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A large mass hierarchy from a small extra dimension (1999)

by L Randall, R Sundrum
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Hierarchies from Fluxes in String Compactifications

by Steven B. Giddings, Shamit Kachru, Joseph Polchinski , 2002
"... Warped compactifications with significant warping provide one of the few known mechanisms for naturally generating large hierarchies of physical scales. We demonstrate that this mechanism is realizable in string theory, and give examples involving orientifold compactifications of IIB string theory a ..."
Abstract - Cited by 715 (33 self) - Add to MetaCart
Warped compactifications with significant warping provide one of the few known mechanisms for naturally generating large hierarchies of physical scales. We demonstrate that this mechanism is realizable in string theory, and give examples involving orientifold compactifications of IIB string theory and F-theory compactifications on Calabi-Yau four-folds. In each case, the hierarchy of scales is fixed by a choice of RR and NS fluxes in the compact manifold. Our solutions involve compactifications of the Klebanov-Strassler gravity dual to a confining N = 1 supersymmetric gauge theory, and the hierarchy reflects the small scale of chiral symmetry breaking in the dual gauge theory.

The Confrontation between General Relativity and Experiment

by Clifford M. Will - Living Rev. Relativity 9
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Abstract - Cited by 214 (1 self) - Add to MetaCart
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...d to suggest the possibility that the inverse-square law could be violated at very short ranges, below the centimeter range of existing laboratory verifications of the 1/r2 behavior. One set of ideas =-=[16, 18, 304, 303]-=- posited that some of the extra spatial dimensions that come with string theory could extend over macroscopic scales, rather than being rolled up at the Planck scale of 10−33 cm, which was then the co...

An alternative to compactification

by Lisa Randall - Phy. Rev. Lett , 1999
"... Conventional wisdom states that Newton’s force law implies only four non-compact dimensions. We demonstrate that this is not necessarily true in the presence of a non-factorizable background geometry. The specific example we study is a single 3-brane embedded in five dimensions. We show that even wi ..."
Abstract - Cited by 186 (1 self) - Add to MetaCart
Conventional wisdom states that Newton’s force law implies only four non-compact dimensions. We demonstrate that this is not necessarily true in the presence of a non-factorizable background geometry. The specific example we study is a single 3-brane embedded in five dimensions. We show that even without a gap in the Kaluza-Klein spectrum, four-dimensional There exists “lore ” that convinces us that we live in four non-compact dimensions. Certainly Standard Model matter cannot propagate a large distance in extra dimensions without conflict with observations. As has recently been emphasized, this can be avoided if the Standard Model is confined to a (3 + 1)-dimensional subspace, or “3-brane”, in the higher dimensions
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...ic, GMN, and Λ and Vbrane are cosmological terms in the bulk and boundary respectively. The coupling to the branes and their fields and the related orbifold boundary conditions are described in Refs. =-=[8]-=-(see also [4]). (The new coordinate y is rcφ in the coordinates of Ref. [8].) The solution to Einstein’s equations was derived in Ref. [8] and is ds 2 = e −2k|y| ηµνdx µ dx ν + dy 2 , (4) where 0 ≤ y ...

Brane/Flux Annihilation and the String Dual of a Non-Supersymmetric Field Theory

by Shamit Kachru, John Pearson, Herman Verlinde , 2006
"... 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 S 3. We find that for p << M the system relaxes to a nonsupersymmetric NS 5-brane “giant graviton ” configuration, which is classically stable, b ..."
Abstract - Cited by 170 (18 self) - Add to MetaCart
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 S 3. We find that for p &lt;&lt; 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 The search for calculable and nontrivial nonsupersymmetric string vacua remains a problem of basic interest in string theory. In the context of AdS/CFT duality [1], this is related to the construction of gravitational “anti-holographic” descriptions for nonsupersymmetric 4d quantum gauge theories. Here, we describe the construction of a simple nonsupersymmetric
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...ersymmetric SU(M) Yang-Mills theory. The KS model can be embedded into a compact geometry [5] and used to realize warping as a means of generating large hierarchies as in the Randall-Sundrum scenario =-=[6]-=- along the lines advocated in [7] (for other discussions along these lines, see e.g. [8]). Roughly speaking, the pure Yang-Mills theory becomes the theory on the “infrared brane” in the RS description...

