Measurements of single top quark production processes with the ATLAS and CMS experimentsThis report contains a brief summary of the latest single top quark production cross-section measurements performed by the ATLAS and CMS collaborations on pp collisions collected during Run 2 of the…Laura Pintucci·Jan 15, 2024SaveLearn
Final CONUS results on coherent elastic neutrino-nucleus scattering at the Brokdorf reactorThe Conus experiment studies coherent elastic neutrino-nucleus scattering in four 1 kg germanium spectrometers. Low ionization energy thresholds of 210 eV were achieved. The detectors were operated…N. Ackermann, H. Bonet, A. Bonhomme et al.·Jan 15, 2024SaveLearn
Summary of CMS Higgs PhysicsSince the discovery of the Higgs boson in 2012, substantial advancements have been achieved in exploring its characteristics. The utilization of extensive data sets has facilitated recent results,…Walaa Elmetenawee·Jan 15, 2024SaveLearn
DNN-based identification of additional b jets for a differential ttbb cross section measurementIn differential measurements of the ttbb process, observables related to the b jets not originating from top quark decays are of special interest to probe the multi-scale QCD nature of…Juhee Song·Jan 15, 2024SaveLearn
Nonproportionality of NaI(Tl) Scintillation Detector for Dark Matter Search ExperimentsWe present a comprehensive study of the nonproportionality of NaI(Tl) scintillation detectors within the context of dark matter search experiments. Our investigation, which integrates COSINE-100 data…S. M. Lee, G. Adhikari, N. Carlin et al.·Jan 15, 2024SaveLearn
CKM and CPV measurements in the beauty and charm sectorMeasurements of CKM elements and CP-violating observables are sensitive to revealing effects beyond the SM. These proceedings discuss four recent LHCb results. The first one presents CP violation…Lei Hao·Jan 15, 2024SaveLearn
CMS highlights on searches for new physics in final states with jetsMany new physics models, e.g., leptoquarks, extra dimensions, extended Higgs sectors, supersymmetric theories, and dark sector extensions, are expected to manifest themselves in the final states with…Emmanouil Vourliotis·Jan 13, 2024SaveLearn
Test of lepton flavor universality in B Kμ+μ- and B Ke+e- decays in proton-proton collisions at s = 13 TeVA test of lepton flavor universality in B Kμ+μ- and B Ke+e- decays, as well as a measurement of differential and integrated branching fractions…CMS Collaboration·Jan 13, 2024SaveLearn
Measurement of Solar pp Neutrino Flux using Electron Recoil Data from PandaX-4T Commissioning RunThe proton-proton (pp) fusion chain dominates the neutrino production from the Sun. The uncertainty of the predicted pp neutrino flux is at the sub-percent level, whereas that of the best…PandaX Collaboration, Xiaoying Lu, Abdusalam Abdukerim et al.·Jan 13, 2024SaveLearn
Inclusive and differential cross section measurements of ttbb production in the lepton+jets channel at s = 13 TeVDifferential cross section measurements of the associated production of top quark and b quark pairs, ttbb, are presented. The results are based on data from…Emanuel Pfeffer·Jan 12, 2024SaveLearn
Central exclusive production in CMS+TOTEMThe central exclusive production of charged hadron pairs in pp collisions at a centre-of-mass energy of 13 TeV is examined, based on data collected in a special high-β* run of the LHC. Events…Ferenc Siklér·Jan 12, 2024SaveLearn
The PANDA Barrel DIRCThe PANDA experiment at the international accelerator Facility for Antiproton and Ion Research in Europe (FAIR), Darmstadt, Germany, will address fundamental questions of hadron physics using…R. Dzhygadlo, A. Belias, A. Gerhardt et al.·Jan 12, 2024SaveLearn
The ATLAS Trigger System for LHC Run 3 and Trigger performance in 2022The ATLAS trigger system is a crucial component of the ATLAS experiment at the LHC. It is responsible for selecting events in line with the ATLAS physics programme. This paper presents an overview of…ATLAS Collaboration·Jan 12, 2024SaveLearn
