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  2. List of particles - Wikipedia

    en.wikipedia.org/wiki/List_of_particles

    Fermions have half-integer spin; for all known elementary fermions this is ⁠ 1 / 2 ⁠. All known fermions except neutrinos, are also Dirac fermions; that is, each known fermion has its own distinct antiparticle. It is not known whether the neutrino is a Dirac fermion or a Majorana fermion. [4] Fermions are the basic building blocks of all ...

  3. Spin (physics) - Wikipedia

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

    The conventional definition of the spin quantum number is s = ⁠ n / 2 ⁠, where n can be any non-negative integer. Hence the allowed values of s are 0, ⁠ 1 / 2 ⁠, 1, ⁠ 3 / 2 ⁠, 2, etc. The value of s for an elementary particle depends only on the type of particle and cannot be altered in any known way (in contrast to the spin ...

  4. Pauli exclusion principle - Wikipedia

    en.wikipedia.org/wiki/Pauli_exclusion_principle

    Atoms can have different overall spin, which determines whether they are fermions or bosons: for example, helium-3 has spin 1/2 and is therefore a fermion, whereas helium-4 has spin 0 and is a boson. [ 2 ] : 123–125 The Pauli exclusion principle underpins many properties of everyday matter, from its large-scale stability to the chemical ...

  5. Spin quantum number - Wikipedia

    en.wikipedia.org/wiki/Spin_quantum_number

    The atom would then be pulled toward or away from the stronger magnetic field a specific amount, depending on the value of the valence electron's spin. When the spin of the electron is ⁠+ + 1 / 2 ⁠ the atom moves away from the stronger field, and when the spin is ⁠− + 1 / 2 ⁠ the atom moves toward it. Thus the beam of silver atoms is ...

  6. Gyromagnetic ratio - Wikipedia

    en.wikipedia.org/wiki/Gyromagnetic_ratio

    An example for such a particle [9] is the spin ⁠ 1 / 2 ⁠ companion to spin ⁠ 3 / 2 ⁠ in the D (½,1) ⊕ D (1,½) representation space of the Lorentz group. This particle has been shown to be characterized by g = ⁠− + 2 / 3 ⁠ and consequently to behave as a truly quadratic fermion.

  7. Electron pair - Wikipedia

    en.wikipedia.org/wiki/Electron_pair

    In both cases a bond is created by the formation of an electron pair. Because electrons are fermions, the Pauli exclusion principle forbids these particles from having all the same quantum numbers. Therefore, for two electrons to occupy the same orbital, and thereby have the same orbital quantum number, they must have different spin quantum ...

  8. Fermion - Wikipedia

    en.wikipedia.org/wiki/Fermion

    More precisely, because of the relation between spin and statistics, a particle containing an odd number of fermions is itself a fermion. It will have half-integer spin. Examples include the following: A baryon, such as the proton or neutron, contains three fermionic quarks. The nucleus of a carbon-13 atom contains six protons and seven neutrons.

  9. Spin polarization - Wikipedia

    en.wikipedia.org/wiki/Spin_polarization

    In particle physics, spin polarization is the degree to which the spin, i.e., the intrinsic angular momentum of elementary particles, is aligned with a given direction. [1] This property may pertain to the spin, hence to the magnetic moment , of conduction electrons in ferromagnetic metals, such as iron , giving rise to spin-polarized currents .