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This has some profound consequences: Elementary bosons with other spins (0, 2, 3, etc.) were not historically known to exist, although they have received considerable theoretical treatment and are well established within their respective mainstream theories.In particular, theoreticians have proposed the graviton (predicted to exist by some quantum gravity theories) with spin 2, and the Higgs boson (explaining electroweak symmetry breaking) with spin 0.Rutherford · Thomson · Chadwick · Bose · Sudarshan · Koshiba · Davis Jr.· Anderson · Fermi · Dirac · Feynman · Rubbia · Gell-Mann · Kendall · Taylor · Friedman · Powell · P. Anderson · Glashow · Iliopoulos · Maiani · Meer · Cowan · Nambu · Chamberlain · Cabibbo · Schwartz · Perl · Majorana · Weinberg · Lee · Ward · Salam · Kobayashi · Maskawa · Yang · Yukawa · 't Hooft · Veltman · Gross · Politzer · Wilczek · Cronin · Fitch · Vleck · Higgs · Englert · Brout · Hagen · Guralnik · Kibble · Ting · Richter Spin is one of two types of angular momentum in quantum mechanics, the other being orbital angular momentum.One of the triumphs of the theory of quantum electrodynamics is its accurate prediction of the electron Composite particles also possess magnetic moments associated with their spin.In particular, the neutron possesses a non-zero magnetic moment despite being electrically neutral.The minimally extended Standard Model that takes into account non-zero neutrino masses predicts neutrino magnetic moments of: is the Bohr magneton.New physics above the electroweak scale could, however, lead to significantly higher neutrino magnetic moments.

The spin-statistics theorem states (1) that particles with half-integer spin (fermions) obey Fermi–Dirac statistics and the Pauli Exclusion Principle, and (2) that particles with integer spin (bosons) obey Bose–Einstein statistics, occupy "symmetric states", and thus can share quantum states.The magnetic moment of the neutron comes from the spins of the individual quarks and their orbital motions.Neutrinos are both elementary and electrically the deflection of particles by inhomogeneous magnetic fields in a Stern–Gerlach experiment, or by measuring the magnetic fields generated by the particles themselves. For exclusively orbital rotations it would be 1 (assuming that the mass and the charge occupy spheres of equal radius).The electron, being a charged elementary particle, possesses a nonzero magnetic moment.

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