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  2. Quark model - Wikipedia

    en.wikipedia.org/wiki/Quark_model

    In particle physics, the quark model is a classification scheme for hadrons in terms of their valence quarks—the quarks and antiquarks that give rise to the quantum numbers of the hadrons. The quark model underlies "flavor SU(3)" , or the Eightfold Way , the successful classification scheme organizing the large number of lighter hadrons that ...

  3. Eightfold way (physics) - Wikipedia

    en.wikipedia.org/wiki/Eightfold_way_(physics)

    In physics, the eightfold way is an organizational scheme for a class of subatomic particles known as hadrons that led to the development of the quark model. Both the American physicist Murray Gell-Mann and the Israeli physicist Yuval Ne'eman independently and simultaneously proposed the idea in 1961.

  4. Hyperon - Wikipedia

    en.wikipedia.org/wiki/Hyperon

    A combination of three u, d or s-quarks with a total spin of 3/2 form the so-called baryon decuplet. The lower six are hyperons. Being baryons, all hyperons are fermions. That is, they have half-integer spin and obey Fermi–Dirac statistics. Hyperons all interact via the strong nuclear force, making them types of hadron.

  5. List of particles - Wikipedia

    en.wikipedia.org/wiki/List_of_particles

    Quark models, first proposed in 1964 independently by Murray Gell-Mann and George Zweig (who called quarks "aces"), describe the known hadrons as composed of valence quarks and/or antiquarks, tightly bound by the color force, which is mediated by gluons. (The interaction between quarks and gluons is described by the theory of quantum ...

  6. 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.

  7. Hypercharge - Wikipedia

    en.wikipedia.org/wiki/Hypercharge

    For a strange quark, with electric charge ⁠− + 1 / 3 ⁠, a baryon number of ⁠+ + 1 / 3 ⁠, and strangeness −1, we get a hypercharge Y = ⁠− + 2 / 3 ⁠, so we deduce that I 3 = 0 . That means that a strange quark makes an isospin singlet of its own (the same happens with charm, bottom and top quarks), while up and down constitute ...

  8. Murray Gell-Mann - Wikipedia

    en.wikipedia.org/wiki/Murray_Gell-Mann

    In the 1960s, he introduced current algebra as a method of systematically exploiting symmetries to extract predictions from quark models, in the absence of reliable dynamical theory. This method led to model-independent sum rules confirmed by experiment, and provided starting points underpinning the development of the Standard Model (SM), the ...

  9. Quark - Wikipedia

    en.wikipedia.org/wiki/Quark

    The discovery finally convinced the physics community of the quark model's validity. [35] In the following years a number of suggestions appeared for extending the quark model to six quarks. Of these, the 1975 paper by Haim Harari [41] was the first to coin the terms top and bottom for the additional quarks. [42]