Critical temperature and Ginzburg region near a quantum critical point in two-dimensional metals
arXiv:1105.0924 · doi:10.1103/PhysRevB.84.075122
Abstract
We compute the transition temperature and the Ginzburg temperature above near a quantum critical point at the boundary of an ordered phase with a broken discrete symmetry in a two-dimensional metallic electron system. Our calculation is based on a renormalization group analysis of the Hertz action with a scalar order parameter. We provide analytic expressions for and as a function of the non-thermal control parameter for the quantum phase transition, including logarithmic corrections. The Ginzburg regime between and occupies a sizable part of the phase diagram.
5 pages, 1 figure
References in corpus (5)
- Exact evolution equation for the effective potential
- Fermi-liquid instabilities at magnetic quantum phase transitions
- Quantum phase transitions of metals in two spatial dimensions: II. Spin density wave order
- Renormalization group for phases with broken discrete symmetry near quantum critical points
- Electronic self-energy and triplet pairing fluctuations in the vicinity of a ferromagnetic instability in 2D systems: the quasistatic approach
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