Brane/Flux Annihilation and the String Dual of a Non-Supersymmetric Field Theory
By S. Kachru, J. Pearson, H. Verlinde. 2001
478 citations recorded by the source corpus.
We consider the dynamics of p anti-D3 branes inside the Klebanov-Strassler geometry, the deformed conifold with M units of RR 3-form flux around the S3. We find that for p << M the system relaxes to a nonsupersymmetric NS 5-brane `giant graviton' configuration, which is classically stable, but quantum mechanically can tunnel to a nearby supersymmetric vacuum with M−p D3 branes. This decay mode is exponentially suppressed and proceeds via the nucleation of an NS 5-brane bubble wall. We propose a dual field theory interpretation of the decay as the transition between a nonsupersymmetric `baryonic' branch and a supersymmetric `mesonic' branch of the corresponding SU(2M−p) × SU(M−p) low energy gauge theory. The NS 5-brane tunneling process also provides a simple visualization of the geometric transition by which D3-branes can dissolve into 3-form flux.
Subfields: Atomic and Molecular Physics, and Optics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/6389b1ce57e6efcbb59fff5c85fb23e9ec96a2af
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In Atomic and Molecular Physics, and Optics
- Eran Palti
- E. Silverstein
- Phil Saad
- Anshuman Maharana
- Frederik Denef
- M. Graña
- Liam McAllister
- S. Trivedi
In Nuclear and High Energy Physics
- Eran Palti
- Liam McAllister
- D. Baumann
- R. Kallosh
- Andrei Linde
- Frederik Denef
- E. Silverstein
- F. Quevedo
Citations in the corpus
- The Scaling of the No Scale Potential and de Sitter Model Building (2004, methodology): “One ingredient of the model [2] is an anti-D3-brane in a warped 3-brane throat of a Calabi-Yau compactification of type IIB string theory [9].”
- The Swampland: Introduction and Review (2019, background): “Locally, near the tip, the metric takes the form [525,526]”
- De Sitter Space In Non-Critical String Theory (2002, unknown): “In addition to the instanton decays to the linear dilaton regime discussed above, there is also the possibility of transitions among the different flux vacua, as in [20][13][16][41].”
- Retrofitting O'Raifeartaigh models with dynamical scales (2006, methodology): “worth remarking that the models need not be chiral and can have non-vanishing Witten index, like the models of [ 19 ,20].”
- Inflation from warped space (2005, background): “The fluxantibrane annihilation process in such a throat proceeds through quantum tunneling [39,22].”
- On the moduli space of the cascading SU(M+p) ? SU(p) gauge theory (2005, background): “In the supergravity dual this domain wall is an NS5-brane wrapped over the 3-sphere [28].”
- Enumerating flux vacua with enhanced symmetries (2004, background): “Inclusion of Kähler Moduli In general, Kähler moduli are also present in these systems, and they do not acquire a potential from the flux superpotential (2.4).”
- Racetrack Inflation (2004, background): “The introduction of the anti-brane does not introduce extra translational moduli because its position is fixed by the fluxes [41], so it just contributes to the energy density of the system.”
- Moduli stabilization from fluxes in a simple IIB orientifold (2002, background): “Inclusion of anti-branes in the flux background might also lead to interesting phenomena, as in [19].”
- de Sitter string vacua from dilaton-dependent non-perturbative effects (2012, background): “The configuration is metastable with the possibility of decay involving brane flux annihilation [15].”
- Inflating in a Better Racetrack (2006, background): “The presence of these branes does not introduce extra translational moduli since their positions are fixed by the fluxes [25], and so their low-energy effect is just a contribution to the energy density of the system.”