Recent measurements of W and Z (+jets) at ATLAS and CMSVector boson measurements at the LHC are an ideal laboratory to study detailed properties of the QCD and electroweak sectors of the Standard Model. These proceedings review several recent…Oz Amram·Jun 2, 2023SaveLearn
Combination and summary of ATLAS dark matter searches interpreted in a 2HDM with a pseudo-scalar mediator using 139 fb-1 of s = 13 TeV pp collision dataResults from a wide range of searches targeting different experimental signatures with and without missing transverse momentum (ETmiss) are used to constrain a…ATLAS Collaboration·Jun 1, 2023SaveLearn
Precise measurement of the D+s lifetime at Belle IIWe measure the lifetime of the Ds+ meson using a data sample of 207 fb-1 collected by the Belle II experiment running at the SuperKEKB asymmetric-energy e+ e- collider. The lifetime is…Belle II Collaboration, I. Adachi, L. Aggarwal et al.·Jun 1, 2023SaveLearn
Search for Boosted Dark Matter in COSINE-100We search for energetic electron recoil signals induced by boosted dark matter (BDM) from the galactic center using the COSINE-100 array of NaI(Tl) crystal detectors at the Yangyang Underground…G. Adhikari, N. Carlin, J. J. Choi et al.·Jun 1, 2023SaveLearn
Indirect searches at CMSIn these proceedings, we present several new measurements of Standard Model (SM) processes, in the Higgs sector and beyond, that push the precision frontier forward at CMS. Results are presented in…Nicholas Smith·May 31, 2023SaveLearn
Investigation of Higgs Boson Decaying to Di-muon, Dark Matter Produced in Association with a Higgs Boson Decaying to b-quarks and Unbinned Profiled UnfoldingThe discovery of the Standard Model (SM) Higgs boson by ATLAS and CMS at the LHC in 2012 marked a major milestone in particle physics. However, many questions remain unanswered, which has led to an…Jay Chan·May 30, 2023SaveLearn
Measurement of the intrinsic hadronic contamination in the NA64-e high-purity e+/e- beam at CERNIn this study, we present the measurement of the intrinsic hadronic contamination at the CERN SPS H4 beamline configured to transport electrons and positrons at 100 GeV/c momentum. The analysis was…Yu. M. Andreev, D. Banerjee, B. Banto Oberhauser et al.·May 30, 2023SaveLearn
Measurement of the cross-sections of the electroweak and total production of a Z γ pair in association with two jets in pp collisions at s = 13 TeV with the ATLAS detectorThis Letter presents the measurement of the fiducial and differential cross-sections of the electroweak production of a Z γ pair in association with two jets. The analysis uses 140 fb-1…ATLAS Collaboration·May 30, 2023SaveLearn
Measurement of the τ-lepton mass with the Belle~II experimentWe present a measurement of the τ-lepton mass using a sample of about 175 million e+e- τ+τ- events collected with the Belle II detector at the SuperKEKB e+e- collider at a…Belle II Collaboration, I. Adachi, K. Adamczyk et al.·May 30, 2023SaveLearn
Evidence for B0 p0π- at BelleWe search for the B0 p0π- decay with 0 γ, where the γ is not measured, using a data sample corresponding to an integrated luminosity…Belle Collaboration, C. -Y. Chang, M. -Z. Wang et al.·May 30, 2023SaveLearn
Search for the lepton-flavor violating decay of the Higgs boson and additional Higgs bosons in the eμ final state in proton-proton collisions at s = 13 TeVA search for the lepton-flavor violating decay of the Higgs boson and potential additional Higgs bosons with a mass in the range 110-160 GeV to an eμ pair is presented. The search is…CMS Collaboration·May 29, 2023SaveLearn
Search for non-resonant production of semi-visible jets using Run 2 data in ATLASSemi-visible jets, with a significant contribution to the event's missing transverse momentum, can arise in strongly interacting dark sectors. This results in an event topology where one of the jets…ATLAS Collaboration·May 29, 2023SaveLearn
Search for the double-charmonium state with ηc J/ at BelleWe measure the cross section of e+e-→ηc J/ at the (nS) (n=1 -- 5) on-resonance and 10.52 GeV off-resonance energy points using the full data sample collected by the…Belle Collaboration, J. H. Yin, Y. B. Li et al.·May 29, 2023SaveLearn
