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womos Jn clarical mechawics So the probakectity of farticles is nglig ible and thus heated as distingusishab le . a cell untaining tuo r mane ngligible (oceu potime 1) 1 ) The pautily camot be heated as diting wihable ,we theu une when vcu Index quantiur stati,ties. at hower energies FD -3 - 2 MB e So BE and FD will an tend to Me. when Hightemperature and las ぐ。 Condition. when TくY strongly adogerarate TくY di «1
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Transcribed Image Text:womos Jn clarical mechawics So the probakectity of farticles is nglig ible and thus heated as distingusishab le . a cell untaining tuo r mane ngligible (oceu potime 1) 1 ) The pautily camot be heated as diting wihable ,we theu une when vcu Index quantiur stati,ties. at hower energies FD -3 - 2 MB e So BE and FD will an tend to Me. when Hightemperature and las ぐ。 Condition. when TくY strongly adogerarate TくY di «1
In the approximation A < 1, Fermi-Dirac and Bose-Einstein statistics both tend to Maxwell-Boltzmann statistics: 1 + e4/kT . e-e/kT. (€ — м) exp 土1 kT
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Transcribed Image Text:In the approximation A < 1, Fermi-Dirac and Bose-Einstein statistics both tend to Maxwell-Boltzmann statistics: 1 + e4/kT . e-e/kT. (€ — м) exp 土1 kT
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