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

Daniel M Danchev-+ and Nicholay S Tonchev++

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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.


PACS

03.65.Pm Relativistic wave equations

05.40.-a Fluctuation phenomena, random processes, noise, and Brownian motion

11.10.Jj Asymptotic problems and properties

11.10.Wx Finite-temperature field theory

MSC

81T40 Two-dimensional field theories, conformal field theories, etc.

82B27 Critical phenomena

Subjects

Particle physics and field theory

Statistical physics and nonlinear systems

Quantum information and quantum mechanics

Dates

Issue 41 (15 October 1999)

Received 16 March 1999



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