Fermions obey the exclusion principle, bosons do not.
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Besides, fermion loops are essential constituents of the corrections to the exchangebosonpropagators.
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All the particles that make up ordinary matter (leptons and quarks) are elementary fermions, while all the force carriers are elementary bosons.
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Particle accelerators with energies necessary to observe neutral current interactions and to measure the mass ofbosonweren't available until 1983.
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The gluons correspond to the unbroken gauge bosons and the color octet axigluons -- which couple strongly to the quarksare massive.
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One of the conclusions is that the presence of a gaugebosonmass suppresses large instantons, so that the instanton gas approximation is consistent.
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When such a theory is quantized, the quanta of the gauge fields are called "gauge bosons".
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Some of non-fundamental bosons (namely, mesons) also may transmit forces (see below), although non-fundamental ones.
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Axions and other light bosons are also expected to have an observable signature in various astrophysical settings.
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In both processes, the intermediate emission of a virtualboson(which then decays to electron and antineutrino) is not shown.
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Consequently, there are as many gauge bosons as there are generators of the gauge field.
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This is an interaction corresponding to a rotation in weak isospin space or in other words, a "transformation between and via emission of aboson".
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As explained above, "these currents mix" to create the physically observed bosons, which also leads to testable relations between the coupling constants.
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In a pair of bound bosons there is an additional component due to the orbital angular momentum.
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Therefore, at a nave theoretical level all gauge bosons are required to be massless, and the forces that they describe are required to be long-ranged.
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