Remarks on the Warped Deformed Conifold
By Christopher P. Herzog, I. Klebanov, P. Ouyang. 2001
179 citations recorded by the source corpus.
We assemble a few remarks on the supergravity solution of hep-th/0007191, whose UV asymptotic form was previously found in hep-th/0002159. First, by normalizing the R-R fluxes, we compare the logarithmic flow of couplings in supergravity with that in field theory, and find exact agreement. We also write the 3-form field strength $G_3 = F_3 - \tau H_3$ present in the solution in a manifestly SO(4) invariant (2,1) form. In addition, we discuss various issues related to the chiral symmetry breaking and wrapped branes.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/e4cd839be10b131222b9c5187f05bbb69f087e89
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In Astronomy and Astrophysics
- Liam McAllister
- Eran Palti
- S. Gubser
- D. Baumann
- I. Klebanov
- Frederik Denef
- S. Hartnoll
- J. Polchinski
In Nuclear and High Energy Physics
- Liam McAllister
- Eran Palti
- I. Klebanov
- D. Baumann
- S. Gubser
- Frederik Denef
- E. Silverstein
- Anatoly Dymarsky
Citations in the corpus
- The Swampland: Introduction and Review (2019, background): “Locally, near the tip, the metric takes the form [525,526]”
- Brane/Flux Annihilation and the String Dual of a Non-Supersymmetric Field Theory (2001, unknown): “The metric near the apex reads [12] (we work in string units, α = 1) ds(2) = a(2)0 dxμdxμ + gsM b 2 0 1 2 dr(2) + dΩ(2)3 + r (2)dΩ̃(2)2 )”
- Symmetry breaking and axionic strings in the warped deformed conifold (2004, background): “Keywords: Spontaneous Symmetry Breaking, D-branes, AdS-CFT and dS-CFT Correspondence, Supergravity Models. c© SISSA/ISAS 2004 http://jhep.sissa.it/archive/papers/jhep092004036/jhep092004036.pdf J H E P 0 9 ( 2 0 0 4 ) 0 3 6 Contents”
- On Penrose limits and gauge Theories (2002, unknown): “For the precise normalizations we refer the reader to [17].”
- Entanglement as a probe of confinement (2007, background): “For the details of the angular forms gi, see [11, 16].”
- Cosmic F- and D-strings (2003, background): “[30], one obtains for (p, q) → (p−M, q) with p > M/2 a decay rate of order”
- Dynamics of warped compactifications and the shape of the warped landscape (2005, background): “In particular, as has been found in explicit studies of conifold geometry[54,55], the (2,1) form corresponding to the conifold modulus”
- Meson spectroscopy from holomorphic probes on the warped deformed conifold (2004, background): “parameter. In the rest of this section we will examine these conditions for the deformed conifold case. To this end we will need the expression for the B-field in terms of the complex coordinates zi’s [55]: B= b(τ)ǫijklziz¯jdzk∧d¯zl with b(τ) = igsMα′ 2ǫ4 τcothτ−1 sinh2τ . (3.7) This expression is ex”
- D3-brane potentials from fluxes in AdS/CFT (2010, background): “We therefore begin by briefly setting our notation for the conifold (more details may be found in [36, 16]).”
- Kinetic Mixing of the Photon with Hidden U(1)s in String Phenomenology (2008, methodology): “We now turn to an example of a Calabi-Yau manifold for which the metric is known, the Klebanov-Tseytlin throat [83, 84].”