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Zeitschrift f�r Physik B Condensed Matter (297)
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Binder, K. (1982). On the behavior of static susceptibilities in spin glasses. Zeitschrift F�r Physik B Condensed Matter, 48(4), 319–334.

Authors 1
  1. K. Binder (first)
References 90 Referenced 70
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  50. See e.g. Sect. 2.3.1. of Fischer, K.H.: Ref. 1; Elderfield, D., Sherrington, D.: Preprint
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  53. See, for example, the data for the field-cooled magnetization shown in Fig. 2a of [28]. Also the susceptibility calculated in Fig. 12 of [27] atT?2/3T f is temperature-independent
  54. In this example, as well as in the following, we use the exponent estimates appropriate for Heisenberg ferromagnetics ?=0.70, ?=1.38, ?=0.36, see Le Guillou, J.C., Zinn-Justin: Phys. Rev. B21, 3976 (1980) (10.1103/PhysRevB.21.3976) / Phys. Rev. B by J.C. Guillou Le (1980)
  55. Maletta, H.: Private communication
  56. Claus, H.: Private communication
  57. I am indebted to W. Kinzel for pointing this argument out to me
  58. In Ref. 7 numerical calculations based on the Sherrington-Kirkpatrick solution [2] were presented. This solution has a reentrant ferromagnetic phase boundary, and thus some qualitative similarity to the ?raw data? of the experiment was noted. Note, however, that this solution is incorrect, and the presumably correct [3] mean-field phase diagram does not show this reentrancy (Fig. 1C)
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  61. Binder, K.: Phys. Rev. Lett.45, 811 (1981) (10.1103/PhysRevLett.45.811) / Phys. Rev. Lett. by K. Binder (1981)
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  66. Binder, K.: Phys. Rev. B8, 3423 (1973) (10.1103/PhysRevB.8.3423) / Phys. Rev. B by K. Binder (1973)
  67. Binder, K.: In: Stochastic nonlinear systems in physics, chemistry and biology. Arnold, L., Lefever, R. (eds.), p. 62. Berlin, Heidelberg, New York: Springer 1981 (10.1007/978-3-642-68038-0_7) / Stochastic nonlinear systems in physics, chemistry and biology by K. Binder (1981)
  68. Penrose, O., Lebowitz, J.L.: J. Statist. Phys.3, 211 (1971) (10.1007/BF01019851) / J. Statist. Phys. by O. Penrose (1971)
  69. Langer, J.S.: Physica73, 61 (1974) (10.1016/0031-8914(74)90226-2) / Physica by J.S. Langer (1974)
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  71. see also Hertz, J.: Preprint; Hertz, J., Khurana, A., Rueskari, M.: Preprint
  72. Young, A.P.: J. Phys. C14, L1085 (1981) (10.1088/0022-3719/14/34/004) / J. Phys. C by A.P. Young (1981)
  73. Mackenzie, N.D., Young, A.P.: Phys. Rev. Lett.49, 301 (1982) (10.1103/PhysRevLett.49.301) / Phys. Rev. Lett. by N.D. Mackenzie (1982)
  74. Morgenstern, I., Horner, H.: Phys. Rev. B25, 504 (1982) (10.1103/PhysRevB.25.504) / Phys. Rev. B by I. Morgenstern (1982)
  75. Morgenstern, I.: Preprint
  76. Chalupa, J.: Solid State Commun.22, 315 (1977) (10.1016/0038-1098(77)91439-9) / Solid State Commun. by J. Chalupa (1977)
  77. Binder, K., Morgenstern, I.: (to be published); note that the analytic form of ? EA (T) asT?0 is rather uncertain, since the data of [4] are then hampered by finite-size effects
  78. Chalupa, J.: Solid State Commun.24, 429 (1977) (10.1016/0038-1098(77)91310-2) / Solid State Commun. by J. Chalupa (1977)
  79. Cragg, D.M., Sherrington, D., Gabay, M.: (to be published)
  80. Moore, M.A., Bray, A.J.: J. Phys. C15, L301 (1982) (10.1088/0022-3719/15/10/008) / J. Phys. C by M.A. Moore (1982)
  81. Gabay, M., Garel, T., Dominicis, C. de: (to be published)
  82. Elderfield, D., Sherrington, D.: (to be published)
  83. At this point, the correlation between the sign of ?S i x ? T in one of the frozen-in spin glass states and the sign ofJ ij xz is neglected. This should be reasonable for a system with dominantly diagonal exchange constants, due to superexchange as in Eu x Sr1?x S or Rudermann-Kittel interactions as in metallic spin glasses. The sign of ?S i x ? T then is in leading order due to the diagonal part
  84. Imry, Y., Ma, S.-K.: Phys. Rev. Lett.35, 1399 (1979) (10.1103/PhysRevLett.35.1399) / Phys. Rev. Lett. by Y. Imry (1979)
  85. see also Binder, K., Imry, Y., Pytte, E.: Phys. Rev. B24, 6736 (1981) and references therein (10.1103/PhysRevB.24.6736) / Phys. Rev. B by K. Binder (1981)
  86. According to a different argument by Aharony, A.: Solid State Commun.28, 667 (1978); any random disorder in the Hamiltonian, Eq. (23), should destroy long-range ferromagnetic order. Additional cubic anisotropy terms restore ferromagnetic order, however, and may lead to a first-order transition, with a spin-glass state above it. However, experimental evidence for this mechanism seems to be lacking. (10.1016/0038-1098(78)90604-X) / Solid State Commun. by A. Aharony (1978)
  87. Gebhardt, W., Kett, H., Krey, U.: (to be published)
  88. Fisch, R., Harris, A.B.: Phys. Rev. Lett.38, 785 (1977) (10.1103/PhysRevLett.38.785) / Phys. Rev. Lett. by R. Fisch (1977)
  89. Bray, A.J., Moore, M.A.: J. Phys. C12, 79 (1979) (10.1088/0022-3719/12/1/020) / J. Phys. C by A.J. Bray (1979)
  90. Banavar, J.R., Cieplak, M.: Phys. Rev. Lett.82, 832 (1982) (10.1103/PhysRevLett.48.832) / Phys. Rev. Lett. by J.R. Banavar (1982)
Dates
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Created 20 years, 4 months ago (March 25, 2005, 4:22 a.m.)
Deposited 6 years, 3 months ago (April 30, 2019, 2:09 p.m.)
Indexed 2 months, 1 week ago (June 14, 2025, 10:23 a.m.)
Issued 42 years, 8 months ago (Dec. 1, 1982)
Published 42 years, 8 months ago (Dec. 1, 1982)
Published Print 42 years, 8 months ago (Dec. 1, 1982)
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@article{Binder_1982, title={On the behavior of static susceptibilities in spin glasses}, volume={48}, ISSN={1434-6036}, url={http://dx.doi.org/10.1007/bf01305191}, DOI={10.1007/bf01305191}, number={4}, journal={Zeitschrift f�r Physik B Condensed Matter}, publisher={Springer Science and Business Media LLC}, author={Binder, K.}, year={1982}, month=dec, pages={319–334} }