Demonstration of Event Position Reconstruction based on Diffusion in the NEXT-White DetectorNoble element time projection chambers are a leading technology for rare event detection in physics, such as for dark matter and neutrinoless double beta decay searches. Time projection chambers…J. Haefner, K. E. Navarro, R. Guenette et al.·Nov 6, 2023SaveLearn
Experimentation at a muon colliderExperimental activities involving multi-TeV muon collisions are a relatively recent endeavor. The community has limited experience in designing detectors for lepton interactions at center-of-mass…Massimo Casarsa, Donatella Lucchesi, Lorenzo Sestini·Nov 6, 2023SaveLearn
Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at s = 13 TeVA search is presented for new Higgs bosons in proton-proton (pp) collision events in which a same-sign top quark pair is produced in association with a jet, via the pp tH/A …CMS Collaboration·Nov 6, 2023SaveLearn
The k4Clue package: Empowering Future Collider Experiments with the CLUE AlgorithmHigh granularity calorimeters have become increasingly crucial in modern particle physics experiments, and their importance is set to grow even further in the future. The CLUstering of Energy (CLUE)…Erica Brondolin, Marco Rovere, Felice Pantaleo·Nov 6, 2023SaveLearn
Constraining (anti)nuclei measurements relevant for astrophysics with ALICEAntinuclei can be produced in space either by collisions of high-energy cosmic rays with the interstellar medium or from the annihilation of dark matter particles stemming into standard model…Chiara Pinto·Nov 6, 2023SaveLearn
Search for high-mass exclusive diphoton production with tagged protons in proton-proton collisions at s = 13 TeVA search is presented for high-mass exclusive diphoton production via photon-photon fusion in proton-proton collisions at s = 13 TeV in events where both protons survive the interaction. The…CMS, TOTEM Collaborations·Nov 5, 2023SaveLearn
Measurement of the absolute branching fraction of the three-body decay c+ 0K+π0 and search for c+ nK+π0, 0K+π0 and K+π0The Cabbibo-favored decay c+ 0K+π0 is studied for the first time using 6.1 fb-1 of e+e- collision data at center-of-mass energies between 4.600 and 4.840 GeV,…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Nov 4, 2023SaveLearn
Triggerless data acquisition pipeline for Machine Learning based statistical anomaly detectionThis work describes an online processing pipeline designed to identify anomalies in a continuous stream of data collected without external triggers from a particle detector. The processing pipeline…Gaia Grosso, Nicolò Lai, Matteo Migliorini et al.·Nov 3, 2023SaveLearn
Quantum Sensors for High Energy PhysicsStrong motivation for investing in quantum sensing arises from the need to investigate phenomena that are very weakly coupled to the matter and fields well described by the Standard Model. These can…Aaron Chou, Kent Irwin, Reina H. Maruyama et al.·Nov 3, 2023SaveLearn
Measurement of the K+π+γγ decayA sample of 3984 candidates of the K+π+γγ decay, with an estimated background of 29114 events, was collected by the NA62 experiment at CERN during 2017-2018. In order to…The NA62 Collaboration·Nov 3, 2023SaveLearn
Fraction of c decays in prompt J/ production measured in pPb collisions at sNN=8.16 TeVThe fraction of c1 and c2 decays in the prompt J/ yield, F c=σ_c J//σJ/, is measured by the LHCb detector in pPb collisions at…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Nov 2, 2023SaveLearn
Search for Periodic Time Variations of the Solar 8B Neutrino Flux between 1996 and 2018 in Super-KamiokandeWe report a search for time variations of the solar 8B neutrino flux using 5804 live days of Super-Kamiokande data collected between May 31, 1996, and May 30, 2018. Super-Kamiokande measured the…K. Abe, C. Bronner, Y. Hayato et al.·Nov 2, 2023SaveLearn
