Bloch wall phase transition in the anisotropic spherical model (abstract)

1997 ◽  
Vol 81 (8) ◽  
pp. 4148-4148 ◽  
Author(s):  
D. A. Garanin
Nature ◽  
1993 ◽  
Vol 361 (6414) ◽  
pp. 699-704 ◽  
Author(s):  
Paul J. Tackley ◽  
David J. Stevenson ◽  
Gary A. Glatzmaier ◽  
Gerald Schubert

2021 ◽  
Vol 87 (6) ◽  
Author(s):  
Chjan C. Lim

An equilibrium statistical mechanics theory for the Hasegawa–Mima equations of toroidal plasmas, with canonical constraint on energy and microcanonical constraint on potential enstrophy, is solved exactly as a spherical model. The use of a canonical energy constraint instead of a fixed-energy microcanonical approach is justified by the preference for viewing real plasmas as an open system. A significant consequence of the results obtained from the partition function, free energy and critical temperature, is the condensation into a ground state exhibiting a blob-hole-like structure observed in real plasmas.


1991 ◽  
Vol 69 (6) ◽  
pp. 753-760 ◽  
Author(s):  
Scott Allen ◽  
R. K. Pathria

The analysis of a previous study (Allen and Pathria. Can. J. Phys. 67, 952 (1989)) on finite-size effects in systems with O(n) symmetry [Formula: see text], confined to geometry Ld−d′ × ∞d′ (where d and d′ are continuous variables such that 2 < d′ < d < 4) and subjected to periodic boundary conditions, is extended (i) to include the region of first-order phase transition (T < Tc) as well as the region of second-order phase transition [Formula: see text] and (ii) to allow the presence of an external field H > 0. Predictions, involving both amplitudes and exponents, are made on the magnetization m and susceptibility χ in different regimes of the variables T, H, and L. Analytical verification of the predicted results is carried out in the case of the spherical model of ferromagnetism (n = ∞), and complete agreement is found.


1969 ◽  
Vol 10 (8) ◽  
pp. 1403-1406 ◽  
Author(s):  
Elliott H. Lieb ◽  
Colin J. Thompson

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