We consider Bose-Einstein condensation for non-interacting particles trappe
d in a harmonic potential by considering the length of permutation cycles a
rising from wave function symmetry. This approach had been considered previ
ously by Matsubara and Feynman for a homogeneous gas in a box with periodic
boundary conditions. For the ideal gas in a harmonic potential, one can tr
eat the problem nearly exactly by analytical means. One clearly sees that t
he noncondensate is made up of permutation loops that are of length less th
an or equal to N-1/3, and that the phase transition consists of the sudden
growth of longer permutation cycles. The condensate is seen to consist of c
ycles of all possible lengths with nearly equal likelihood. (C) 2000 Elsevi
er Science B.V. All rights reserved.