Comparison of the measured atmospheric muon flux with Monte Carlo simulations for the first KM3NeT detection unitsThe KM3NeT Collaboration has successfully deployed its first detection units in the Mediterranean Sea in December 2015 (ARCA) and September 2017 (ORCA). The sample of data collected between September…Piotr Kalaczyński, Rosa Coniglione·Jan 4, 2021SaveLearn
Search for new physics via baryon EDM at LHCPermanent electric dipole moments (EDMs) of fundamental particles provide powerful probes for physics beyond the Standard Model. We propose to search for the EDM of strange and charm baryons at LHC,…L. Henry, D. Marangotto, A. Merli et al.·Jan 4, 2021SaveLearn
Measurements of W and Z Production at =13 TeV with the CMS Experiment at the LHCThis note presents selected measurements of W and Z boson production, carried out with the CMS experiment at the LHC, based on samples of events collected during 2015-2018 physics runs. W boson…B. Bilin·Jan 4, 2021SaveLearn
Results and Prospects of Radiative and Electroweak Penguin Decays at Belle IIRadiative and electroweak penguin mediated decays of B mesons are a great probe for physics beyond the Standard Model of particle physics. Furthermore, recently anomalies on exclusive $b…Yo Sato·Dec 31, 2020SaveLearn
Recent XYZ results at BESIIIBESIII experiment has collected about 20 fb-1 luminosity data between s=3.8 and 4.7 GeV via e+e- collision. In this talk, we present the recent XYZ results at BESIII,…Lianjin Wu·Dec 31, 2020SaveLearn
Measurements of the center-of-mass energies of e+e- collisions at BESIIIDuring the 2016-17 and 2018-19 running periods, the BESIII experiment collected 7.5~fb-1 of e+e- collision data at center-of-mass energies ranging from 4.13 to 4.44 GeV. These data samples…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Dec 29, 2020SaveLearn
Adiabatic Quantum Algorithm for Multijet Clustering in High Energy PhysicsThe currently predicted increase in computational demand for the upcoming High-Luminosity Large Hadron Collider (HL-LHC) event reconstruction, and in particular jet clustering, is bound to challenge…Diogo Pires, Yasser Omar, João Seixas·Dec 28, 2020SaveLearn
Nuclear dependence of light neutral meson production in p-A collisions at 400 GeV with NA60The NA60 experiment has studied low-mass muon pair production in proton-nucleus collisions with a system of Be, Cu, In, W, Pb and U targets, using a 400 GeV proton beam at the CERN SPS. The…R. Arnaldi, K. Banicz, K. Borer et al.·Dec 28, 2020SaveLearn
Vector Bosons and Jets in Proton CollisionsEvents with vector bosons produced in association with jets have been extensively studied at hadron colliders and provide high-accuracy tests of the Standard Model. A good understanding of these…Alessandro Tricoli, Marek Schönherr, Paolo Azzurri·Dec 27, 2020SaveLearn
Slow Control System for PandaX-III experimentThe PandaX-III experiment uses high pressure gaseous time projection chamber to search for the neutrinoless double beta decay of 136Xe. A modular slow control system~(SCS) has been designed to…Xiyu Yan, Xun Chen, Yu Chen et al.·Dec 24, 2020SaveLearn
Angular analysis of the B+→ K+μ+μ- decayWe present an angular analysis of the B+→ K+(→ KS0π+)μ+μ- decay using 9\,fb-1 of pp collision data collected with the LHCb experiment. For…LHCb collaboration, R. Aaij, C. Abellán Beteta et al.·Dec 24, 2020SaveLearn
Measurement of CP violation in the decay B+ → K+ π0A measurement of direct CP violation in the decay B+ → K+ π0 is reported using a data sample corresponding to an integrated luminosity of 5.4 fb-1, collected with…LHCb collaboration, R. Aaij, C. Abellán Beteta et al.·Dec 23, 2020SaveLearn
