The Boltzmann temperature and Lagrange multiplier

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dc.creatorWada, T.
dc.creatorScarfone, A. M.
dc.date2005-09-14
dc.date.accessioned2026-07-07T03:06:37Z
dc.date.available2026-07-07T03:06:37Z
dc.descriptionWe consider the relation between the Boltzmann temperature and the Lagrange multipliers associated with energy average in the nonextensive thermostatistics. In Tsallis' canonical ensemble, the Boltzmann temperature depends on energy through the probability distribution unless $q=1$. It is shown that the so-called 'physical temperature' introduced in [Phys. Lett. A \textbf{281} (2001) 126] is nothing but the ensemble average of the Boltzmann temperature.
dc.description8 pages, no figure. The International conference Complexity and Nonextensivity: New Trends in Statistical Mechanics. - Yukawa Institute for Theoretical Physics - (14-18 March 2005) Kyoto, Japan
dc.identifierhttps://arxiv.org/abs/cond-mat/0509367
dc.identifierhttp://arxiv.org/abs/cond-mat/0509367
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/26877
dc.subjectStatistical Mechanics
dc.titleThe Boltzmann temperature and Lagrange multiplier
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