Measurement of the e+e-→ωπ0π0 cross section at center-of-mass energies from 2.0 to 3.08 GeVThe cross section of the process e+e-ωπ0π0 is measured at nineteen center-of-mass energies from 2.0 to 3.08 GeV using data collected with the BESIII detector at the BEPCII…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Dec 30, 2021SaveLearn
Top quark production in association with a vector boson at the LHCCross section measurements of top quark production in association with a vector boson in proton-proton collisions at s=13\,TeV at the CERN LHC provide an important probe of the…Joscha Knolle·Dec 30, 2021SaveLearn
Analysis of the result of the Neutrino-4 experiment in conjunction with other experiments on the search for sterile neutrinos within the framework of the 3 + 1 neutrino modelThe correspondence of the results obtained in the Neutrino-4 experiment with the results of the NEOS, DANSS, STEREO, PROSPECT experiments at reactors, the MiniBooNE, LSND, MicroBoone experiments at…A. P. Serebrov, R. M. Samoilov, M. E. Chaikovskii·Dec 29, 2021SaveLearn
Neutrino interactions at COMETThe experimental search for coherent neutrinoless conversion of muon to electron in the presence of a nucleus, aims to probe the possibility of charged lepton flavour violation. The COMET experiment…D. Mulmule·Dec 29, 2021SaveLearn
Search for non-standard neutrino interactions with 10 years of ANTARES dataNon-standard interactions of neutrinos arising in many theories beyond the Standard Model can significantly alter matter effects in atmospheric neutrino propagation through the Earth. In this paper,…A. Albert, S. Alves, M. André et al.·Dec 29, 2021SaveLearn
Damping signatures at JUNO, a medium-baseline reactor neutrino oscillation experimentWe study damping signatures at the Jiangmen Underground Neutrino Observatory (JUNO), a medium-baseline reactor neutrino oscillation experiment. These damping signatures are motivated by various new…JUNO collaboration, Jun Wang, Jiajun Liao et al.·Dec 29, 2021SaveLearn
Observation of J/ Electromagnetic Dalitz Decays to X(1835), X(2120) and X(2370)Using a sample of about 10 billion J/ events collected at a center-of-mass energy s = 3.097 GeV with the BESIII detector, the electromagnetic Dalitz decays $J/ e+e- π+…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Dec 29, 2021SaveLearn
First Measurement of the c+ p η' decayWe present the first measurement of the branching fraction of the singly Cabibbo-suppressed (SCS) decay c+ p η' with η' ηπ+π-, using a data sample corresponding to…Belle Collaboration, S. X. Li, J. X. Cui et al.·Dec 28, 2021SaveLearn
Search for the decay D0 π0We present the first experimental search for the rare charm decay D0 π0 . It is based on an e+e- collision sample consisting of 10.6×106 pairs of…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Dec 28, 2021SaveLearn
Search for long-lived particles decaying into muon pairs in proton-proton collisions at s = 13 TeV collected with a dedicated high-rate data streamA search for long-lived particles decaying into muon pairs is performed using proton-proton collisions at a center-of-mass energy of 13 TeV, collected by the CMS experiment at the LHC in 2017 and…CMS Collaboration·Dec 27, 2021SaveLearn
New results from the DANSS experimentThe DANSS experiment collected 5.5 million Inverse Beta Decay (IBD) events during 5 years of operation. Data were collected at 3 distances (10.9~m, 11.9~m, and 12.9~m) from the center of the core of…Mikhail Danilov, Nataliya Skrobova·Dec 26, 2021SaveLearn
Probing new physics at the LUXE experimentThe proposed Laser Und XFEL (LUXE) Experiment at DESY, Hamburg, aims to probe QED in the strong field non-perturbative regime. This regime will be created in collisions between high-intensity laser…Arka Santra·Dec 26, 2021SaveLearn
Measurement of e+e-φπ+π- cross sections at center-of-mass energies from 2.00 to 3.08 GeVUsing data corresponding to an integrated luminosity of 651~pb-1 accumulated at 22 center-of-mass energies from 2.00 to 3.08 GeV by the BESIII experiment, the process…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Dec 25, 2021SaveLearn
