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Vortex Solution in Holographic Two-Band Superconductor
-- A model of holographic type 1.5 superconductor ? ? Hai-Qing Zhang Institute for Theoretical Physics, Utrecht University KITPC, Beijing 13/07/2015 Cooperators: Jackson M.-S. Wu, Shang-Yu Wu, in progress
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What is type 1.5 superconductor?
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Type I Meissner Normal Type II Vortex Type 1.5 Semi-Meissner H
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M- Magnetization H- External Magnetic Field
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Features Long-range attractive , short-range repulsive
Semi-Meissner: mixtures of Meissner and vortex Non-axialsymmetric vortex Vortex clusters
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* Two component Ginzburg-Landau (TCGL) free-energy functional
Then, they can get , type 1.5 E. Babaev and M.Speight, PRB 72, (2005) J. Carlstrom, E. Babaev, M. Speight, PRL105, (2010); PRB, 83, (2011)
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* Numerical Simulation
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Holographic setup
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* Action of the two-band superconductor
* 4-d AdS-Schwarzchild black hole Note that we are considering one single vortex solution
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* Boundary condition (B.C.) near z ~ 0
* Ansatz for vortex * Boundary condition (B.C.) near z ~ 0 velocity current
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* B.C. at vortex border ρ=R
* B.C. near horizon At=0, regular b.c. for other fields * B.C. at vortex core ρ=0 … … * B.C. at vortex border ρ=R Homogenerous b.c. for At and φi
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In order to avoid the divergence of the energy with fractional multiple
quantum flux Other numerical parameters:
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Numerical Results Holography CMT M.E.Zhitomirsky, V.H. Dao,
PRB 69, (2004)
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Free Energy * On-shell action * Counter term
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* Regularized free energy
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* Critical magnetic field Bc1
* For n=1
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Parameter Regimes for Type 1.5 SC
* Superconducting density
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* Magnetic penetration depth
* Coherence length
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* For ε=0.05, η=0, B=0.0125 In order that We find e=5q
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Further directions
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To estimate Bc2 1. From the M-B plots II. From the formula
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The effects of η
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Dependent of temperature
Vortex clusters (dependent of time)
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Thanks for your attention!
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