Physics perspectives of a CMS near-beam proton spectrometer at the HL-LHCThe High-Luminosity Large Hadron Collider (HL-LHC) is designed to achieve higher instantaneous luminosities, enabling the exploration of the rarest processes of the Standard Model (SM). The CMS…Michael Pitt·Jan 12, 2024SaveLearn
Performance study of the JadePix-3 telescope from a beam testWe present the results of a beam test conducted on a telescope using the JadePix-3 pixel sensor, developed with TowerJazz 180 nm CMOS imaging technology. The telescope is composed of five planes,…Sheng Dong, Zhiliang Chen, Jia Zhou et al.·Jan 12, 2024SaveLearn
Search for + in KLp K+n reaction in KLF at JLabThe possibility of the existence of multiquark hadrons made of 4-quark for mesons and 5-quark for baryons was predicted by Gell-Mann in Ref. [1]. The renewed interest for the search of exotic…Moskov J. Amaryan, Shu Hirama, Daisuke Jido et al.·Jan 11, 2024SaveLearn
First observation of the decay +c nK0Sπ+π0Based on 4.5 fb-1 of e+e- collision data accumulated at center-of-mass energies between 4599.53 MeV and 4698.82 MeV with the BESIII detector, the decay $c+…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jan 11, 2024SaveLearn
Measurement of the total and differential cross-sections of ttW production in pp collisions at s=13 TeV with the ATLAS detectorMeasurements of inclusive and differential production cross-sections of a top-quark-top-antiquark pair in association with a W boson (ttW) are presented. They are performed by targeting…The ATLAS Collaboration·Jan 10, 2024SaveLearn
Search for Long-lived Particles at Future Lepton Colliders Using Deep Learning TechniquesLong-lived particles (LLPs) provide an unambiguous signal for physics beyond the Standard Model (BSM). They have a distinct detector signature, with decay lengths corresponding to lifetimes of around…Yulei Zhang, Cen Mo, Xiang Chen et al.·Jan 10, 2024SaveLearn
Search for ηc (2S)π+π-ηc and ηc (2S)π+π-K0S Kπ decaysBased on (27.12 0.14)× 108 (2S) events collected with the BESIII detector, we search for the decay ηc (2S) → π+ π- ηc with $ηc→ KS0…The BESIII Collaboration·Jan 10, 2024SaveLearn
Measurement of Born cross section of e+e-→+- at center-of-mass energies between 3.510 and 4.951 GeVUsing 24.1 fb-1 of e+e- collision data collected with the BESIII detector at the BEPCII collider, the Born cross sections and effective form factors of the…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jan 10, 2024SaveLearn
Top mass measurementsThe top quark mass measurements are based either on a direct kinematic reconstruction of the top quark decay products or on indirect measurements, where an observable sensitive to the top quark mass,…Mikael Myllymäki·Jan 9, 2024SaveLearn
Search for Baryon-Number-Violating Processes in B- Decays to the c0 c- Final StateWe report the results of the first search for B- decays to the c0 c- final state using 711~ fb-1 of data collected at the (4S) resonance…Belle Collaboration, T. Gu, V. Savinov et al.·Jan 9, 2024SaveLearn
Measurements of the branching fraction, polarization, and CP asymmetry for the decay B0→ ω ωWe present a measurement of B0 → ω ω, a charmless decay into two vector mesons, using 772 × 106 BB pairs collected with the Belle detector at the KEKB…Belle Collaboration, Y. Guan, A. J. Schwartz et al.·Jan 9, 2024SaveLearn
GPU-accelerated Interval Arithmetic to solve the Apollonius Problem applied to a Stereo Drift ChamberWe propose a new system of equations which identifies the helix common to all drift distance hits produced by a full stereo drift chamber detector when a charged particle passes through this…Wilfrid da Silva, Patrice Lebrun, Jean-Claude Angélique et al.·Jan 9, 2024SaveLearn