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2007
DOI: 10.1103/physrevb.75.014105
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Unified static renormalization-group treatment of finite-temperature crossovers close to a quantum critical point

Abstract: A nonconventional renormalization-group (RG) treatment close to and below four dimensions is used to explore, in a unified and systematic way, the low-temperature properties of a wide class of systems in the influence domain of their quantum critical point. The approach consists in a preliminary averaging over quantum degrees of freedom and a successive employment of the Wilsonian RG transformation to treat the resulting effective classical Ginzburg-Landau free energy functional. This allows us to perform a de… Show more

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Cited by 19 publications
(3 citation statements)
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“…) where H 0 = J(0) + 17 18 I(0) − 2 3 D. Then, to order of interest for H → 0 we have the required critical line equation…”
Section: The Anderson-callen Decoupling Frameworkmentioning
confidence: 99%
See 1 more Smart Citation
“…) where H 0 = J(0) + 17 18 I(0) − 2 3 D. Then, to order of interest for H → 0 we have the required critical line equation…”
Section: The Anderson-callen Decoupling Frameworkmentioning
confidence: 99%
“…In particular, it has received recently a great attention for understanding the thermodynamic properties of advanced magnetic materials with general non-collinear magnetic structures as the helimagnetic thin films [7][8][9]. From these investigations, a very rich structure of the phase diagram emerges providing a remarkable tool for understanding the complex magnetic properties of several innovative materials [10][11][12][13][14][15], also involving quantum phase transitions (QPTs) [16][17][18]. The effect of the BQE interactions on the finite temperature phase transitions in systems with XY symmetry, also in presence of a SIA, has received less attention.…”
Section: Introductionmentioning
confidence: 99%
“…In the last decade there has been a renewed interest in investigating the role played by the interplay between quantum fluctuations, bilinear and biquadratic exchange interactions and crystal lattice geometry which is expected to result in a rich variety of quantum phases and exotic phenomena [1][2][3][4][5][6][7] especially when magnetic field induced quantum phase transitions (QPTs) [8][9][10][11] are present. In this context, the effect of competition between biquadratic exchange (BQE) and single-ion anisotropy (SIA) has been explored for quantum anisotropic magnetic models by using different approximate schemes (see, for instance, [12][13][14][15][16]).…”
Section: Introductionmentioning
confidence: 99%