FermionEn physique des particules, un fermion (nom attribué par Paul Dirac d'après Enrico Fermi) est une particule de spin demi-entier (c'est-à-dire 1/2, 3/2, 5/2...). Elle obéit à la statistique de Fermi-Dirac. Un fermion peut être une particule élémentaire, tel l'électron, ou une particule composite, tel le proton, ou toutes leurs antiparticules. Toutes les particules élémentaires observées sont soit des fermions, soit des bosons (l'hypothétique matière noire, encore non observée en , n'est actuellement pas catégorisée).
Energy–momentum relationIn physics, the energy–momentum relation, or relativistic dispersion relation, is the relativistic equation relating total energy (which is also called relativistic energy) to invariant mass (which is also called rest mass) and momentum. It is the extension of mass–energy equivalence for bodies or systems with non-zero momentum. It can be written as the following equation: This equation holds for a body or system, such as one or more particles, with total energy E, invariant mass m0, and momentum of magnitude p; the constant c is the speed of light.
Abstract ImagistsAbstract Imagists is a term derived from a 1961 exhibition in the Guggenheim Museum, New York called American Abstract Expressionists and Imagists. This exhibition was the first in the series of programs for the investigation of tendencies in American and European painting and sculpture. It had been recognized that the paintings of Josef Albers, Barnett Newman, Mark Rothko, Adolph Gottlieb, Ad Reinhardt, Clyfford Still and Robert Motherwell were all very different yet the symbolic content was achieved "through dramatic statement of isolated and highly simplified elements.