Trigger efficiencies of a proposed beam monitoring detector (BeBe) for p+p collisions at NICA energiesThe Multipurpose Detector (MPD) consists of a typical array of sub-detectors to study the nuclear matter originating from the collisions of beams provided by the Nuclotron-based Ion Collider fAcility…Marco Alberto Ayala-Torres, Lucina Gabriela Espinoza Beltrán, Luis A. Hernández-Cruz et al.·May 29, 2023SaveLearn
Observation of WZγ Production in pp Collisions at s=13 TeV with the ATLAS DetectorThis Letter reports the observation of WZγ production and a measurement of its cross-section using 140.1 1.2 fb-1 of proton-proton collision data recorded at a center-of-mass energy…ATLAS Collaboration·May 26, 2023SaveLearn
Measurements of multijet event isotropies using optimal transport with the ATLAS detectorA measurement of novel event shapes quantifying the isotropy of collider events is performed in 140 fb-1 of proton-proton collisions with s=13 TeV centre-of-mass energy recorded with the…ATLAS Collaboration·May 26, 2023SaveLearn
Measurements of the azimuthal anisotropy of prompt and nonprompt charmonia in PbPb collisions at sNN = 5.02 TeVThe second-order (v2) and third-order (v3) Fourier coefficients describing the azimuthal anisotropy of prompt and nonprompt (from b-hadron decays) J/, as well as prompt (2S) mesons…CMS Collaboration·May 26, 2023SaveLearn
Measurements of the Cross-Section for the tt + Heavy-Flavor Production at the LHCAt the LHC, the process of a Higgs boson decaying into bottom or charm quarks produced in association with a pair of top quarks, ttbarH , allows for an empirical exploration of the heavy-flavor quark…Jorgen D'Hondt, Tae Jeong Kim·May 26, 2023SaveLearn
Study of Kinematics of the Jets in VBS Process at the Large Hadron ColliderThe comparison of the kinematic properties of different Vector Boson Scattering (VBS) and Vector Boson Fusion (VBF) processes using multivariate discriminator is presented. The search is performed to…Kadri Ozdemir·May 26, 2023SaveLearn
First measurement of η production in neutrino interactions on argon with MicroBooNEWe present a measurement of η production from neutrino interactions on argon with the MicroBooNE detector. The modeling of resonant neutrino interactions on argon is a critical aspect of the…MicroBooNE collaboration, P. Abratenko, O. Alterkait et al.·May 25, 2023SaveLearn
Search for leptoquarks decaying into the bτ final state in pp collisions at s=13 TeV with the ATLAS detectorA search for leptoquarks decaying into the bτ final state is performed using Run 2 proton-proton collision data from the Large Hadron Collider, corresponding to an integrated luminosity of 139…The ATLAS Collaboration·May 25, 2023SaveLearn
Amplitude analysis and branching fraction measurement of the decay D+ KS0π+π0π0Using 2.93 fb-1 of e+e- collision data collected with the BESIII detector at the center-of-mass energy 3.773\,GeV, we perform the first amplitude analysis of the decay $D+…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·May 25, 2023SaveLearn
Associated production of prompt J/ and mesons in pp collisions at s=13\,TeVThe associated production of prompt J/ and mesons in pp collisions at a centre-of-mass energy of s=13\,TeV is studied using LHCb data,…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·May 24, 2023SaveLearn
Weak decays of heavy-quark baryonsWeak decays of heavy-quark baryons offer an attractive laboratory to search for effects beyond the Standard Model (SM), complementary to searches in meson decays. However, the properties of these…Janina Nicolini·May 24, 2023SaveLearn
Measurement of the mass difference and relative production rate of the -b and -b baryonsThe mass difference between the -b and -b baryons is measured using proton-proton collision data collected by the LHCb experiment, corresponding to an integrated luminosity of $9 \,…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·May 24, 2023SaveLearn