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  2. Baryon number - Wikipedia

    en.wikipedia.org/wiki/Baryon_number

    Three antiquarks of different anticolors, giving an antibaryon with baryon number −1. The baryon number was defined long before the quark model was established, so rather than changing the definitions, particle physicists simply gave quarks one third the baryon number. Nowadays it might be more accurate to speak of the conservation of quark ...

  3. List of baryons - Wikipedia

    en.wikipedia.org/wiki/List_of_baryons

    These lists detail all known and predicted baryons in total angular momentum J = ⁠ 1 / 2 ⁠ and J = ⁠ 3 / 2 ⁠ configurations with positive parity. [5]Baryons composed of one type of quark (uuu, ddd, ...) can exist in J = ⁠ 3 / 2 ⁠ configuration, but J = ⁠ 1 / 2 ⁠ is forbidden by the Pauli exclusion principle.

  4. Baryon asymmetry - Wikipedia

    en.wikipedia.org/wiki/Baryon_asymmetry

    Baryon number violation is a necessary condition to produce an excess of baryons over anti-baryons. But C-symmetry violation is also needed so that the interactions which produce more baryons than anti-baryons will not be counterbalanced by interactions which produce more anti-baryons than baryons.

  5. Baryogenesis - Wikipedia

    en.wikipedia.org/wiki/Baryogenesis

    Baryon number violation is a necessary condition to produce an excess of baryons over anti-baryons. But C-symmetry violation is also needed so that the interactions which produce more baryons than anti-baryons will not be counterbalanced by interactions which produce more anti-baryons than baryons.

  6. Mathematical formulation of the Standard Model - Wikipedia

    en.wikipedia.org/wiki/Mathematical_formulation...

    By Noether's theorem, each symmetry above has an associated conservation law: the conservation of baryon number, [12] electron number, muon number, and tau number. Each quark is assigned a baryon number of , while each antiquark is assigned a baryon number of . Conservation of baryon number implies that the number of quarks minus the number of ...

  7. B − L - Wikipedia

    en.wikipedia.org/wiki/B_%E2%88%92_L

    This quantum number is the charge of a global/gauge U(1) symmetry in some Grand Unified Theory models, called U(1) B−L.Unlike baryon number alone or lepton number alone, this hypothetical symmetry would not be broken by chiral anomalies or gravitational anomalies, as long as this symmetry is global, which is why this symmetry is often invoked.

  8. Proton decay - Wikipedia

    en.wikipedia.org/wiki/Proton_decay

    Some beyond-the-Standard-Model grand unified theories (GUTs) explicitly break the baryon number symmetry, allowing protons to decay via the Higgs particle, magnetic monopoles, or new X bosons with a half-life of 10 31 to 10 36 years. For comparison, the universe is roughly 1.38 × 10 10 years old. [3]

  9. Glossary of string theory - Wikipedia

    en.wikipedia.org/wiki/Glossary_of_string_theory

    3. Lambda baryon, a baryon with 2 light quarks and isospin 0 μ 1. Renormalization scale, with the dimensions of mass 2. Muon ν Neutrino Ξ 1. Xi baryon, a baryon with 1 light quark π 1. 3.14159... 2. Pion Π The momentum density conjugate to X ρ Rho meson, a light meson with PC = –– σ 1. Spacelike coordinate on the world-sheet 2.