Meson Spectroscopy in AdS/CFT with Flavour
By M. Kruczenski, D. Mateos, R. Myers, D. Winters. 2003
544 citations recorded by the source corpus.
We compute the meson spectrum of an = 2 super Yang-Mills theory with fundamental matter from its dual string theory on AdS5 × S5 with a D7-brane probe [1]. For scalar and vector mesons with arbitrary R-charge the spectrum is computed in closed form by solving the equations for D7-brane fluctuations; for matter with non-zero mass mq it is discrete, exhibits a mass gap of order mq/(gsN)1/2 and furnishes representations of SO(5) even though the manifest global symmetry of the theory is only SO(4). The spectrum of mesons with large spin J is obtained from semiclassical, rotating open strings attached to the D7-brane. It displays Regge-like behaviour for J > (gsN)1/2 it corresponds to that of two non-relativistic quarks bound by a Coulomb potential. Meson interactions, baryons and `giant gauge bosons' are briefly discussed.
Subfields: Atomic and Molecular Physics, and Optics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/b48c877e36bbbf1147f9307c119d510e76f65c12
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Citations in the corpus
- Superconductivity from gauge/gravity duality with flavor (2008, methodology): “Flavor degrees are added by embedding Nf coincident probe D7 branes with Nf ≪ Nc into the AdS black hole background [10, 11, 12].”
- Holographic spectral functions and diffusion constants for fundamental matter (2007, methodology): “, corresponding to the meson spectrum found in [11].”
- Energy loss of a heavy quark moving through Script N = 4 supersymmetric Yang-Mills plasma (2006, background): “The static potential between a heavy quark and antiquark in N = 4 SYM rises linearly at short distance before switching to a Coulombic form at a cross-over distance set by the inverse quark mass [39].”
- Metallic AdS/CFT (2007, background): “The only way for SD7 to remain real all the way from z = zH to z = 0, then, is if both numerator and denominator change sign at the same special value3 z = z∗ defined by the equations |gtt|gxx − (2πα′)2E2 = 0 (3.1) |gtt|g3xx cos6 θ(z∗) + |gtt|D2 − gxxB2 N 2(2πα′)2 = 0 (3.2) where all metric…”
- Probing flavored mesons of confining gauge theories by supergravity (2003, methodology): “The first goal was in fact proposed but not explicitly proven in [5] and as for the second goal recall that the computation in [7] involves N = 2 SQCD which is not a confining gauge theory.”
- Mesons in gauge/gravity duals (2007, methodology): “It is possible to extract the bound state masses [17].”
- Holographic meson melting (2006, background): “The spectrum is discrete with a mass gap M ∼ mq/ √ λ and grows linearly [9,21].”
- Chiral symmetry breaking and pions in nonsupersymmetric gauge / gravity duals (2004, methodology): “This was solved exactly in [ 31 ], where it was shown that the solutions can be written as hyper-”
- Thermodynamics of the brane (2007, methodology): “In the last equality, we are relating M̄ to the meson mass gap in the D3/D7 theory at zero temperature [9].”
- Flavor superconductivity from gauge/gravity duality (2009, methodology): “The grey lines correspond to the supersymmetric mass spectrum calculated in [24].”