Scalar speed limits and cosmology: Acceleration from D- cceleration

by Eva Silverstein, David Tong - Phys. Rev. D70 (2004) 103505, hep-th/0310221
"... Causality on the gravity side of the AdS/CFT correspondence restricts motion on the moduli space of the N = 4 super Yang Mills theory by imposing a speed limit on how fast the scalar field may roll. This effect can be traced to higher derivative operators arising from integrating out light degrees o ..."
Abstract - Cited by 166 (11 self) - Add to MetaCart
Causality on the gravity side of the AdS/CFT correspondence restricts motion on the moduli space of the N = 4 super Yang Mills theory by imposing a speed limit on how fast the scalar field may roll. This effect can be traced to higher derivative operators arising from integrating out light degrees of freedom near the origin. In the strong coupling limit of the theory, the dynamics is well approximated by the Dirac-Born-Infeld Lagrangian for a probe D3-brane moving toward the horizon of the AdS Poincare patch, combined with an estimate of the (ultimately suppressed) rate of particle and string production in the system. We analyze the motion of a rolling scalar field explicitly in the strong coupling regime of the field theory, and extend the analysis to cosmological systems obtained by coupling this type of field theory to four dimensional gravity. This leads to a mechanism for slow roll inflation for a massive scalar at subPlanckian VEV without need for a flat potential (realizing a version of k-inflation in a microphysical framework). It also leads to a variety of novel FRW cosmologies, some of which
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...φ on the Coulomb branch translates into r/α ′ in the gravity variables. We further have the relations R = (gsN) 1/4√α ′ and g2 Y M = 4πgs. As in other applications of AdS/CFT [20] and Randall-Sundrum =-=[21]-=-, the warp factor in (2.5) plays an important role in understanding the energy spectrum of the system. The string mass scale at position r is related to that at position r ′ by the ratio of warp facto...

Moduli Stabilization from Fluxes in a Simple IIB Orientifold

by Shamit Kachru , Michael Schulz , Sandip P. Trivedi , 2002
"... We study novel type IIB compactifications on the T 6 /Z2 orientifold. This geometry arises in the T-dual description of Type I theory on T 6, and one normally introduces 16 space-filling D3-branes to cancel the RR tadpoles. Here, we cancel the RR tadpoles either partially or fully by turning on thre ..."
Abstract - Cited by 149 (10 self) - Add to MetaCart
We study novel type IIB compactifications on the T 6 /Z2 orientifold. This geometry arises in the T-dual description of Type I theory on T 6, and one normally introduces 16 space-filling D3-branes to cancel the RR tadpoles. Here, we cancel the RR tadpoles either partially or fully by turning on three-form flux in the compact geometry. The resulting (super)potential for moduli is calculable. We demonstrate that one can find many examples of N = 1 supersymmetric vacua with greatly reduced numbers of moduli in this system. A few examples with N&gt; 1 supersymmetry or complete supersymmetry breaking are also discussed.
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...n, for example, [8]). Compactications withsuxes have also been proposed as a natural setting for warped solutions to the hierarchy problem [9], along the lines of the proposal of Randall and Sundrum =-=[10]-=-. The combination ofsuxes and spaceslling D-branes which often need to be introduced for tadpole cancellation in these models leads to a nontrivial warped metric, with the scale of 4d Minkowski space ...

The holographic principle

by Raphael Bousso - Rev. Mod. Phys , 2002
"... There is strong evidence that the area of any surface limits the information content of adjacent spacetime regions, at 1.4 ×10 69 bits per square meter. We review the developments that have led to the recognition of this entropy bound, placing special emphasis on the quantum properties of black hole ..."
Abstract - Cited by 132 (9 self) - Add to MetaCart
There is strong evidence that the area of any surface limits the information content of adjacent spacetime regions, at 1.4 ×10 69 bits per square meter. We review the developments that have led to the recognition of this entropy bound, placing special emphasis on the quantum properties of black holes. The construction of light-sheets, which associate relevant spacetime regions to any
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...e in AdS. In recent years there has been great interest in models of our universe in which four-dimensional gauge fields are holographic duals to the physics of an extra spatial dimension (see, e.g., =-=Randall and Sundrum, 1999-=-a,b)—a kind of “inverse holography”. Such models can be realized by introducing codimension one objects, branes, into a five-dimensional bulk spacetime. If the bulk is Anti-de Sitter space, the hologr...

