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Volumn 53, Issue 10, 1996, Pages 6543-6553

Spin-glass and antiferromagnet critical behavior in a diluted fcc antiferromagnet

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EID: 2842573865     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.53.6543     Document Type: Article
Times cited : (20)

References (50)
  • 23
    • 0039847112 scopus 로고
    • A renormalization-group approach could be formulated with a Landau-Ginzburg effective free energy as a function of the order-parameter field (Formula presented). The fact that in a particular ordered configuration, only one of the ordering wave vectors can be present, translates to a "cubic" anisotropy in order-parameter space favoring the three coordinate axes. This implies a first-order phase transition [see D. J. Wallace, J. Phys. C 6, 1390 (1973)].
    • (1973) J. Phys. C , vol.6 , pp. 1390
    • Wallace, D.1
  • 32
    • 0042950803 scopus 로고
    • and compare also W. G. Wilson, Phys. Lett. A 137, 398 (1989)].
    • (1989) Phys. Lett. A , vol.137 , pp. 398
    • Wilson, W.1
  • 35
    • 4243390367 scopus 로고
    • This situation is similar to the problem of propagating order in, e.g., the three-state Potts antiferromagnet on a triangular lattice, where a single chain of bonds is insufficient to force the relationship between two clusters [see J. Adler, R. G. Palmer and H. Meyer, Phys. Rev. Lett. 58, 882 (1987).
    • (1987) Phys. Rev. Lett. , vol.58 , pp. 882
    • Adler, J.1    Palmer, R.2    Meyer, H.3
  • 36
    • 25744444598 scopus 로고
    • this is not true for a frustrated system such as the fcc antiferromagnet (compare Ref. 30) owing to its frustration and this complicates the propagation of order
    • and H. Fried and M. Schick, Phys. Rev. B 41, 4389 (1990)]. However, that problem is unfrustrated, in that the restriction of a pure system ground state to the sites of the diluted system is always one of the valid ground states; this is not true for a frustrated system such as the fcc antiferromagnet (compare Ref. 30) owing to its frustration and this complicates the propagation of order.
    • (1990) Phys. Rev. B , vol.41 , pp. 4389
    • Fried, H.1    Schick, M.2
  • 48
    • 4243259994 scopus 로고
    • On the basis of simulations, it is argued by R. Kühn and A. Huber, Phys. Rev. Lett. 73, 2268 (1994) and by J.-K. Kim and A. Patrascioiu, ibid. 72, 2785 (1994), that the critical exponents of unfrustrated diluted Ising models show a nonuniversal dilution dependence.
    • (1994) , vol.72 , pp. 2785
    • Huber, A.1    Patrascioiu, A.2
  • 50
    • 0000397729 scopus 로고    scopus 로고
    • Recently, N. Kawashima and A. P. Young [Phys. Rev. B 53, 484 (1996)] have found evidence for a finite transition temperature and ordering below (Formula presented) for the ±J Ising spin glass, indicating that the lower critical dimension is indeed below 3. Their critical exponents (ν=1.7±0.3 and η=-0.35±0.05), are slightly different from those found earlier (ν≈1.2 and η ≈-0.25). A comparison with the exponents of the present simulation suggests that the diluted fcc AFM and the Ising ±J spin glass do not lie in the same universality class.
    • (1996) Phys. Rev. B , vol.53 , pp. 484


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.