2001
DOI: 10.1134/1.1417166
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On critical behavior of phase transitions in certain antiferromagnets with complicated ordering

Abstract: Within the four-loop ε expansion, we study the critical behavior of certain antiferromagnets with complicated ordering. We show that an anisotropic stable fixed point governs the phase transitions with new critical exponents. This is supported by the estimate of critical dimensionality N C c = 1.445(20) obtained from six loops via the exact relation N C c = 1 2 N R c established for the real and complex hypercubic models.

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Cited by 10 publications
(13 citation statements)
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“…This method, proposed in [16] and extensively reviewed in [17], makes no assumptions on the underlying microscopic description and studies CFTs based only on global and conformal symmetry, unitarity, and consistency with the operator algebra (crossing symmetry). In agreement with the experimental (20,2). The allowed region lies below the curves for the corresponding parameter values.…”
Section: Introductionsupporting
confidence: 88%
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“…This method, proposed in [16] and extensively reviewed in [17], makes no assumptions on the underlying microscopic description and studies CFTs based only on global and conformal symmetry, unitarity, and consistency with the operator algebra (crossing symmetry). In agreement with the experimental (20,2). The allowed region lies below the curves for the corresponding parameter values.…”
Section: Introductionsupporting
confidence: 88%
“…While the critical exponents corresponding to the second kink show reasonable agreement, within uncertainties, with the results of [8,19], neither set of values is compatible with the predictions from the expansion, which gives β = 0.370 (5) and ν = 0.715(10) [20,21]. 3 Although it was speculated in [15] that the first kink may be related to the expansion through the large m limit, the results of that study were not sufficient to make any conclusive statements.…”
Section: Introductionsupporting
confidence: 50%
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“…Past discussions include [46,47,48]. The β-functions for such theories have been determined to four loops [49,50] for m = 2 and are physically relevant for m = 2, n = 2, 3. For m = n = 2 this case with O(2) 2 symmetry is identical with the O(2) × O(2) symmetric theory, taking…”
Section: N Fixed Pointsmentioning
confidence: 99%
“…The polynomial f (x), as defined in (5.14), now has roots, apart from x = 0, given by For m = 2, n = 2, 3 results to four loops are given in [50] (where κ = −2ω). The fixed point realised for x * = x + corresponds to decoupled O(m) theories, this is the stable fixed point for m > 4.…”
Section: N Fixed Pointsmentioning
confidence: 99%