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Hadrons and nuclei
Published 2021“…Here, we discuss opportunities for lattice QCD calculations related to the structure and spectroscopy of hadrons and nuclei. An overview of recent lattice calculations of the structure of the proton and other hadrons is presented along with prospects for future extensions. …”
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FCC-hh: The Hadron Collider
Published 2021“…Combining ingredients from the Large Hadron Collider (LHC), the high-luminosity LHC upgrade and adding novel technologies and approaches, the FCC-hh design aims at significantly extending the energy frontier to 100 TeV. …”
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Jet substructure at the Large Hadron Collider
Published 2021“…Jet substructure has emerged to play a central role at the Large Hadron Collider, where it has provided numerous innovative ways to search for new physics and to probe the standard model, particularly in extreme regions of phase space. …”
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Observation of New Charmless Decays of Bottom Hadrons
Published 2010“…We search for new charmless decays of neutral b hadrons to pairs of charged hadrons, using 1 fb[superscript -1] of data collected by the CDF II detector at the Fermilab Tevatron. …”
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Deciphering the MSSM Higgs mass at future hadron colliders
Published 2017“…Future hadron colliders will have a remarkable capacity to discover massive new particles, but their capabilities for precision measurements of couplings that can reveal underlying mechanisms have received less study. …”
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Radial scaling in inclusive jet production at hadron colliders
Published 2018“…Here we demonstrate that inclusive jet production at the Large Hadron Collider (LHC) in high-energy p-p collisions and at the Tevatron in p[over ¯]-p inelastic scattering shows similar behavior. …”
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Elliptic Flow of Charm and Strange Hadrons in High-Multiplicity
Published 2018“…The elliptic azimuthal anisotropy coefficient (v[subscript 2]) is measured for charm (D[superscript 0]) and strange (K[superscript 0][subscript S], Λ, Ξ[superscript -], and Ω[superscript -]) hadrons, using a data sample of p+Pb collisions collected by the CMS experiment, at a nucleon-nucleon center-of-mass energy of √s[subscript NN] =8.16 TeV. …”
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HE-LHC: The High-Energy Large Hadron Collider
Published 2021“…Combining ingredients from the Large Hadron Collider (LHC), the high-luminosity LHC upgrade and adding novel technologies and approaches, the FCC-hh design aims at significantly extending the energy frontier to 100 TeV. …”
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Λ+ c polarimetry using the dominant hadronic mode
Published 2023“…The obtained representation can facilitate polarisation measurements of the Λ c + $$ {\Lambda}_c^{+} $$ baryon and eases inclusion of the Λ c + $$ {\Lambda}_c^{+} $$ → pK−π+ decay mode in hadronic amplitude analyses.…”
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Measurement of the azimuthal ordering of charged hadrons with the ATLAS detector
Published 2013“…This paper presents a study of the possible ordering of charged hadrons in the azimuthal angle relative to the beam axis in high-energy proton-proton collisions at the Large Hadron Collider (LHC). …”
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Reconstruction of hadronic decay products of tau leptons with the ATLAS experiment
Published 2018“…This paper presents a new method of reconstructing the individual charged and neutral hadrons in tau decays with the ATLAS detector. The reconstructed hadrons are used to classify the decay mode and to calculate the visible four-momentum of reconstructed tau candidates, significantly improving the resolution with respect to the calibration in the existing tau reconstruction. …”
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Study of B+c decays to charmonia and three light hadrons
Published 2022“…Abstract Using proton-proton collision data, corresponding to an integrated luminosity of 9 fb−1 collected with the LHCb detector, seven decay modes of the B c + $$ {\mathrm{B}}_{\mathrm{c}}^{+} $$ meson into a J/ψ or ψ(2S) meson and three charged hadrons, kaons or pions, are studied. The decays B c + $$ {\mathrm{B}}_{\mathrm{c}}^{+} $$ → (ψ(2S) → J/ψπ+π−)π+, B c + $$ {\mathrm{B}}_{\mathrm{c}}^{+} $$ → ψ(2S)π+π−π+, B c + $$ {\mathrm{B}}_{\mathrm{c}}^{+} $$ → J/ψK+π−π+ and B c + $$ {\mathrm{B}}_{\mathrm{c}}^{+} $$ → J/ψK+K−K+ are observed for the first time, and evidence for the B c + $$ {\mathrm{B}}_{\mathrm{c}}^{+} $$ → ψ(2S)K+K−π+, decay is found, where J/ψ and ψ(2S) mesons are reconstructed in their dimuon decay modes. …”
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Strange hadron collectivity in pPb and PbPb collisions
Published 2023“…Comparisons of the pPb and PbPb results for both strange hadrons and charged particles illustrate how event-by-event flow fluctuations depend on the system size.…”
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Measurement of the top quark mass in the all-hadronic mode at CDF
Published 2014“…A measurement of the top quark mass (Mtop) in the all-hadronic decay channel is presented. It uses 5.8 fb[superscript −1] of pp¯ data collected with the CDF II detector at the Fermilab Tevatron Collider. …”
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Identification techniques for highly boosted W bosons that decay into hadrons
Published 2015“…Algorithms are defined to identify such W jets for different signals of interest, using techniques that are also applicable to other decays of bosons to hadrons that result in a single jet, such as those from highly boosted Z and Higgs bosons. …”
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No radial excitations in low energy QCD. II. The shrinking radius of hadrons
Published 2016“…Inescapably, they lead to three laws governing the size of hadrons, including in particular protons and neutrons that make up the bulk of ordinary matter: (a) there are no radial excitations in low-energy QCD; (b) the size of a hadron is largest in its ground state; (c) the hadron’s size shrinks when its orbital excitation increases. …”
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Measurement of b hadron lifetimes in pp collisions at √s = 8 TeV
Published 2018“…Measurements are presented of the lifetimes of the B[superscript 0], B[superscript 0][subscript s], Λ[superscript 0][subscript b], and B[superscript +][superscript c] hadrons using the decay channels B[superscript 0]→J/ψK[superscript ∗](892)[superscript 0], B[superscript 0]→J/ψK[superscript 0][subscript S], B[superscript 0][subscript s]→J/ψπ[superscript +]π[superscript −], B[superscript 0][subscript s]→J/ψϕ(1020), Λ[superscript 0][subscript b]→J/ψΛ[superscript 0], and B[superscript +][subscript c]→J/ψπ[superscript +]. …”
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