Abstract
We discuss the nature of symmetry breaking in quantum antiferromagnets. We show that published arguments concerning the order parameter for the 2d s =1/2 Heisenberg antiferromagnet have to be reconsidered. These had led to 3‾√3textbackslashsqrt3 and 1 for the ratio r of the mean z -component m of the staggered spin per particle m s z in an infinitesimal staggered field B , to the r.m.s. value m 0 of m s z with B =0, in the thermodynamic limit. We give arguments which put doubt on both values. Also we prove r ≧1, given m 0 ≠0.
Original language | English |
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Pages (from-to) | 3894-3898 |
Number of pages | 5 |
Journal | Journal of the Physical Society of Japan |
Volume | 58 |
Issue number | 11 |
DOIs | |
Publication status | Published - 1 Nov 1989 |