Measurement of the Z boson production cross-section in pp collisions at s = 5.02 TeVThe first measurement of the Z boson production cross-section at centre-of-mass energy s = 5.02\,TeV in the forward region is reported, using pp collision data collected by the LHCb…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Aug 24, 2023SaveLearn
Jet energy calibration with deep learning as a Kubeflow pipelinePrecise measurements of the energy of jets emerging from particle collisions at the LHC are essential for a vast majority of physics searches at the CMS experiment. In this study, we leverage…Daniel Holmberg, Dejan Golubovic, Henning Kirschenmann·Aug 24, 2023SaveLearn
Differential cross-section measurements of the production of four charged leptons in association with two jets using the ATLAS detectorDifferential cross-sections are measured for the production of four charged leptons in association with two jets. These measurements are sensitive to final states in which the jets are produced via…ATLAS Collaboration·Aug 23, 2023SaveLearn
Experimental and Phenomenological Investigations of the MiniBooNE AnomalyThis thesis covers a range of experimental and theoretical efforts to elucidate the origin of the 4.8σ MiniBooNE low energy excess (LEE). We begin with the follow-up MicroBooNE experiment,…Nicholas Kamp·Aug 23, 2023SaveLearn
Searching for Charged Lepton Flavour Violation with Mu3eThe observation of lepton flavour violation (LFV) in the charged lepton sector would be an unambiguous sign of physics beyond the Standard Model (BSM), and thus, it is the channel of choice for many…Ann-Kathrin Perrevoort·Aug 22, 2023SaveLearn
Further investigation of dilepton-based center-of-mass energy measurements at e+e- collidersMethods for measuring the absolute center-of-mass energy using dileptons from e+e- collision events are further developed with an emphasis on accelerator, detector, and physics limitations.…Graham W. Wilson·Aug 21, 2023SaveLearn
Hadronization mechanisms (via heavy-flavour hadrons): ExperimentThe formation of hadrons is a fundamental process in nature that can be investigated at particle colliders. Given their large mass, heavy quarks (charm and beauty) are produced only in initial…Andrea Rossi·Aug 20, 2023SaveLearn
An Integrated Simulation Tool for Dark Current Radiation Effects Using ACE3P and Geant4A simulation workflow is under development to interface particle data transfer and matching of geometry between the electromagnetic (EM) cavity simulation code ACE3P and radiation code Geant4. The…Lixin Ge, Zenghai Li, Cho-Kuen Ng et al.·Aug 18, 2023SaveLearn
Using the GP2X framework for center-of-mass energy precision studies at e+e- Higgs factoriesTwo channels for measuring the absolute center-of-mass energy, s, and collision beam energies, E- and E+, are investigated for future e+e- Higgs factories. These two channels of…Brendon Madison·Aug 18, 2023SaveLearn
Measurement of the tt cross section and its ratio to the Z production cross section using pp collisions at s = 13.6 TeV with the ATLAS detectorThe inclusive top-quark-pair production cross section σtt and its ratio to the Z-boson production cross section have been measured in proton--proton collisions at s = 13.6…ATLAS Collaboration·Aug 18, 2023SaveLearn
Software Performance of the ATLAS Track Reconstruction for LHC Run 3Charged particle reconstruction in the presence of many simultaneous proton-proton (pp) collisions in the LHC is a challenging task for the ATLAS experiment's reconstruction software due to the…ATLAS Collaboration·Aug 18, 2023SaveLearn
Compatibility and combination of world W-boson mass measurementsThe compatibility of W-boson mass measurements performed by the ATLAS, LHCb, CDF, and D0 experiments is studied using a coherent framework with theory uncertainty correlations. The measurements are…Simone Amoroso, Nansi Andari, William Barter et al.·Aug 18, 2023SaveLearn
Design and performance of the ENUBET monitored neutrino beamThe ENUBET project is aimed at designing and experimentally demonstrating the concept of monitored neutrino beams. These novel beams are enhanced by an instrumented decay tunnel, whose detectors…F. Acerbi, I. Angelis, L. Bomben et al.·Aug 18, 2023SaveLearn
