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Non-Fermi liquid at the FFLO quantum critical point

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Pimenov,  Dimitri
IMPRS (International Max Planck Research School), Max Planck Institute of Quantum Optics, Max Planck Society;

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Mandal,  Ipsita
Max Planck Institute for the Physics of Complex Systems, Max Planck Society;

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Piazza,  Francesco
Max Planck Institute for the Physics of Complex Systems, Max Planck Society;

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1711.10514.pdf
(プレプリント), 964KB

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引用

Pimenov, D., Mandal, I., Piazza, F., & Punk, M. (2018). Non-Fermi liquid at the FFLO quantum critical point. Physical Review B, 98(2):. doi:10.1103/PhysRevB.98.024510.


引用: https://hdl.handle.net/21.11116/0000-0004-CC19-B
要旨
When a 2D superconductor is subjected to a strong in-plane magnetic field, Zeeman polarization of the Fermi surface can give rise to inhomogeneous FFLO order with a spatially modulated gap. Further increase of the magnetic field eventually drives the system into a normal metal state. Here, we perform a renormalization group analysis of this quantum phase transition, starting from an appropriate low-energy theory recently introduced in phys. Rev. B 93, 085112 (2016). We compute one-loop flow equations within the controlled dimensional regularization scheme with fixed dimension of Fermi surface, expanding in epsilon = 5/2 - d. We find a new stable non-Fermi-liquid fixed point and discuss its critical properties. One of the most interesting aspects of the FFLO non-Fermi-liquid scenario is that the quantum critical point is potentially naked, with the scaling regime observable down to arbitrary low temperatures. In order to study this possibility, we perform a general analysis of competing instabilities, which suggests that only charge density wave order is enhanced in the vicinity of the quantum critical point.