Large-volume flux compactifications: Moduli spectrum and D3/D7 soft supersymmetry breaking

by Joseph P. Conlon, Fernando Quevedo, Kerim Suruliz - SYSTEMATICS OF MODULI STABILISATION IN CALABI-YAU FLUX COMPACTIFICATIONS,” JHEP 0503 (2005) 007 [ARXIV:HEP-TH/0502058]. – 42 , 2005
"... We present an explicit calculation of the spectrum of a general class of string models, corresponding to Calabi-Yau flux compactifications with h1,2> h1,1> 1 with leading perturbative and non-perturbative corrections, in which all geometric moduli are stabilised as in hep-th/0502058. The volum ..."
Abstract - Cited by 129 (20 self) - Add to MetaCart
We present an explicit calculation of the spectrum of a general class of string models, corresponding to Calabi-Yau flux compactifications with h1,2&gt; h1,1&gt; 1 with leading perturbative and non-perturbative corrections, in which all geometric moduli are stabilised as in hep-th/0502058. The volume is exponentially large, leading to a range of string scales from the Planck mass to the TeV scale, realising for the first time the large extra dimensions scenario in string theory. We provide a general analysis of the relevance of perturbative and non-perturbative effects and the regime of validity of the effective field theory. We compute the spectrum in the moduli sector finding a hierarchy of masses depending on inverse powers of the volume. We also compute soft supersymmetry breaking terms for particles living on D3 and D7 branes. We find a hierarchy of soft terms corresponding to ‘volume dominated ’ F-term supersymmetry breaking. F-terms for Kähler moduli dominate both those for dilaton and complex

Towards inflation in string theory

by Shamit Kachru, Renata Kallosh, Andrei Linde, Juan Maldacena , Liam McAllister, Sandip P. Trivedi - JCAP , 2003
"... We investigate the embedding of brane inflation into stable compactifications of string theory. At first sight a warped compactification geometry seems to produce a naturally flat inflaton potential, evading one well-known difficulty of brane-antibrane scenarios. Careful consideration of the closed ..."
Abstract - Cited by 82 (9 self) - Add to MetaCart
We investigate the embedding of brane inflation into stable compactifications of string theory. At first sight a warped compactification geometry seems to produce a naturally flat inflaton potential, evading one well-known difficulty of brane-antibrane scenarios. Careful consideration of the closed string moduli reveals a further obstacle: superpotential stabilization of the compactification volume typically modifies the inflaton potential and renders it too steep for inflation. We discuss the non-generic conditions under which this problem does not arise. We conclude that brane inflation models can only work if restrictive assumptions about the method of volume stabilization, the warping of the internal space, and the source of inflationary energy are satisfied. We argue that this may not be a real problem, given the large range of available fluxes and background geometries in string theory.
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...will choose to truncate AdS5 to the region r0 < r < rmax. The reader will notice that, apart from the additional manifold X5, this background is identical to that considered by Randall and Sundrum in =-=[18]-=-. Two physical insights from [18] will be crucial for our model. First, one can see from the warped metric (3.1) that the region of small r is the bottom of a gravitational well. Energies along the t,...

Spectral Dimension of the Universe in Quantum Gravity at a Lifshitz Point

by Petr Horava , 2009
"... We extend the definition of “spectral dimension ” (usually defined for fractal and lattice geometries) to theories on smooth spacetimes with anisotropic scaling. We show that in quantum gravity dominated by a Lifshitz point with dynamical critical exponent z in D+1 spacetime dimensions, the spectr ..."
Abstract - Cited by 81 (0 self) - Add to MetaCart
We extend the definition of “spectral dimension ” (usually defined for fractal and lattice geometries) to theories on smooth spacetimes with anisotropic scaling. We show that in quantum gravity dominated by a Lifshitz point with dynamical critical exponent z in D+1 spacetime dimensions, the spectral dimension of spacetime is equal to ds = 1 + D z. In the case of gravity in 3 + 1 dimensions presented in arXiv:0901.3775, which is dominated by z = 3 in the UV and flows to z = 1 in the IR, the spectral dimension of spacetime flows from ds = 4 at large scales, to ds = 2 at short distances. Remarkably, this is the qualitative behavior of ds found numerically by Ambjørn, Jurkiewicz and Loll in their causal dynamical
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