Quantum phase transitions in holographic models of magnetism and superconductors
By N. Iqbal, Hong Liu, M. Mezei, Qimiao Si. 2010
177 citations recorded by the source corpus.
We study a holographic model realizing an "antiferromagnetic" phase in which a global SU(2) symmetry representing spin is broken down to a U(1) by the presence of a finite electric charge density. This involves the condensation of a neutral scalar field in a charged anti-de Sitter black hole. We observe that the phase transition for both neutral and charged (as in the standard holographic superconductor) order parameters can be driven to zero temperature by a tuning of the UV conformal dimension of the order parameter, resulting in a quantum phase transition of the Berezinskii-Kosterlitz-Thouless-type. We also characterize the antiferromagnetic phase and an externally forced ferromagnetic phase by showing that they contain the expected spin waves with linear and quadratic dispersions, respectively.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics, Statistical and Nonlinear Physics
View Paper: https://www.semanticscholar.org/paper/c945c8e9188d8fda575eb475af8d94bfbca5c899
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Citations in the corpus
- Holographic Quantum Matter (2016, methodology): “In [416] the zero temperature destruction of holographic superconductivity by a magnetic field was shown to be in this class.”
- Introduction to holographic superconductor models (2015, unknown): “[127, 147].”
- Semi-local quantum liquids (2011, methodology): “We do point out that various holographic constructions do provide us with such a knob [8, 52, 53], often related to an applied magnetic field.”
- Integrating out geometry: holographic Wilsonian RG and the membrane paradigm (2010, background): “, [25, 47]), order parameters close to a phase transition [48].”
- Lectures on holographic non-Fermi liquids and quantum phase transitions (2011, background): “For the first type of instability a quantum critical point occurs when we violate the Breitenlohner-Freedman bound of the AdS2 region at k = 0 [45, 139], i.”
- Analytic holographic superconductor (2010, background): “[17, 18] where the authors make similar statements about the exponents in the mean field case.”