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On the finite-temperature generalization of the C-theorem and the interplay between classical and quantum fluctuations

Daniel M Danchev et al 1999 J. Phys. A: Math. Gen. 32 7057-7070   doi: 10.1088/0305-4470/32/41/302  Help

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Daniel M Danchev-+ and Nicholay S Tonchev++
-+ Institute of Mechanics, Bulgarian Academy of Sciences, Acad G, Bonchev St blvd 4, 1113 Sofia, Bulgaria
++ Institute of Solid State Physics, Bulgarian Academy of Sciences, Tzarigradsko chaussée blvd 72, 1784 Sofia, Bulgaria

Abstract. The behaviour of the finite-temperature C-function, defined by Neto and Fradkin (1993 Nucl. Phys. B 400 525), is analysed within a d -dimensional exactly solvable lattice model, recently considered by Vojta (1996 Phys. Rev. B 53 710), which is of the same universality class as the quantum nonlinear O(n) sigma model in the limit nrightarrowinfty. The scaling functions of C for the cases d = 1 (absence of long-range order), d = 2 (existence of a quantum critical point), d = 4 (existence of a line of finite-temperature critical points that ends up with a quantum critical point) are derived and analysed. The locations of regions where C is monotonically increasing (which depend significantly on d) are exactly determined. The results are interpreted within the finite-size scaling theory that has to be modified for d = 4.

Print publication: Issue 41 (15 October 1999)
Received 16 March 1999

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