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Holographic Multi-Band Superconductor
High Energy Physics - Theory · Submitted 4 Feb 2011
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We study the phase diagram of our model, and find it qualitatively agrees with the one for the realistic 2-band superconductor, such as $MgB_2$.
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The abstract, sentence by sentence
We propose a gravity dual for the holographic superconductor with multi-band carriers. Moreover, the currents of these carriers are unified under a global flavored SO(3) symmetry, which is dual to the bulk SO(3) gauge symmetry. We study the phase diagram of our model, and find it qualitatively agrees with the one for the realistic 2-band superconductor, such as $MgB_2$. We also identify the bulk field dual to the electromagnetic $U(1)_{EM}$ current, which should be invariant under the global flavored SO(3) rotation. We then evaluate the corresponding holographic conductivity and find the expected mean field like behaviors.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We propose a gravity dual for the holographic superconductor with multi-band carriers. | contribution 0.99 | 0.89 | 0.19 | asserted 0.75 |
| s1 | Moreover, the currents of these carriers are unified under a global flavored SO(3) symmetry, which is dual to the bulk SO(3) gauge symmetry. | contribution 0.70 | 0.55 | 0.11 | asserted 1.00 |
| s2 | We study the phase diagram of our model, and find it qualitatively agrees with the one for the realistic 2-band superconductor, such as $MgB_2$. | result 0.98 | 0.96 | 0.30 | asserted 0.97 |
| s3 | We also identify the bulk field dual to the electromagnetic $U(1)_{EM}$ current, which should be invariant under the global flavored SO(3) rotation. | contribution 0.70 | 0.87 | 0.07 | asserted 0.71 |
| s4 | We then evaluate the corresponding holographic conductivity and find the expected mean field like behaviors. | result 1.00 | 0.96 | 0.24 | asserted 1.00 |
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The paper
Original abstract
We propose a gravity dual for the holographic superconductor with multi-band carriers. Moreover, the currents of these carriers are unified under a global flavored SO(3) symmetry, which is dual to the bulk SO(3) gauge symmetry. We study the phase diagram of our model, and find it qualitatively agrees with the one for the realistic 2-band superconductor, such as $MgB_2$. We also identify the bulk field dual to the electromagnetic $U(1)_{EM}$ current, which should be invariant under the global flavored SO(3) rotation. We then evaluate the corresponding holographic conductivity and find the expected mean field like behaviors.
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References
How the literature uses it
17 arXiv papers cite this in 19 sentences
Papers citing it · 7 sentences without a confident label
Uses its method or tool 1 paper
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In our present study we will also use the approach similar to [ref] where the multiband superconductor was considered, although our construction is different from that used in [ref] providing us with the possibility to treat the phases of condensates and electric current straightforwardly.
Holographic model of the S^{+/-} multiband superconductor · Introduction · 0.80
Cites it as background 11 papers
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[ref] studied a multi-band superconductor model, while regarding two bulk scalar fields as the fundamental representation of U(2) group, the authors of ref.
Competition and Coexistence of Order Parameters in Holographic Multi-Band Superconductors · Introduction · 0.92
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The application of AdS/CFT techniques to strongly correlated systems in condensed matter situations is a very promising development [ref] .
Strong Coupling BCS Superconductivity and Holography · Introduction · 0.97
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To describe them, holographic models with two or more fields corresponding to the order parameters were studied [ref] .
Phase Diagram of a Holographic Superconductor Model with s-wave and d-wave · Introduction · 0.81
What it cites · 4 sentences without a confident label
Uses the method or tool of 3 papers
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Then from the asymptotic behavior of all the fields at the asymptotic boundary we found a_j(r,k⃗,ω)=a_j^(0)(k⃗,ω)+a_j^(1)r (k⃗,ω)+⋯, It then seems that one can evaluate the holographic conductivity by the standard holographic prescription for the Ohmic law [ref] .
Ohm's Law at strong coupling: S duality and the cyclotron resonance · Holographic Conductivity · 0.98
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Then from the asymptotic behavior of all the fields at the asymptotic boundary we found a_j(r,k⃗,ω)=a_j^(0)(k⃗,ω)+a_j^(1)r (k⃗,ω)+⋯, It then seems that one can evaluate the holographic conductivity by the standard holographic prescription for the Ohmic law [ref] .
Universality of the hydrodynamic limit in AdS/CFT and the membrane paradigm · Holographic Conductivity · 0.98
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Then from the asymptotic behavior of all the fields at the asymptotic boundary we found a_j(r,k⃗,ω)=a_j^(0)(k⃗,ω)+a_j^(1)r (k⃗,ω)+⋯, It then seems that one can evaluate the holographic conductivity by the standard holographic prescription for the Ohmic law [ref] .
Real-time response in AdS/CFT with application to spinors · Holographic Conductivity · 0.98
Compares with 2 papers
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The numerical fitting gives $C∼14$, $D≃24$ and $γ≃0.97$ for the 3-band case, this is the typical mean-field like behavior as for the holographic s-wave superconductor [ref] .
Building an AdS/CFT superconductor · Holographic Conductivity · 0.91
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At this point we would like to remind the readers that our model is different from holographic p-wave superconductors considered in [ref] , where only the non-Abelian gauge fields are introduced, not the fundamental scalars.
The gravity dual of a p-wave superconductor · Introduction · 0.97
Cites as background 3 papers
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Similarly, in the recent proposal of holographic superconductor [ref] , the global U(1) symmetry for the charge conservation is again dual to a U(1) gauge symmetry in the bulk gravity.
Building an AdS/CFT superconductor · Introduction · 0.81
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Similarly, in the recent proposal of holographic superconductor [ref] , the global U(1) symmetry for the charge conservation is again dual to a U(1) gauge symmetry in the bulk gravity.
Holographic Superconductors · Introduction · 0.81
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For example, in the study of meson dynamics of the holographic QCD, the flavor symmetry of QCD is dual to the gauge symmetry on the probe mesonic branes [ref] .
Low energy hadron physics in holographic QCD · Introduction · 0.87
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