Spin systems on hierarchical lattices. Introduction and thermodynamic limit

1982 ◽  
Vol 26 (9) ◽  
pp. 5022-5032 ◽  
Author(s):  
Robert B. Griffiths ◽  
Miron Kaufman
1984 ◽  
Vol 30 (1) ◽  
pp. 244-249 ◽  
Author(s):  
Miron Kaufman ◽  
Robert B. Griffiths

1970 ◽  
Vol 23 (5) ◽  
pp. 927 ◽  
Author(s):  
RW Gibberd

The partition function and the Gibb's free energy are calculated exactly in the thermodynamic limit, using techniques which are well known in the theory of superconductivity. This calculation illustrates explicitly the similarity between the phase transition in superconductivity and the molecular field transitions in spin systems.


2006 ◽  
Vol 20 (17) ◽  
pp. 1059-1066 ◽  
Author(s):  
MARCO FRASCA

Intrinsic decoherence in the thermodynamic limit is shown for a large class of many-body quantum systems in the unitary evolution in NMR and cavity QED. The effect largely depends on the inability of the system to recover the phases. Gaussian decaying in time of the fidelity is proved for spin systems and radiation-matter interaction.


2020 ◽  
Vol 8 (2) ◽  
Author(s):  
Christiaan J. F. van de Ven ◽  
Gerrit C. Groenenboom ◽  
Robin Reuvers ◽  
Klaas Landsman

Spontaneous symmetry breaking (ssb) is mathematically tied to some limit, but must physically occur, approximately, before the limit. Approximate ssb has been independently understood for Schrödinger operators with double well potential in the classical limit (Jona-Lasinio et al, 1981; Simon, 1985) and for quantum spin systems in the thermodynamic limit (Anderson, 1952; Tasaki, 2019). We relate these to each other in the context of the Curie–Weiss model, establishing a remarkable relationship between this model (for finite NN) and a discretized Schrödinger operator with double well potential.


1996 ◽  
Vol 89 (5) ◽  
pp. 1397-1408 ◽  
Author(s):  
LAWRENCE LOHR

1975 ◽  
Vol 116 (7) ◽  
pp. 485 ◽  
Author(s):  
V.G. Pokazan'ev ◽  
G.V. Skrotskii ◽  
L.I. Yakub

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