Abstract

The hysteresis loop in the zero-temperature random-field Ising model exhibits a critical point as the width of the disorder increases. Above six dimensions, the critical exponents of this transition, where the ``infinite avalanche'' first disappears, are described by mean-field theory. We expand the critical exponents about mean-field theory, in 6-\ensuremath{\epsilon} dimensions, to first order in \ensuremath{\epsilon}. Despite \ensuremath{\epsilon}=3, the values obtained agree reasonably well with the numerical values in three dimensions.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.