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The aim of this paper is twofold. First, we shall derive the Fermi-Dirac
(FD) and Bose-Einstein (BE) distributions from the classical
Maxwell-Boltzmann (MB) distribution by introducing into the classical
system the consequences of quantum mechanical indistinguishability in a
direct and simple manner. Next, we go through a brief introduction to
feedback systems and see how the FD and BE systems may be viewed as
classical systems with appropriate feedback. We shall see that the
resemblance to feedback systems is more than formal and that a feedback
mechanism does exist in systems obeying quantum statistical mechanics.

To read the full-text of this research,

you can request a copy directly from the author.

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