Holography and phenomenology

By N. Arkani-Hamed, M. Porrati, L. Randall. 2000

531 citations recorded by the source corpus.

We examine various aspects of the conjectured duality between warped AdS5 geometries with boundary branes and strongly coupled (broken) conformal field theories coupled to dynamical gravity. We also examine compactifications with 5-d gauge fields, in which case the holographic dual is a broken CFT weakly coupled to dynamical gauge fields in addition to gravity. The holographic picture is used to clarify a number of important phenomenological issues in these and related models, including the questions of black hole production, radius stabilization, early universe cosmology, and gauge coupling unification.

Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics, Statistical and Nonlinear Physics

View Paper: https://www.semanticscholar.org/paper/dfb069262255141310d3e3807b6bcdeaa8af89f4

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Citations in the corpus

Lower bound on the propagation speed of gravity from gravitational Cherenkov radiation (2001, background): “The ADS/CFT correspondence [22] has given rise to a purely 4 dimensional interpretation, in the infrared, of warped higher dimensional geometry [23, 24, 25, 26 , 27, 18].”
Proton stability in grand unified theories, in strings and in branes (2006, methodology): “Thus RS models where most or all of the Standard Model fields are in the RS bulk may have a dual to a purely 4D composite Higgs scenario via a AdS/CFT correspondence [299,300].”
Discovering the top partners at the LHC using same-sign dilepton final states (2008, background): “As suggested by the theoretical developments on the connection between gravity in higher-dimensional curved spacetimes and strongly-coupled gauge theories [8, 9], the strong dynamics that generates the light Higgs could be realized by the”
Gravitational waves from warped spacetime (2006, background): “With nonzero δT1 < 0 there is also the desired minimum at μ ∼ μ0(v0/v1)(1 − √ δT1/2v1) 1/|ǫ| and a viable solution can be obtained for v0 < v1 [16, 17].”
The Bulk RS KK-gluon at the LHC (2007, background): “The fact that this coupling is not exponentially suppressed [2] can be understood in the CFT picture as the result of kinetic mixing between the SM gauge field and the composite vector states (KK-gauge bosons in the AdS) [11].”
Light-front holographic QCD and emerging confinement (2014, methodology): “so we obtain an analytic solution for the polarization ΠV [335, 330, 70], ΠV (q (2)) = − (J0(qzm)Y0(qǫ)− Y0(qzm)J0(qǫ)) 2g(2) 5 J0(qzm) .”
A Warped supersymmetric standard model (2000, methodology): “Since the gaugino mass comes from the mixing between the gaugino and the CFT bound-state, the mass will be proportional to √ g(2)bCFT/(8π(2)) = 1/ √ πkR, where we have used the AdS/CFT relation [13] g(2) 5k = 8π (2)/bCFT and g 2 = g(2) 5/(πR).”
Open and closed string interpretation of SUSY CFT's on branes with boundaries (2001, unknown): “July 2000 karch@mit.edu,randall@mit.edu”
Interpolating between low and high energy QCD via a 5D Yang-Mills model (2005, background): “ory: exact locality in the extra dimension. This implies an even softer high-energy behavior [23]. An independent motivation to consider a 5D model with YM ﬁelds comes from the AdS/CFT correspondence [24, 25, 26, 27]. This correspondence established an equivalence between two very precise theories, ”