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(Received 11 September 1998)
Phase diagrams as a function of anisotropy D and magnetic field H are obtained for discommensurations and surface states for an antiferromagnet in which H is parallel to the easy axis, by modeling it using the ground states of a one-dimensional chain of classical XY spins. A surface spin-flop phase exists for all D, but the interval in H over which it is stable becomes extremely small as D goes to zero. First-order transitions, separating different surface states and ending in critical points, exist inside the surface spin-flop region. They accumulate at a field H
(depending on D) significantly less than the value HSF for a bulk spin-flop transition. For H
< H < HSF there is no surface spin-flop phase in the strict sense; instead, the surface restructures by, in effect, producing a discommensuration infinitely far away in the bulk. The results are used to explain in detail the phase transitions occurring in systems consisting of a finite, even number of layers.
©1999 The American Physical Society
URL: http://link.aps.org/abstract/PRB/v59/p6239
PACS:
75.10.Hk, 75.50.Ee, 75.30.Gw, 68.35.Rh
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