Abstract:We construct the nonlocal braneworld action in the two-brane Randall-Sundrum model in a holographic setup alternative to Kaluza-Klein description: the action is written as a functional of the two metric and radion fields on the branes. This action effectively describes the dynamics of the gravitational field both on the branes and in the bulk in terms of the brane geometries directly accessible for observations. Its nonlocal form factors incorporate the cumulative effect of the bulk Kaluza-Klein modes. We also… Show more
“…For flat 4-dimensional branes, R(g) = 0, d = 4, this expression reduces to the result obtained in [14] 11 .…”
Section: Scalar and Vector Sectorsmentioning
confidence: 76%
“…These properties of the braneworld formalism were considered in much detail in a number of papers [14,21,22] where the location of branes in the bulk was described in the Gaussian normal coordinates, G yy = 1, G yµ = 0, by an additional scalar field -the radion.…”
“…We will calculate the braneworld effective action defined by the procedure that was discussed in much detail in [14]. In contrast to the conventional Kaluza-Klein reduction, usually used for the construction of the effective action [18,19], our action is a functional of the fields that have direct physical and geometrical interpretation.…”
Section: Braneworld Effective Actionmentioning
confidence: 99%
“…In contrast to the results of these works we concentrate on two-brane models with independent metric configurations on their branes. This is done along the lines of the previous papers [13,14] where the weak field (quadratic in perturbations) approximation for braneworld action was obtained on the background of flat branes. In distinction from [7,9,10] we obtain the nonlocal action nontrivially intertwining metric fields on both branes.…”
Section: Introductionmentioning
confidence: 99%
“…Its derivation is based on the technique of linearized invariants of the diffeomorphism gauge transformations intensively used in the theory of cosmological perturbations [15,16,17]. Sect.4 gives a review of the alternative calculation [14] of the same result, based on its recovery from the effective equations of motion. In Sect.5 we show the equality of the two manifestly different quadratic forms of the action by proving that their kernels are equal to one another -the main duality relation between specific operators of the Dirichlet and Neumann boundary value problems.…”
Braneworld effective action is constructed by two different methods based respectively on the Dirichlet and Neumann boundary value problems. The equivalence of these methods is shown due to nontrivial duality relations between special boundary operators of these two problems. Previously known braneworld action algorithms in two-brane Randall-Sundrum model are generalized to curved branes with deSitter and Anti-deSitter geometries. †
“…For flat 4-dimensional branes, R(g) = 0, d = 4, this expression reduces to the result obtained in [14] 11 .…”
Section: Scalar and Vector Sectorsmentioning
confidence: 76%
“…These properties of the braneworld formalism were considered in much detail in a number of papers [14,21,22] where the location of branes in the bulk was described in the Gaussian normal coordinates, G yy = 1, G yµ = 0, by an additional scalar field -the radion.…”
“…We will calculate the braneworld effective action defined by the procedure that was discussed in much detail in [14]. In contrast to the conventional Kaluza-Klein reduction, usually used for the construction of the effective action [18,19], our action is a functional of the fields that have direct physical and geometrical interpretation.…”
Section: Braneworld Effective Actionmentioning
confidence: 99%
“…In contrast to the results of these works we concentrate on two-brane models with independent metric configurations on their branes. This is done along the lines of the previous papers [13,14] where the weak field (quadratic in perturbations) approximation for braneworld action was obtained on the background of flat branes. In distinction from [7,9,10] we obtain the nonlocal action nontrivially intertwining metric fields on both branes.…”
Section: Introductionmentioning
confidence: 99%
“…Its derivation is based on the technique of linearized invariants of the diffeomorphism gauge transformations intensively used in the theory of cosmological perturbations [15,16,17]. Sect.4 gives a review of the alternative calculation [14] of the same result, based on its recovery from the effective equations of motion. In Sect.5 we show the equality of the two manifestly different quadratic forms of the action by proving that their kernels are equal to one another -the main duality relation between specific operators of the Dirichlet and Neumann boundary value problems.…”
Braneworld effective action is constructed by two different methods based respectively on the Dirichlet and Neumann boundary value problems. The equivalence of these methods is shown due to nontrivial duality relations between special boundary operators of these two problems. Previously known braneworld action algorithms in two-brane Randall-Sundrum model are generalized to curved branes with deSitter and Anti-deSitter geometries. †
We discuss the theory and phenomenology of the interplay between the massless graviton and its massive Kaluza-Klein modes in the Randall-Sundrum two-brane model. The equations of motion of the transverse traceless degrees of freedom are derived by means of a Green function approach as well as from an effective nonlocal action. The second procedure clarifies the extraction of the particle content from the nonlocal action and the issue of its diagonalization. The situation discussed is generic for the treatment of two-brane models if the on-brane fields are used as the dynamical degrees of freedom. The mixing of the effective graviton modes of the localized action can be interpreted as radion-induced gravitational-wave oscillations, a classical analogy to meson and neutrino oscillations. We show that these oscillations arising in M-theorymotivated braneworld setups could lead to effects detectable by gravitational-wave interferometers. The implications of this effect for models with ultra-light gravitons are discussed.
We discuss the theory and phenomenology of the interplay between the massless graviton and its massive Kaluza‐Klein modes in the Randall‐Sundrum two‐brane model. The equations of motion of the transverse traceless degrees of freedom are derived by means of a Green function approach as well as from an effective nonlocal action. The second procedure clarifies the extraction of the particle content from the nonlocal action and the issue of its diagonalization. The situation discussed is generic for the treatment of two‐brane models if the on‐brane fields are used as the dynamical degrees of freedom. The mixing of the effective graviton modes of the localized action can be interpreted as radion‐induced gravitational‐wave oscillations, a classical analogy to meson and neutrino oscillations. We show that these oscillations arising in M‐theory‐motivated braneworld setups could lead to effects detectable by gravitational‐wave interferometers. The implications of this effect for models with ultra‐light gravitons are discussed.
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