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Lepton

  • The Five Common Particles

    The Five Common Particles

  • Decays of the Tau Lepton*

    Decays of the Tau Lepton*

  • Lepton Flavor and Number Conservation, and Physics Beyond the Standard Model

    Lepton Flavor and Number Conservation, and Physics Beyond the Standard Model

  • Neutrino Opacity I. Neutrino-Lepton Scattering*

    Neutrino Opacity I. Neutrino-Lepton Scattering*

  • Review of Lepton Universality Tests in B Decays

    Review of Lepton Universality Tests in B Decays

  • 1 Drawing Feynman Diagrams

    1 Drawing Feynman Diagrams

  • Phenomenology of Gev-Scale Heavy Neutral Leptons Arxiv:1805.08567

    Phenomenology of Gev-Scale Heavy Neutral Leptons Arxiv:1805.08567

  • Production of the Doubly Charged Higgs Boson in Association with the SM Gauge Bosons And/Or Other HTM Scalars at Hadron Colliders

    Production of the Doubly Charged Higgs Boson in Association with the SM Gauge Bosons And/Or Other HTM Scalars at Hadron Colliders

  • Lepton/Photon Highlights

    Lepton/Photon Highlights

  • Lepton Mixing and Neutrino Mass

    Lepton Mixing and Neutrino Mass

  • Search for Rare Multi-Pion Decays of the Tau Lepton Using the Babar Detector

    Search for Rare Multi-Pion Decays of the Tau Lepton Using the Babar Detector

  • Neutrino Masses-How to Add Them to the Standard Model

    Neutrino Masses-How to Add Them to the Standard Model

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

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

  • Z, W+, W-, Gluon, Photon Happy Families Snap Name: Down

    Z, W+, W-, Gluon, Photon Happy Families Snap Name: Down

  • ELEMENTARY PARTICLES in PHYSICS 1 Elementary Particles in Physics S

    ELEMENTARY PARTICLES in PHYSICS 1 Elementary Particles in Physics S

  • Field Theory and the Standard Model

    Field Theory and the Standard Model

  • Measurement Definitions Based on Truth Particles Tancredi Carli Fabio Cossuti

    Measurement Definitions Based on Truth Particles Tancredi Carli Fabio Cossuti

  • LIGHT UNFLAVORED MESONS (S = C = B = 0) for I =1(Π, B, Ρ, A): Ud, (Uu Dd)/√2, Du; − for I =0(Η, Η′, H, H′, Ω, Φ, F , F ′): C1(U U + D D) + C2(S S)

    LIGHT UNFLAVORED MESONS (S = C = B = 0) for I =1(Π, B, Ρ, A): Ud, (Uu Dd)/√2, Du; − for I =0(Η, Η′, H, H′, Ω, Φ, F , F ′): C1(U U + D D) + C2(S S)

Top View
  • Current Situation in the Neutrino (And Charged-Lepton) Sector
  • Lepton Dipole Moments
  • BOTTOM, STRANGE MESONS (B = ±1, S = ∓1) 0 0 ∗ Bs = Sb, Bs = S B, Similarly for Bs ’S
  • Model with Lepton-Flavour Non-Universality
  • The Periodic Table of Elementary Particles
  • 1 Theory of Pion Decays
  • PIENUXE: Testing Lepton Flavor Universality and CKM Unitarity with Rare Pion Decays
  • Magnetic Moment of Leptons
  • 113. Searches for Quark and Lepton Compositeness 1 113
  • Implementation of Τ-Lepton Decays Into the Event-Generator SHERPA
  • Lepton Pair Production Through Two Photon Process in Heavy Ion Collisions
  • Baryon and Lepton Numbers in Particle Physics Beyond the Standard Model
  • Chapter 5: Quarks and Hadrons
  • Pion-Quark Scattering Model for Lepton Pair Production*
  • Lepton Number Violating Processes and Majorana
  • Lepton-Flavour-Violating Gluonic Operators: Arxiv:1802.09822V2 [Hep
  • Mixed Beauty at Hamburg Logical Big Bang (Reviewed by M.S
  • Implications of Lepton Universality Violation in B-Meson Decays


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