Search for a muonphilic scalar X0 or vector X1 via J/μ+μ-+invisible decays at BESIIA light scalar X0 or vector X1 particles have been introduced as a possible explanation for the (g-2)μ anomaly and dark matter phenomena. Using (8.998 0.039)×109 …BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Nov 2, 2023SaveLearn
Measuring the Electric and Magnetic Form Factors of Protons and Antiprotons at small Q2 and the charge radii of hadronsCharge radii of hadrons are back in the focus since precision spectroscopic measurements in muonic hydrogen revealed a proton charge radius considerably smaller than generally accepted ever since…Stephan Paul·Nov 1, 2023SaveLearn
Measurement of the Ratio of Partial Branching Fractions of Inclusive B Xu to B Xc and the Ratio of their Spectra with Hadronic TaggingWe present a measurement of the ratio of partial branching fractions of the semi-leptonic inclusive decays, B Xu to $B Xc …Belle Collaboration, M. Hohmann, P. Urquijo et al.·Nov 1, 2023SaveLearn
Progress in the partial-wave analysis methods at COMPASSWe study the excitation spectrum of light and strange mesons in diffractive scattering. We identify different hadron resonances through partial wave analysis, which inherently relies on analysis…Julien Beckers, Florian Kaspar, Jakob Knollmüller·Nov 1, 2023SaveLearn
New results on |Vub| using inclusive and exclusive B decays from the Belle experimentWe present two recent measurements of semileptonic B decays at Belle, offering valuable insights into the determination of the Cabibbo-Kobayashi-Maskawa (CKM) matrix element |Vub|. These…Lu Cao·Nov 1, 2023SaveLearn
Measurements of |Vcb| and |Vub| from Belle and Belle IIThis proceeding summarizes recent measurements of the Cabibbo-Kobayashi-Maskawa (CKM) matrix elements |Vcb| and |Vub| at the Belle and Belle~II experiments. It provides insights derived…Lu Cao·Nov 1, 2023SaveLearn
Search for an exotic decay of the Higgs boson into a Z boson and a pseudoscalar particle in proton-proton collisions at s = 13 TeVA search for an exotic decay of the Higgs boson to a Z boson and a light pseudoscalar particle (a), decaying to a pair of leptons and a pair of photons, respectively, is presented. The search is…CMS Collaboration·Oct 31, 2023SaveLearn
Reconstructing long-lived particles with the ILD detectorFuture e+e- colliders, thanks to their clean environment and triggerless operation, offer a unique opportunity to search for long-lived particles (LLPs). Considered in this contribution are…Jan Klamka·Oct 31, 2023SaveLearn
Exotic Meson candidates in COMPASS dataOne of the prime goals of the COMPASS experiment at CERN is the study of the light meson spectrum, with a particular emphasis on the search for exotic states. The focus of this paper is on signals of…David Spülbeck·Oct 31, 2023SaveLearn
First observation and study of the K → π0 π0 μ decayThe NA48/2 experiment at CERN reports the first observation of the K → π0 π0 μ decay based on a sample of 2437 candidates with 15% background contamination…2 Collaboration, J. R. Batley, G. Kalmus et al.·Oct 31, 2023SaveLearn
Measurement of Angular Coefficients of B D* : Implications for |Vcb| and Tests of Lepton Flavor UniversalityWe measure the complete set of angular coefficients Ji for exclusive B D* decays ( = e, μ). Our analysis uses the full 711\,fb-1 Belle data…Belle Collaboration, M. T. Prim, F. Bernlochner et al.·Oct 31, 2023SaveLearn
Search for the Sagittarius tidal stream of axion dark matter around 4.55 μeVWe report the first search for the Sagittarius tidal stream of axion dark matter around 4.55 μeV using CAPP-12TB haloscope data acquired in March of 2022. Our result excluded the Sagittarius…B. R. Ko·Oct 31, 2023SaveLearn
Search for W' bosons decaying to a top and a bottom quark in leptonic final states in proton-proton collisions at s = 13 TeVA search for W' bosons decaying to a top and a bottom quark in final states including an electron or a muon is performed with the CMS detector at the LHC. The analyzed data correspond to an…CMS Collaboration·Oct 30, 2023SaveLearn