by using bent crystal technology at the LHC. The experimental method, proposed in recent years,…V. M. Biryukov, J. Ruiz Vidal·Oct 2, 2021SaveLearn
Punzi-loss: A non-differentiable metric approximation for sensitivity optimisation in the search for new particlesWe present the novel implementation of a non-differentiable metric approximation and a corresponding loss-scheduling aimed at the search for new particles of unknown mass in high energy physics…P. Feichtinger, H. Haigh, G. Inguglia et al.·Oct 2, 2021SaveLearn
B-flavor tagging at Belle IIWe report on new flavor tagging algorithms developed to determine the quark-flavor content of bottom (B) mesons at Belle II. The algorithms provide essential inputs for measurements of quark-flavor…F. Abudinén, N. Akopov, A. Aloisio et al.·Oct 2, 2021SaveLearn
Study of the reactions e+e-π+π-π0π0π0π0 and π+π-π0π0π0η at center-of-mass energies from threshold to 4.5 GeV using initial-state radiationWe study the processes e+e-π+π-π0π0π0π0γ and e+e-π+π-π0π0π0ηγ in which an energetic photon is radiated from the initial state. The data were collected with the BaBar detector…BaBar Collaboration·Oct 2, 2021SaveLearn