Search for resonances decaying to three W bosons in the hadronic final state in proton-proton collisions at s = 13 TeVA search for Kaluza-Klein excited vector boson resonances, WKK, decaying in cascade to three W bosons via a scalar radion R, WKK WR WWW, with two or three massive…CMS Collaboration·Dec 24, 2021SaveLearn
Neutrino Tagging, a new tool for accelerator based neutrino experimentsThis article describes a new experimental method for accelerator based neutrino experiments called neutrino tagging. The method consists in exploiting the neutrino production mechanism, the…Mathieu Perrin-Terrin·Dec 23, 2021SaveLearn
Inclusive and differential ttγ measurement in the dilepton channel and effective field theory interpretationThe production cross section of ttγ is measured in the dilepton channel using 138 fb-1 of proton-proton collision data recorded by the CMS experiment at s= 13 TeV during…Gianny Mestdach·Dec 23, 2021SaveLearn
Improvements in Antineutrino Detector Response by Including Fission Product Isomeric Transitions and Corrections using New DataCEvNS detectors could provide new opportunities in nuclear physics applications if they can improve existing parameters such as neutrino detector size, portability, their sensitivity to a large range…Wei Eng Ang, Sanghun Lee, Shikha Prasad·Dec 22, 2021SaveLearn
Probing charm quark dynamics via multiparticle correlations in PbPb collisions at sNN = 5.02 TeVMultiparticle azimuthal correlations of prompt D0 mesons are measured in PbPb collisions at a nucleon-nucleon center-of-mass energy of sNN = 5.02 TeV. For the first time, a…CMS Collaboration·Dec 22, 2021SaveLearn
Emission of Single and Few Electrons in XENON1T and Limits on Light Dark MatterDelayed single- and few-electron emissions plague dual-phase time projection chambers, limiting their potential to search for light-mass dark matter. This paper examines the origins of these events…E. Aprile, K. Abe, F. Agostini et al.·Dec 22, 2021SaveLearn
Search for Higgs boson pair production in the two bottom quarks plus two photons final state in pp collisions at s=13 TeV with the ATLAS detectorSearches are performed for nonresonant and resonant di-Higgs boson production in the bbγγ final state. The data set used corresponds to an integrated luminosity of 139 fb-1 of…ATLAS Collaboration·Dec 22, 2021SaveLearn
Search for a light Higgs boson in single-photon decays of (1S) using (2S) π+ π- (1S) tagging methodWe search for a light Higgs boson (A0) decaying into a τ+τ- or μ+μ- pair in the radiative decays of (1S). The production of (1S) mesons is tagged by…Belle Collaboration, S. Jia, C. P. Shen et al.·Dec 22, 2021SaveLearn
First Directional Measurement of sub-MeV Solar Neutrinos with BorexinoWe report the measurement of sub-MeV solar neutrinos through the use of their associated Cherenkov radiation, performed with the Borexino detector at the Laboratori Nazionali del Gran Sasso. The…M. Agostini, K. Altenmüller, S. Appel et al.·Dec 22, 2021SaveLearn
Measurement of the Cross Section for e+e- hadrons at Energies from 2.2324 to 3.6710 GeVBased on electron-positron collision data collected with the BESIII detector operating at the Beijing Electron Positron Collider II storage rings, the value of…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Dec 22, 2021SaveLearn
Observation of the B0→D*0K+π- and Bs0→D*0K-π+ decaysThe first observations of B0→D*(2007)0K+π- and Bs0→D*(2007)0K-π+ decays are presented, and their branching fractions…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Dec 21, 2021SaveLearn
Determination of the parton distribution functions of the proton using diverse ATLAS data from pp collisions at s = 7, 8 and 13 TeVThis paper presents an analysis at next-to-next-to-leading order in the theory of quantum chromodynamics for the determination of a new set of proton parton distribution functions using diverse…ATLAS Collaboration·Dec 21, 2021SaveLearn