Astroparticle Physics with the Forward Physics Facility at the High-Luminosity LHCHigh-energy collisions at the High-Luminosity Large Hadron Collider (HL-LHC) will produce an enormous flux of particles along the beam collision axis that is not accessible by existing LHC…Dennis Soldin·Aug 17, 2023SaveLearn
Extended Axion Dark Matter Search Using the CAPP18T HaloscopeWe report an extended search for the axion dark matter using the CAPP18T haloscope. The CAPP18T experiment adopts innovative technologies of a high-temperature superconducting magnet and a Josephson…Byeongsu Yang, Hojin Yoon, Moohyun Ahn et al.·Aug 17, 2023SaveLearn
SR-GAN for SR-gamma: super resolution of photon calorimeter images at collider experimentsWe study single-image super-resolution algorithms for photons at collider experiments based on generative adversarial networks. We treat the energy depositions of simulated electromagnetic showers of…Johannes Erdmann, Aaron van der Graaf, Florian Mausolf et al.·Aug 17, 2023SaveLearn
Observation of charmed strange meson pair production in (2S) decays and in e+e- annihilation at s = 10.52~ GeVWe observe the process (2S) Ds(*)+ DsJ- and continuum production e+e- Ds(*)+ DsJ- at s = 10.52 GeV (and their charge conjugates) using the data…Belle Collaboration, B. S. Gao, W. J. Zhu et al.·Aug 17, 2023SaveLearn
Search for vector-boson resonances decaying into a top quark and a bottom quark using pp collisions at s = 13 TeV with the ATLAS detectorA search for a new massive charged gauge boson, W', is performed with the ATLAS detector at the LHC. The dataset used in this analysis was collected from proton-proton collisions at a…ATLAS Collaboration·Aug 16, 2023SaveLearn
Observation of Cabibbo-Suppressed Two-Body Hadronic Decays and Precision Mass Measurement of the c0 BaryonThe first observation of the singly Cabibbo-suppressed c0-K+ and c0-π+ decays is reported, using proton-proton collision data at a…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Aug 16, 2023SaveLearn
First results of the SUPAX Experiment: Probing Dark PhotonsWe show the first results of a new cavity based haloscope searching for dark photons with masses around 34~μeV. Dark photons are hypothetical vector particles and a compelling dark matter…Tim Schneemann, Kristof Schmieden, Matthias Schott·Aug 16, 2023SaveLearn
Study of e+e-ηφ at center-of-mass energies from 3.773 to 4.600 GeVWe present a study of the process e+e-ηφ using data samples collected with the BESIII detector corresponding to an integrated luminosity of 15.03 fb-1 at 23 center-of-mass…M. Ablikim, M. N. Achasov, P. Adlarson et al.·Aug 16, 2023SaveLearn
Dark sector and Axion-like particle search at BESIIIDark matter (DM) refers to a new type of matter that may explain observed rotation curves of galaxies and the composite structure of the Universe. It may couple to the Standard Model particles via…Vindhyawasini Prasad·Aug 16, 2023SaveLearn
Search for a third-generation leptoquark coupled to a τ lepton and a b quark through single, pair, and nonresonant production in proton-proton collisions at s = 13 TeVA search is presented for a third-generation leptoquark (LQ) coupled exclusively to a τ lepton and a b quark. The search is based on proton-proton collision data at a center-of-mass energy of 13…CMS Collaboration·Aug 15, 2023SaveLearn
Measurement of the Higgs boson mass with H → γγ decays in 140 fb-1 of s=13 TeV pp collisions with the ATLAS detectorThe mass of the Higgs boson is measured in the Hγγ decay channel, exploiting the high resolution of the invariant mass of photon pairs reconstructed from the decays of Higgs bosons…ATLAS Collaboration·Aug 14, 2023SaveLearn
Projections of Discovery Potentials from Expected BackgroundBackground channels with their expected strength and uncertainty levels are usually known in searches of novel phenomena prior to the experiments are conducted at their design stage. We…M. K. Singh, H. B. Li, H. T. Wong et al.·Aug 14, 2023SaveLearn