Measurement of transverse single-spin asymmetries of π0 and electromagnetic jets at forward rapidity in 200 and 500 GeV transversely polarized proton-proton collisionsThe STAR Collaboration reports measurements of the transverse single-spin asymmetry (TSSA) of inclusive π0 at center-of-mass energies ( s) of 200 GeV and 500 GeV in transversely polarized…STAR Collaboration, J. Adam, L. Adamczyk et al.·Dec 21, 2020SaveLearn
Observation of the Bs0 → D D decayA search for the B0s \!→ D* D decay is performed using proton-proton collision data at centre-of-mass energies of 7, 8 and 13\,TeV collected by the LHCb…LHCb collaboration, R. Aaij, C. Abellán Beteta et al.·Dec 21, 2020SaveLearn
Polarised Beams at Future e+e- CollidersBeam polarisation is an integral part of the physics case of future Linear Colliders. In this contribution, important examples from Higgs coupling measurements, top and electroweak physics at high…Jenny List·Dec 21, 2020SaveLearn
Measurement of the absolute branching fraction of Λc+ p K0Sη decaysBased on 586 pb-1 of e+e- annihilation data collected at a center-of-mass energy of s=4.6~GeV with the BESIII detector at the BEPCII collider, the absolute branching…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Dec 21, 2020SaveLearn
Study of e+e- 2(pp) at center-of-mass energies between 4.0 and 4.6 GeVUsing data taken at 23 center-of-mass energies between 4.0 and 4.6 GeV with the BESIII detector at the BEPCII collider and with a total integrated luminosity of approximately 15 fb-1, the…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Dec 21, 2020SaveLearn
Kinematic Edge Detection Using Finite Impulse Response FiltersVarious physics observables can be determined from the localisation of distinct edge-like features in distributions of measurement values. In this paper, we address the observation that neither…Mikael Berggren, Stefano Caiazza, Madalina Chera et al.·Dec 21, 2020SaveLearn
First Results from Axion Haloscope at CAPP around 10.7 μeVThe Center for Axion and Precision Physics research at the Institute for Basic Science is searching for axion dark matter using ultra-low temperature microwave resonators. We report the exclusion of…Ohjoon Kwon, Doyu Lee, Woohyun Chung et al.·Dec 19, 2020SaveLearn
Proposal: JSNS2-IIThis article describes the goal and expected sensitivity of the JSNS2-II experiment at J-PARC Materials and Life Science Experimental Facility (MLF). The JSNS2-II experiment is the second phase…S. Ajimura, M. Botran, J. H. Choi et al.·Dec 19, 2020SaveLearn
Evidence of a J/ψ structure and observation of excited - states in the b- J/ψ K- decayFirst evidence of a structure in the J/ψ invariant mass distribution is obtained from an amplitude analysis of b- J/ψ K- decays. The observed structure is…LHCb collaboration, R. Aaij, C. Abellán Beteta et al.·Dec 18, 2020SaveLearn
New results from the DANSS experimentWe present new preliminary DANSS results based on 3.5 million Inverse Beta Decay (IBD) events collected at 3 distances (10.9 m, 11.9 m, and 12.9 m) from the detector center to the reactor core…Mikhail Danilov·Dec 18, 2020SaveLearn
ILC as a SUSY discovery and precision instrumentData from the LHC at 7, 8, and 13 TeV have so far yielded no evidence for new particles beyond the 125 GeV Higgs boson; in particular, there have been no signs of SUSY. However, the complementary…María Teresa Núñez Pardo de Vera·Dec 18, 2020SaveLearn
Measurement of C\!P observables in B D(*) K and B D(*) π decays using two-body D final statesMeasurements of C\!P observables in B → D(*) K and B → D(*) π decays are presented, where D(*) indicates a neutral D or D* meson that is an…LHCb collaboration, R. Aaij, C. Abellán Beteta et al.·Dec 17, 2020SaveLearn
Neutrino Energy Estimation in Neutral Current Interactions and Prospects for Sterile Neutrino SearchesModern neutrino detectors, particularly the large liquid argon time projection chambers (LAr TPCs) at SBN and DUNE, provide an unprecedented amount of information about GeV-scale interactions. By…Andrew P. Furmanski, Christopher Hilgenberg·Dec 17, 2020SaveLearn