✦ LIBER ✦

The asymmetric continuous distribution function of the effective field of the Ising model in the spin glass and the ferromagnetic states on the Bethe lattice

✍ Scribed by Mitsuhiro Sasaki; Shigetoshi Katsura

Publisher: Elsevier Science
Year: 1989
Tongue: English
Weight: 329 KB
Volume: 157
Category: Article
ISSN: 0378-4371
DOI: 10.1016/0378-4371(89)90039-3

No coin nor oath required. For personal study only.

📜 SIMILAR VOLUMES

The distribution function of the effecti

The distribution function of the effective field of the Ising spin glass on the Bethe Lattice for the coordination number z = 4, 5, 6

✍ Mitsuhiro Sasaki; Shigetoshi Katsura 📂 Article 📅 1989 🏛 Elsevier Science 🌐 English ⚖ 573 KB

The continuous distribution function of

The continuous distribution function of the effective fields of the Ising spin glass of the ±J model

✍ Shigetoshi Katsura 📂 Article 📅 1987 🏛 Elsevier Science 🌐 English ⚖ 270 KB

The continuous distribution function of

The continuous distribution function of the effective fields of the Ising spin glass of the ±J model

✍ Shigetoshi Katsura 📂 Article 📅 1988 🏛 Elsevier Science 🌐 English ⚖ 37 KB

Variational principle for the distributi

Variational principle for the distribution function of the effective field for the random Ising model in the Bethe approximation

✍ T. Morita 📂 Article 📅 1979 🏛 Elsevier Science 🌐 English ⚖ 367 KB

The free energy at T = 0 of the spin gla

The free energy at T = 0 of the spin glass in the case of the continuous distribution of the effective field on the Bethe lattice for Z = 4, 5, 6

✍ Eiichi Akagi; Mitsuhiro Seino; Shigetoshi Katsura 📂 Article 📅 1991 🏛 Elsevier Science 🌐 English ⚖ 384 KB

The boundary between the spin-glass and

The boundary between the spin-glass and ferromagnetic states of the bond-random Ising model in the square lattice at T = 0

✍ Shigetoshi Katsura; Toshiyuki Suenaga; Takahiro Imaizumi 📂 Article 📅 1982 🏛 Elsevier Science 🌐 English ⚖ 516 KB

The bond-random (-tJ) Ising model in the square lattice is considered in the square cluster approximation. The boundary between the ferromagnetic and spin-glass states at T = 0 is obtained as the transition point from the asymmetric distribution of the effective fields to the symmetric distribution.