Two-point Functions in a Holographic Kondo Model
Dec 6, 2016
65 pages
Published in:
- JHEP 03 (2017) 039
- Published: Mar 7, 2017
e-Print:
- 1612.02005 [hep-th]
Report number:
- OUTP-16-27P,
- SISSA-61-2016-FISI,
- FPAUO-16-16
View in:
Citations per year
Abstract: (Springer)
We develop the formalism of holographic renormalization to compute two-point functions in a holographic Kondo model. The model describes a (0 + 1)-dimensional impurity spin of a gauged SU(N ) interacting with a (1 + 1)-dimensional, large-N , strongly-coupled Conformal Field Theory (CFT). We describe the impurity using Abrikosov pseudo-fermions, and define an SU(N )-invariant scalar operator built from a pseudo-fermion and a CFT fermion. At large N the Kondo interaction is of the form , which is marginally relevant, and generates a Renormalization Group (RG) flow at the impurity. A second-order mean-field phase transition occurs in which condenses below a critical temperature, leading to the Kondo effect, including screening of the impurity. Via holography, the phase transition is dual to holographic superconductivity in (1 + 1)-dimensional Anti-de Sitter space. At all temperatures, spectral functions of exhibit a Fano resonance, characteristic of a continuum of states interacting with an isolated resonance. In contrast to Fano resonances observed for example in quantum dots, our continuum and resonance arise from a (0 + 1)-dimensional UV fixed point and RG flow, respectively. In the low-temperature phase, the resonance comes from a pole in the Green’s function of the form −i〈 〉, which is characteristic of a Kondo resonance.Note:
- 65 pages, 17 figures; v2 minor improvements. Version published in JHEP
- Holography and condensed matter physics (AdS/CMT)
- AdS-CFT Correspondence
- Gauge-gravity correspondence
- field theory: conformal
- superconductivity: holography
- renormalization group: flow
- critical phenomena
- two-point function
- Kondo model
- SU(N)
References(100)
Figures(17)
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