Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

The Method of Gauge Transformation in Random Spin Systems

之康 尾関, Yukiyasu Ozeki

Published Jan 1, 1996• 0 citations
OpenAlex

Related papers

Gauge Transformation for Dynamical Systems of Ising Spin Glasses

之康 尾関, Yukiyasu Ozeki

•Jan 1, 1995•0 citations

Non-Frustrated Random Spin Systems with Gauge Symmetry

之康 尾関, Yukiyasu Ozeki

•Jan 1, 1996•0 citations

Potential fields and the generalized gauge transformation in the theory of spin particles

Bernard Kwal

•Jun 1, 1949•0 citations

Numerical study of phase diagram and reentrance in random spin systems without gauge symmetry

Yukiyasu Ozeki, 尾関 之康

•Jan 1, 1995•0 citations

Non-frustrated random spin systems with gauge symmetry

Yukiyasu Ozeki

We introduce a class of random spin systems without frustration, which satisfies the conditions for gauge symmetry. The method of gauge transformation provides several properties on the phase diagram of gauge symmetric models; this method is almost rigorous, while the derivation for the absence of re-entrance contains unproved assumption. In the present random models, the absence of re-entrance can be shown exactly. Furthermore, the phase diagram and the critical properties are exactly related with those in the original pure system. The present random systems correspond to the Mattis model with asymmetric bond distribution in the Ising case, and a kind of the gauge glass model in the XY case. In the case of the clock model in two dimensions, we find a new thermodynamic phase which has long-range spin-glass correlation with critical (power-decaying) ferromagnetic correlation.

Journal of Physics A Mathematical and General•Sep 21, 1996•3 citations

Statistical mechanics of quantum spin systems

Derek W. Robinson

Communications in Mathematical Physics•Jun 1, 1967•65 citations
We introduce a class of random spin systems without frustration, which satisfies the conditions for gauge symmetry. The method of gauge transformation provides several properties on the phase diagram of gauge symmetric models; this method is almost rigorous, while the derivation for the absence of re-entrance contains unproved assumption. In the present random models, the absence of re-entrance can be shown exactly. Furthermore, the phase diagram and the critical properties are exactly related with those in the original pure system. The present random systems correspond to the Mattis model with asymmetric bond distribution in the Ising case, and a kind of the gauge glass model in the XY case. In the case of the clock model in two dimensions, we find a new thermodynamic phase which has long-range spin-glass correlation with critical (power-decaying) ferromagnetic correlation.