(statistical mechanics) The factor exp(E/kT) that appears in the expression giving the probability for atoms to have an excitation energy E when at temperature T, where k is the Boltzmann constant.
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(statistical mechanics) The factor exp(E/kT) that appears in the expression giving the probability for atoms to have an excitation energy E when at temperature T, where k is the Boltzmann constant.
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In physics, the Boltzmann factor is a weighting factor that determines the relative probability of a state i in a multi-state system in thermodynamic equilibrium at temperature T.

Where kB is Boltzmann's constant, and Ei is the energy of state i. The ratio of the probabilities of two states is given by the ratio of their Boltzmann factors.
The Boltzmann factor is not a probability by itself, because it is not normalized. The normalization factor is one divided by the Partition Function (denoted as Z), the sum of the Boltzmann factors for all states of the system. This gives the Boltzmann distribution.
From the Boltzmann factor it is possible to derive the Maxwell-Boltzmann statistics, Bose-Einstein statistics, and Fermi-Dirac statistics that govern classical particles as well as quantum mechanical bosons, and fermions, respectively.
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| Statistical weight | |
| Canonical probability distribution | |
| Excitation temperature |
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