Finite Size Effects on Spin Glass Dynamics
| dc.creator | Joh, Y. G. | |
| dc.creator | Orbach, R. | |
| dc.creator | Wood, G. G. | |
| dc.creator | Hammann, J. | |
| dc.creator | Vincent, E. | |
| dc.date | 2000-02-02 | |
| dc.date | 2000-02-08 | |
| dc.date.accessioned | 2026-07-07T02:36:41Z | |
| dc.date.available | 2026-07-07T02:36:41Z | |
| dc.description | The recent identification of a time and temperature dependent spin glass correlation length, $ξ({t_w},T)$, has consequences for samples of finite size. Qualitative arguments are given on this basis for departures from t/{t_w} scaling for the time decay of the thermoremanent magnetization, {M_{TRM}}(t,{t_w},T), where t is the measurement time after a ``waiting time'' t_w, and for the imaginary part of the ac susceptibility, ${χ^{{\prime}{\prime}}}(ω,t)$. Consistency is obtained for a more rapid decay of $M_{TRM}(t,{t_w},T)$ with increasing t_w when plotted as a function of t/{t_w}, for the deviation of the characteristic time for {M_{TRM}}(t,{t_w},T) from a linear dependence upon H^2 at larger values of H, and for the deviation of the decay of ${χ^{{\prime}{\prime}}}(ω,t)$ from $ωt$ scaling upon a change in magnetic field at large values of $ωt$. These departures from scaling can, in principle, be used to extract the particle size distribution for a given spin glass sample. | |
| dc.description | 9 pages, 5 eps figures (typos corrected) | |
| dc.identifier | https://arxiv.org/abs/cond-mat/0002040 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/0002040 | |
| dc.identifier | J. Phys. Soc. Jpn. 69 (2000) Suppl. A, pp. 215-222 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/16013 | |
| dc.subject | Disordered Systems and Neural Networks | |
| dc.subject | Statistical Mechanics | |
| dc.title | Finite Size Effects on Spin Glass Dynamics | |
| dc.type | text |