ANOMALOUS SPIN DYNAMICS IN THE PARAMAGNETIC PHASE OF SPIN GLASSES

1988 ◽  
Vol 49 (C8) ◽  
pp. C8-1045-C8-1046
Author(s):  
F. Mezei ◽  
H. Maletta ◽  
B. Farago ◽  
S. M. Shapiro
1980 ◽  
Vol 3 ◽  
Author(s):  
H. Lütgemeier ◽  
Ch. Sauer ◽  
W. Zinn

ABSTRACTThe systematic variations of experimentally determined exchange and hyperfine (h.f.) interactions between Eu2+ ions are compared firstly within the EuX (X=0,S,Se,Te) series of compounds and secondly in the magnetic dilution system EuxSr1−xS. Reasonably relations can be established between the individual nearest and next nearest neighbour exchange interactions (J1,J2 ) and the transferred h.f. interactions (ΔB1 , ΔB2 ), respectively, by considering their variations with the Eu–Eu distances (R1,R2). Using these results, the measured mean hyperfine field, BI(x), and the ferromagnetic saturation h.f. field, B↑↑ (x), of the EuxSr1−xS system can be related reasonably well to the ferro- and paramagnetic phase boundaries, Tc(x) and θ (x), respectively.


2009 ◽  
Vol 80 (14) ◽  
Author(s):  
K. Hayashi ◽  
T. Nozaki ◽  
R. Fukatsu ◽  
Y. Miyazaki ◽  
T. Kajitani

2012 ◽  
Vol 86 (8) ◽  
Author(s):  
Rong Yu ◽  
Zhentao Wang ◽  
Pallab Goswami ◽  
Andriy H. Nevidomskyy ◽  
Qimiao Si ◽  
...  

1989 ◽  
Vol 40 (7) ◽  
pp. 5036-5041 ◽  
Author(s):  
Ranjan Chaudhury ◽  
B. S. Shastry

1999 ◽  
Vol 59 (22) ◽  
pp. R14149-R14152 ◽  
Author(s):  
Peter Horsch ◽  
Janez Jaklič ◽  
Frank Mack

2022 ◽  
Vol 12 (1) ◽  
Author(s):  
Silvio Franz ◽  
Flavio Nicoletti ◽  
Giorgio Parisi ◽  
Federico Ricci-Tersenghi

We study the energy minima of the fully-connected mm-components vector spin glass model at zero temperature in an external magnetic field for m\ge 3m≥3. The model has a zero temperature transition from a paramagnetic phase at high field to a spin glass phase at low field. We study the eigenvalues and eigenvectors of the Hessian in the minima of the Hamiltonian. The spectrum is gapless both in the paramagnetic and in the spin glass phase, with a pseudo-gap behaving as \lambda^{m-1}λm−1 in the paramagnetic phase and as \sqrt{\lambda}λ at criticality and in the spin glass phase. Despite the long-range nature of the model, the eigenstates close to the edge of the spectrum display quasi-localization properties. We show that the paramagnetic to spin glass transition corresponds to delocalization of the edge eigenvectors. We solve the model by the cavity method in the thermodynamic limit. We also perform numerical minimization of the Hamiltonian for N\le 2048N≤2048 and compute the spectral properties, that show very strong corrections to the asymptotic scaling approaching the critical point.


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