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Flux-branes and the Dielectric Effect in String Theory
High Energy Physics - Theory · Submitted 2 May 2001
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim This provides a new setup to consider the gauge theory/gravity duality.
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The abstract, sentence by sentence
We consider the generalization to String and M-theory of the Melvin solution. These are flux p-branes which have (p+1)-dimensional Poincare invariance and are associated to an electric (p+1)-form field strength along their worldvolume. When a stack of Dp-branes is placed along the worldvolume of a flux (p+3)-brane it will expand to a spherical D(p+2)-brane due to the dielectric effect. This provides a new setup to consider the gauge theory/gravity duality. Compactifying M-theory on a circle we find the exact gravity solution of the type IIA theory describing the dielectric expansion of N D4-branes into a spherical bound state of D4-D6-branes, due to the presence of a flux 7-brane. In the decoupling limit, the deformation of the dual field theory associated with the presence of the flux brane is irrelevant in the UV. We calculate the gravitational radius and energy of the dielectric brane which give, respectively, a prediction for the VEV of scalars and vacuum energy of the dual field theory. Consideration of a spherical D6-brane probe with n units of D4-brane charge in the dielectric brane geometry suggests that the dual theory arises as the Scherk-Schwarz reduction of the M5-branes (2,0) conformal field theory. The probe potential has one minimum placed at the locus of the bulk dielectric brane and another associated to an inner dielectric brane shell.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We consider the generalization to String and M-theory of the Melvin solution. | contribution 0.66 | 0.75 | 0.04 | asserted 0.59 |
| s1 | These are flux p-branes which have (p+1)-dimensional Poincare invariance and are associated to an electric (p+1)-form field strength along their worldvolume. | background 0.69 | 0.21 | 0.05 | asserted 1.00 |
| s2 | When a stack of Dp-branes is placed along the worldvolume of a flux (p+3)-brane it will expand to a spherical D(p+2)-brane due to the dielectric effect. | result 0.51 | 0.30 | 0.23 | asserted 1.00 |
| s3 | This provides a new setup to consider the gauge theory/gravity duality. | interpretation 0.95 | 0.30 | 0.15 | asserted 0.82 |
| s4 | Compactifying M-theory on a circle we find the exact gravity solution of the type IIA theory describing the dielectric expansion of N D4-branes into a spherical bound state of D4-D6-branes, due to the presence of a flux 7-brane. | result 0.80 | 0.92 | 0.22 | asserted 1.00 |
| s5 | In the decoupling limit, the deformation of the dual field theory associated with the presence of the flux brane is irrelevant in the UV. | result 0.80 | 0.62 | 0.10 | asserted 1.00 |
| s6 | We calculate the gravitational radius and energy of the dielectric brane which give, respectively, a prediction for the VEV of scalars and vacuum energy of the dual field theory. | contribution 0.46 | 0.95 | 0.18 | asserted 1.00 |
| s7 | Consideration of a spherical D6-brane probe with n units of D4-brane charge in the dielectric brane geometry suggests that the dual theory arises as the Scherk-Schwarz reduction of the M5-branes (2,0) conformal field theory. | interpretation 0.74 | 0.65 | 0.16 | hedged possibility 1.00 |
| s8 | The probe potential has one minimum placed at the locus of the bulk dielectric brane and another associated to an inner dielectric brane shell. | result 1.00 | 0.77 | 0.09 | asserted 0.97 |
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Original abstract
We consider the generalization to String and M-theory of the Melvin solution. These are flux p-branes which have (p+1)-dimensional Poincare invariance and are associated to an electric (p+1)-form field strength along their worldvolume. When a stack of Dp-branes is placed along the worldvolume of a flux (p+3)-brane it will expand to a spherical D(p+2)-brane due to the dielectric effect. This provides a new setup to consider the gauge theory/gravity duality. Compactifying M-theory on a circle we find the exact gravity solution of the type IIA theory describing the dielectric expansion of N D4-branes into a spherical bound state of D4-D6-branes, due to the presence of a flux 7-brane. In the decoupling limit, the deformation of the dual field theory associated with the presence of the flux brane is irrelevant in the UV. We calculate the gravitational radius and energy of the dielectric brane which give, respectively, a prediction for the VEV of scalars and vacuum energy of the dual field theory. Consideration of a spherical D6-brane probe with n units of D4-brane charge in the dielectric brane geometry suggests that the dual theory arises as the Scherk-Schwarz reduction of the M5-branes (2,0) conformal field theory. The probe potential has one minimum placed at the locus of the bulk dielectric brane and another associated to an inner dielectric brane shell.
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References
How the literature uses it
5 arXiv papers cite this in 6 sentences
Papers citing it · 1 sentence without a confident label
Cites it as background 4 papers
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It lends itself to many applications and generalizations ($e.g.$ [ref] ), including accommodating a Schwarzschild [ref] (or Reissner-Nordström [ref] or Kerr [ref] ) black hole (BH).
Black holes in scalar multipolar Universes · Introduction · 0.86
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Melvin twist applied to the $Dp$-brane background and the subsequent near horizon limit gives rise to supergravity duals for a variety of decoupled field theories[An earlier discussion of a construction of this type is [ref] .] depending on the orientation of the brane and the Melvin twist.
Melvin Twists of global AdS_5 \times S_5 and their Non-Commutative Field Theory Dual · Introduction · 0.82
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Melvin twist, also known as the T-s-T transformation, is a powerful solution generating technique in string and supergravity theories [ref] .
Microscopic Formulation of Puff Field Theory · Introduction · 0.93
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