The results of extensive Monte Carlo simulations are reported on X Y and Heisenberg antiferromagnets on a d =3-dimensional stacked-triangular lattice, which are expected to belong to the recently identified n =2 and 3 chiral universality classes, respectively. The lattices studied consist of L 3 spins with 18≤ L ≤60. The study is an extension of earlier Monte Carlo simulations for the same system with smaller lattices. A continuous transition characterized by the novel critical exponents is found with α=0.34±0.06, β=0.253±0.01, γ=1.13±0.05 and ν=0.54±0.02 for the X Y ( n =2) case, and with α=0.24±0.08, β=0.30±0.02, γ=1.17±0.07 and ν=0.59±0.02 for the Heisenberg ( n =3) case. The specific-heat amplitude ratio is estimated to be A + / A - =0.36±0.2 and A + / A - =0.54±0.2 in the n =2 and n =3 cases, respectively. The nature of the chiral ordering is also studied, and various chirality exponents are determined. The results are discussed in conjunction with the recent renormalization-group calculations and experiments.
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Hikaru Kawamura (1992) studied this question.
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