We present a general strategy to extend quantum cluster algorithms for S0ex0ex=0ex0ex1/2 spin systems, such as the loop algorithm, to those with an arbitrary size of spins. The partition function of a high- S spin system is generally represented by the path integral of a S0ex0ex=0ex0ex1/2 model with special boundary conditions in the imaginary-time direction. We introduce additional graphs for the boundary part and give the labeling probability explicitly, which completes the algorithm together with an existing S0ex0ex=0ex0ex1/2 algorithm. As a demonstration, we simulate the integer-spin antiferromagnetic Heisenberg chains. The magnitude of the first excitation gap is estimated to be 0.41048(6), 0.08917(4), and 0.01002(3) for S0ex0ex=0ex0ex1, 2, and 3, respectively.
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Todo et al. (2001) studied this question.
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