We examine Bose-Einstein condensation (BEC) for particles trapped in a harm
onic potential by considering it as a transition in the length of permutati
on cycles that arise from wave-function symmetry. This "loop-gas" approach
was originally developed by Feynman in his path-integral study of BEC for a
homogeneous gas in a box. For the harmonic oscillator potential it is poss
ible to treat the ideal gas exactly so that one can easily see how standard
approximations become more accurate in the thermodynamic limit (TDL). One
clearly sees that the condensate is made up of very long permutation loops
whose length fluctuates ever more widely as the number of particles increas
es. In the TDL, the Wentzel-Kramers-Brillouin approximation, equivalent to
the standard approach to BEG, becomes precise for the noncondensate; howeve
r, this approximation neglects completely the long cycles that make up the
condensate. We examine the exact form for the density matrix for the system
and show how it describes the condensate and behaves in the TDL. (C) 2000
American Association of Physics teachers.