We study a Hamiltonian of S = 1/2 spins with two-, three and four-spin
exchange interactions on the triangular lattice as a possible model o
f the nuclear magnetism of solid He-3 layers. The spin wave theory sho
ws that the ''tetrahedral'' ground state, which was shown to be favour
ed by the four-spin exchange interaction in our previous paper, is sta
ble against quantum fluctuations in some parameter region. Since this
state has a scalar chiral long-range order, a phase transition occurs
at a finite temperature even. though the Hamiltonian has a full rotati
onal symmetry in the spin space. critical behavior of this phase trans
ition was examined by classical Monte Carlo simulations. The specific
heat diverges much more strongly than that of the 2D Ising model.