We discuss the probability distribution function for the magnetic order par
ameter M, in the low temperature phase of the two-dimensional XY model. In
this phase the system is critical over the whole range of temperature. The
thermally averaged value of the order parameter [M], which is zero in the t
hermodynamic limit, has abnormally large finite size corrections. An exact
result, within a spin wave calculation gives [M] = (1/2N)(T/8 pi J), where
J is the magnetic exchange constant and N the number of spins. We show, usi
ng Monte Carlo simulation, that the distribution function, Q(y - [y]), y =
(T-1LT/4 pi J) M, is asymmetric universal function. Using a diagramatic tec
hnique, we show that the asymmetry comes from three-spin and higher correla
tions. If only two-spin correlations are considered, the distribution is Ga
ussian. However, as there are contributions from two-spin terms separated b
y all distances, the distribution remains broad and is consistent with a di
vergent susceptibility. (C) 1998 American Institute of Physics. [S0021-8979
(98)51911-1].