Relaxation of Thermoremanent Magnetization in Different Magnetic Phases Of Fe-rich $\mbox{$γ$}$-FeNiCr Alloys
| dc.creator | Sinha, G. | |
| dc.creator | Chatterjee, R. | |
| dc.creator | Uehara, M. | |
| dc.creator | Majumdar, A. K. | |
| dc.date | 1995-08-25 | |
| dc.date.accessioned | 2026-07-07T03:07:52Z | |
| dc.date.available | 2026-07-07T03:07:52Z | |
| dc.description | The time decay of the thermoremanent magnetization(TRM) of the $\mbox{Fe}_{80-\mbox{x}}\mbox{Ni}_{\mbox{x}}\mbox{Cr}_{20}$ ($14\leq \mbox{x} \leq 30$) alloys has been measured for four different magnetic phases within the fcc $\mbox{$γ$}$-phase using a SQUID magnetometer. In the spin-glass phase(SG)(X=19) very distinct ageing effects are observed where M(t) can be described as $M(t)=M_0(t/t_{w})^{-γ}\exp[-(t/τ)^{1-n}]$ for the entire time domain. In the reentrant spin-glass(RSG)(X= 23 and 26), M(t) can be better represented by the stretched exponential with an addition of a constant term which can be well explained by the Gabay-Toulouse(GT) model. We have also measured the linear and non-linear ac susceptibilities for the sample X=23 and confirmed the presence of the ferromagnetic(FM) ordering down to the lowest temperature. In the RSG(X=23), the TRM shows a minimum near T$_{\mbox{c}}$ and a local maximum just above T$_{\mbox{c}}$. In the FM phase (X=30) the popular prediction of the power law decay of the TRM is observed. The latter is indistinguishable from the stretched exponential in the antiferromagnetic(AF) phase (X=14). | |
| dc.description | Figures available upon request | |
| dc.identifier | https://arxiv.org/abs/cond-mat/9508116 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/9508116 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/27334 | |
| dc.subject | Condensed Matter | |
| dc.title | Relaxation of Thermoremanent Magnetization in Different Magnetic Phases Of Fe-rich $\mbox{$γ$}$-FeNiCr Alloys | |
| dc.type | text |