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D meson

  • Spectator Model in D Meson Decays

    Spectator Model in D Meson Decays

  • HADRONIC DECAYS of the Ds MESON and a MODEL-INDEPENDENT DETERMINATION of the BRANCHING FRACTION

    HADRONIC DECAYS of the Ds MESON and a MODEL-INDEPENDENT DETERMINATION of the BRANCHING FRACTION

  • Effective Field Theory for Doubly Heavy Baryons and Lattice

    Effective Field Theory for Doubly Heavy Baryons and Lattice

  • Charm Meson Decays 3 for Charm Production Is Relatively High, Σ(D0D¯ 0) = 3.66 0.03 0.06 Nb and Σ(D+D−) = 2.91 0.03 0.05 Nb (6)

    Charm Meson Decays 3 for Charm Production Is Relatively High, Σ(D0D¯ 0) = 3.66 0.03 0.06 Nb and Σ(D+D−) = 2.91 0.03 0.05 Nb (6)

  • B Meson Decays Marina Artuso1, Elisabetta Barberio2 and Sheldon Stone*1

    B Meson Decays Marina Artuso1, Elisabetta Barberio2 and Sheldon Stone*1

  • Masses of Scalar and Axial-Vector B Mesons Revisited

    Masses of Scalar and Axial-Vector B Mesons Revisited

  • D-Meson Production in P-Pb Collisions at √ Snn = 5.02 Tev and in Pp

    D-Meson Production in P-Pb Collisions at √ Snn = 5.02 Tev and in Pp

  • Monte Carlo Simulations of D-Mesons with Extended Targets in the PANDA Detector

    Monte Carlo Simulations of D-Mesons with Extended Targets in the PANDA Detector

  • Medium Modifications of Mesons

    Medium Modifications of Mesons

  • Transverse Momentum Dependence of D-Meson Production in Pb-Pb

    Transverse Momentum Dependence of D-Meson Production in Pb-Pb

  • ELEMENTARY PARTICLES in PHYSICS 1 Elementary Particles in Physics S

    ELEMENTARY PARTICLES in PHYSICS 1 Elementary Particles in Physics S

  • Azimuthal Correlations of Prompt D Mesons with Charged Particles in Pp and P–Pb Collisions at √Snn=5.02Tev

    Azimuthal Correlations of Prompt D Mesons with Charged Particles in Pp and P–Pb Collisions at √Snn=5.02Tev

  • D MESON PRODUCTION in E+E ANNIHILATION* Petros-Afentoulis Rapidis Stanford Linear Accelerator Center Stanford University Stanfor

    D MESON PRODUCTION in E+E ANNIHILATION* Petros-Afentoulis Rapidis Stanford Linear Accelerator Center Stanford University Stanfor

  • Hep-Ph/9503414

    Hep-Ph/9503414

  • Measurement of B Quark Fragmentation Fractions in the Production of Strange and Light B Mesons in Pp̅ Collisions at √S =1.8 Tev

    Measurement of B Quark Fragmentation Fractions in the Production of Strange and Light B Mesons in Pp̅ Collisions at √S =1.8 Tev

  • Arxiv:2011.06078V2 [Nucl-Ex] 13 May 2021 Erdcino Hsatceo at Fi Salwda Spec As Allowed Is It of Parts Or Collaboration

    Arxiv:2011.06078V2 [Nucl-Ex] 13 May 2021 Erdcino Hsatceo at Fi Salwda Spec As Allowed Is It of Parts Or Collaboration

  • Exotics: Heavy Pentaquarks and Tetraquarks Arxiv:1706.00610V2

    Exotics: Heavy Pentaquarks and Tetraquarks Arxiv:1706.00610V2

  • Quantum Field Theory Approaches to Meson Structure

    Quantum Field Theory Approaches to Meson Structure

Top View
  • D Meson Reconstruction at Star Using the Silicon Vertex Tracker (Svt) Sarah Lapointe Wayne State University
  • Rare B Meson Decays with Omega Mesons
  • Nuclear Modification Factor of D0 Mesons in Pbpb Collisions At
  • Measurement of the Charged and Neutral D Meson Lifetimes*
  • D-Meson Nuclear Modification Factor and Elliptic Flow Measurements in Pb–Pb Collisions at √Snn=5.02 Tev with ALICE at the LH
  • 71. Leptonic Decays of Charged Pseudoscalar Mesons
  • Meson–Nucleus Potentials and the Search for Meson-Nucleus Bound States
  • Measurement of the D-Meson Nuclear Modification Factor and Elliptic Flow in Pb–Pb Collisions at √SNN = 5.02 Tev with ALICE A
  • Measurement of the B< Lifetime
  • Calculation of the Masses of All Fundamental Elementary Particles with an Accuracy of Approx
  • Chapter 2 B Meson Physics
  • Flavor Symmetry and Quark Model of Hadrons
  • B- and D-Meson Leptonic Decay Constants from Four-Flavor Lattice QCD
  • D Meson Mass and Heavy Quark Potential at Finite Temperature
  • Measurement of D-Meson Nuclear Modification Factor and Flow in Pb-Pb Collisions with ALICE at the LHC
  • In-Medium Excitations
  • Observation and Study of the Baryonic B-Meson Decays B→D(∗)P(P(Π) Π)
  • A Challenge to Lepton Universality in B Meson Decays


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