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Magnetic field induced lattice ground states from holography
High Energy Physics - Theory · Submitted 24 Oct 2012
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We find a new ground state when a magnetic component of the gauge field is larger than a critical value.
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The abstract, sentence by sentence
We study the holographic field theory dual of a probe SU(2) Yang-Mills field in a background $(4+1)$-dimensional asymptotically Anti-de Sitter space. We find a new ground state when a magnetic component of the gauge field is larger than a critical value. The ground state forms a triangular Abrikosov lattice in the spatial directions perpendicular to the magnetic field. The lattice is composed of superconducting vortices induced by the condensation of a charged vector operator. We perform this calculation both at finite temperature and at zero temperature with a hard wall cutoff dual to a confining gauge theory. The study of this state may be of relevance to both holographic condensed matter models as well as to heavy ion physics. The results shown here provide support for the proposal that such a ground state may be found in the QCD vacuum when a large magnetic field is present.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study the holographic field theory dual of a probe SU(2) Yang-Mills field in a background $(4+1)$-dimensional asymptotically Anti-de Sitter space. | contribution 0.66 | 0.65 | 0.03 | asserted 0.88 |
| s1 | We find a new ground state when a magnetic component of the gauge field is larger than a critical value. | result 1.00 | 0.97 | 0.51 | asserted 1.00 |
| s2 | The ground state forms a triangular Abrikosov lattice in the spatial directions perpendicular to the magnetic field. | result 1.00 | 0.91 | 0.35 | asserted 1.00 |
| s3 | The lattice is composed of superconducting vortices induced by the condensation of a charged vector operator. | result 0.89 | 0.86 | 0.14 | asserted 1.00 |
| s4 | We perform this calculation both at finite temperature and at zero temperature with a hard wall cutoff dual to a confining gauge theory. | method 0.96 | 0.95 | 0.03 | asserted 1.00 |
| s5 | The study of this state may be of relevance to both holographic condensed matter models as well as to heavy ion physics. | interpretation 0.91 | 0.12 | 0.05 | hedged possibility 1.00 |
| s6 | The results shown here provide support for the proposal that such a ground state may be found in the QCD vacuum when a large magnetic field is present. | interpretation 1.00 | 0.33 | 0.41 | hedged possibility 0.98 |
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The paper
Original abstract
We study the holographic field theory dual of a probe SU(2) Yang-Mills field in a background $(4+1)$-dimensional asymptotically Anti-de Sitter space. We find a new ground state when a magnetic component of the gauge field is larger than a critical value. The ground state forms a triangular Abrikosov lattice in the spatial directions perpendicular to the magnetic field. The lattice is composed of superconducting vortices induced by the condensation of a charged vector operator. We perform this calculation both at finite temperature and at zero temperature with a hard wall cutoff dual to a confining gauge theory. The study of this state may be of relevance to both holographic condensed matter models as well as to heavy ion physics. The results shown here provide support for the proposal that such a ground state may be found in the QCD vacuum when a large magnetic field is present.
Human review
References
How the literature uses it
42 arXiv papers cite this in 65 sentences
Papers citing it · 37 sentences without a confident label
Builds on it 2 papers
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This works builds on the recent results of [ref] , and the older studies in [ref] .
Crystalline Scaling Geometries from Vortex Lattices · Introduction · 0.97
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Our work builds on the earlier papers [ref] , which found an elegant solution for a vortex lattice in the probe approximation, and [ref] , where the backreaction of such a lattice on bulk gauge fields was studied in a different setting.
Vortex Lattices and Crystalline Geometries · Introduction · 0.98
Uses its method or tool 1 paper
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We make the following ansatz [equation] Here, alternating of the powers of the expansion in $δχ$ and $δΛ$ is motivated by [ref] and in turn by the original paper [ref] .
Signals of a new phase in N=2 gauge theory with a magnetic field on the three-sphere · Investigating the gap · 0.80
Compares with it 2 papers
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This distinguishes our situation from that considered in e.g. [ref] .
Vortex Lattices and Crystalline Geometries · The vortex lattice · 0.99
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This distinguishes our situation from that considered in e.g. [ref] .
Crystalline Scaling Geometries from Vortex Lattices · Inclusion of “monopole" operator · 0.99
Cites it as background 21 papers
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A lot of work has gone into the difficult problem of finding the inhomogeneous end states of such instabilities [ref] .
Gravity dual of spin and charge density waves · Introduction · 0.83
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To date, the effect of rho meson condensation has been discussed in [ref] using phenomenological and lattice approaches, in our work [ref] using the Sakai-Sugimoto model, and in [ref] using a bottom-up holographic approach.
Background field and time dependence effects in holographic models · Rho meson condensation · 0.95
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The AdS/CFT correspondence emerged as an appropriate playground for strongly coupled condensed matter systems [ref] starting with the holographic superconductors and superfluids [ref] , the Kondo model [ref] , topological fractional insulators [ref] , and external electromagnetic sources [ref] .
Non-equilibrium dynamics in Holography · Zusammenfassung · 0.91
What it cites · 31 sentences without a confident label
Compares with 4 papers
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It is also the result found by Chernodub et al. in [ref] .
Electromagnetically superconducting phase of vacuum in strong magnetic field: structure of superconductor and superfluid vortex lattices in the ground state · Solving the equations to linear order · 0.95
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Whereas in [ref] , a Meissner effect is shown to occur by which a magnetic field reduces the transition temperature, here it is again the magnetic field which induces condensation at zero density.
Superconductivity from gauge/gravity duality with flavor · Introduction · 1.00
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Whereas in [ref] , a Meissner effect is shown to occur by which a magnetic field reduces the transition temperature, here it is again the magnetic field which induces condensation at zero density.
Flavor Superconductivity from Gauge/Gravity Duality · Introduction · 1.00
Cites as support 3 papers
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In addition to being interesting in the broader context of holographic lattices, the model we discuss serves as supporting evidence for a phenomenon first described by Chernodub et al. in [ref] .
Superconductivity of QCD vacuum in strong magnetic field · Introduction · 1.00
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In addition to being interesting in the broader context of holographic lattices, the model we discuss serves as supporting evidence for a phenomenon first described by Chernodub et al. in [ref] .
Electromagnetically superconducting phase of QCD vacuum induced by strong magnetic field · Introduction · 1.00
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Moreover, our holographic model provides support for recent QCD studies of $ρ$ meson condensation from a strong magnetic field [ref] .
Electromagnetically superconducting phase of vacuum in strong magnetic field: structure of superconductor and superfluid vortex lattices in the ground state · Introduction · 0.99
Cites as background 7 papers
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In [ref] a type II superconductor was modelled using a $(3+1)$-dimensional gravitational setup.
Vortex lattice for a holographic superconductor · Introduction · 0.95
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In [ref] the holographic dual of a self-gravitating Julia-Zee Dyon was constructed, and it was shown to contain a vortex condensate.
On Holography of Julia-Zee Dyon · Introduction · 0.92
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The former was first studied by Gauntlett et al. in [ref] and [ref] where the instability of the magnetically charged black hole in a top-down framework was studied in detail.
Holographic striped phases · Introduction · 0.87
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