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Particle Data Group

  • Neutrino Mixing

    Neutrino Mixing

  • 33. Passage of Particles Through Matter 1

    33. Passage of Particles Through Matter 1

  • Gauge and Higgs Bosons

    Gauge and Higgs Bosons

  • Rho(770), Ω(782), Φ(1020) Resonances, and an Addi- Tional Resonance Describing the Total Contribution of the Ρ(1450) and Ω(1420) States

    Rho(770), Ω(782), Φ(1020) Resonances, and an Addi- Tional Resonance Describing the Total Contribution of the Ρ(1450) and Ω(1420) States

  • Quark Masses 1 66

    Quark Masses 1 66

  • QCD, Jets, & Gluons

    QCD, Jets, & Gluons

  • Particle Interactions in Detectors Outline

    Particle Interactions in Detectors Outline

  • Particle Data Group

    Particle Data Group

  • Review Article STANDARD MODEL of PARTICLE PHYSICS—A

    Review Article STANDARD MODEL of PARTICLE PHYSICS—A

  • 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)

  • Neutrino Properties

    Neutrino Properties

  • Elementary Particle

    Elementary Particle

  • 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)

  • Neutrino Properties

    Neutrino Properties

  • 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)

  • Higgs Bosons — H0 and H± a REVIEW GOES HERE – Check Our WWW List of Reviews

    Higgs Bosons — H0 and H± a REVIEW GOES HERE – Check Our WWW List of Reviews

  • 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)

  • Passage of Particles Through Matter

    Passage of Particles Through Matter

Top View
  • Neutrino Mixing
  • 14. Neutrino Masses, Mixing, and Oscillations 1 14
  • Γ (Photon) I (J ) = 0,1(1 )
  • BARYONS (S =0,I =1/2)= 1/2) P, N+ = Uud; N, N0 = Udd
  • Other Particle Searches OMITTED from SUMMARY TABLE OTHER PARTICLE SEARCHES Revised February 2018 by K
  • 33. Passage of Particles Through Matter 1
  • BARYONS (S = 0, I = 1/2) P, N+ = Uud; N, N0 = Udd
  • 34. Passage of Particles Through Matter
  • BOTTOM MESONS (B = ±1) B+ = Ub, B0 = Db, B0 = D B, B− = U B, Similarly for B∗’S
  • See the Related Review(S): Top Quark
  • Bachelor's Thesis in Theoretical Physics on the Possibility of Massive
  • Fundamentals of Interactions of Particles in Matter
  • Neutrino Properties
  • Rpp2020-List-Higgs-Boson.Pdf
  • 34. Passage of Particles Through Matter 1
  • See the Related Review(S): Mass and Width of the W Boson
  • 10. Electroweak Model and Constraints on New Physics 1 10
  • Particle Data Group 57 Yearsnovember of Service 2014


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