2012
DOI: 10.1016/j.physletb.2012.07.026
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D3–D5 holography with flux

Abstract: It is shown that the Berezinski-Kosterlitz-Thouless phase transition that has been found in D3-D5 brane systems with nonzero magnetic field and charge density can also be found by tuning an extra-dimensional magnetic flux. We find numerical solutions for the probe D5-brane embedding and discuss properties of the solutions. We also demonstrate that the nontrivial embeddings include those which can be regarded as spontaneously breaking chiral symmetry.

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Cited by 14 publications
(17 citation statements)
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References 37 publications
(48 reference statements)
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“…If the boundary condition at infinity were different, so that the constant ψ = 0 everywhere were a solution, this solution would describe a D5-brane with flux in this geometry [42]. This is an interesting possibility, but not the one that we need here.…”
Section: Conformal Field Theorymentioning
confidence: 97%
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“…If the boundary condition at infinity were different, so that the constant ψ = 0 everywhere were a solution, this solution would describe a D5-brane with flux in this geometry [42]. This is an interesting possibility, but not the one that we need here.…”
Section: Conformal Field Theorymentioning
confidence: 97%
“…This phenomenon is called magnetic catalysis [9]- [17]. The interesting question as to whether it persists at strong coupling has been addressed in some holographic models where it has indeed been found to occur, particularly in holographic D3-D5 systems [18]- [42]. However, it has proven to be more elusive in the D3-D7 system [8] and there are even cases of "anti-catalysis", suppression of a chiral condensate by a magnetic field [30] [31].…”
Section: Introductionmentioning
confidence: 99%
“…Namely, we study the embedding equations obtained from the DBI action of the D5/D5-branes, and compare the free energies of the resulting configurations. This construction can potentially play a rôle in improving the understanding of dynamical symmetry breaking in graphene monolayers and bilayers, see e.g., [7,8] and references therein; the reader should also consult [9][10][11][12] for a recent related holographic model involving D7-branes, and a more detailed explanation of the relevance of holographic setups to learn some lessons about graphene bilayers.…”
Section: Jhep07(2014)043mentioning
confidence: 99%
“…The regularised free energy density of the U-shaped monolayer phase can be expressed as 12) while the regularised free energy density of the U-shaped bilayer phase is given by…”
Section: Zero Temperature and Zero Magnetic Fieldmentioning
confidence: 99%
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