| dc.description.abstract | Statistical mechanics to show how the nature of many particle systems makrospic
touch with nature itself mikrospic particles, statistical mechanics do not question the
actual movement or interaction the individual particles, but questioned the behavior of
particles with the greatest opportunity to occupy a particular energy state.
Maxwell-Bolztmann statistics applied to the identical system with
distinguishable particles, each particle is enough to spin away from where the wave
function does not clasping and categorized as classical particles, for example, the gas
molecules. Bose-Enstein statistics applied to systems that are identical and
indistinguishable particles that do not meet the exclusion principle, each spin particles:
0,1,2, ... with a symmetric wave function for the exchange of labels and categorized
Boson particle, for example: liquid helium in solids , photons in the cavity, and
Phonon in a solid. Fermi-Dirac statistics apply to systems that are identical and
indistinguishable particles that satisfy the exclusion principle, each spin of particles:
1/ 2, 3 / 2, 5 / 2, ... with the anti-symmetric wave function for the exchange of particles
and particle labels categorized fermions. | en_US |
