Renormalized AdS action and Critical Gravity

Aug 9, 2014 - n(2n - 2)! . (2.6). Above, the totally antisymmetric Kronecker delta of order m ..... Euler characteristic χ(M) in the Euler theorem in...

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e-Print: hep-th/9905111. [3] S.W. Hawking and D. Page Commun. Math. Phys. 87 (1983) 577. [4] M. Henningson and K. Skenderis, JHEP 9807 (1998) 023, ...

Jun 21, 2017 - In order to do so we have taken the liberty of fixing the scale to analyze two possible scenarios which reproduce the two conflicting views.

Mar 13, 2018 - 4G. +. (-1) n l2(n−1). 4G[2 (n - 1)]!. ∫. ∂Σ. B2n−3,. (2) where l is the ..... EE, and then we check that the divergences are exactly cancelled by the ...

ory, as derived from the AdS/CFT correspondence, and the RG flow equations in. 4–dimensional ..... 5For another (different) discussion of the role of Weyl gravity in the context of the AdS/CFT correspon- dence, see [24]. ..... Let us also quote the

Sep 6, 2006 - arXiv:hep-ph/0609058v1 6 Sep 2006 ..... Wang, World Scientific, Singapore, hep-ph/0303185; J. O. Andersen, M. Strickland,. AP 317, 281 ...

already be studied in simple scalar theories. For recent reviews in this context see. Ref. [10]. A promising candidate for an improved convergence behavior is the loop ... [12] for a similar strategy in the context of Schwinger-Dyson equations. .....

Jul 22, 2008 - [email protected] ... is expressible as the sum of two higher derivative SL(2, R) “vector” Chern- ... spins in higher dimensions [7,8].

Dec 25, 2013 - the volume renormalization of conformally compact Einstein (CCE) metrics [1]: 1. in 'Lanczos-form', as volume ... 2. in 'Weyl-form', as renormalized volume of 4D CCE metrics [3, 4]. ∫M4. Weyl2 . (2). The integral of ..... V. DIMENSIO

Oct 1, 2012 - [4] E.A. Bergshoeff, O. Hohm and P.K. Townsend, Massive gravity in ... [8] R. Andringa, E.A. Bergshoeff, M. de Roo, O. Hohm, E. Sezgin and P.K. ...

worldvolume field theory and especially a regular horizon translates into a non- trivial IR fixpoint. For this interpretation we have to rewrite the AdS models into a flat space description with a linear dilaton vacuum. The dual models (linear dilato

Jan 21, 2014 - finding AdS wave solutions of the full non-linear theory, that behave as logarithmic modes towards the AdS ... give gravity duals of LCFTs and this correspondence has been termed the AdS/LCFT correspondence (see ...... Chern-Simons hol

Aug 5, 2011 - We deform the anti-de Sitter algebra by adding additional generators Zab, forming in this way the negative ... address: [email protected] †Electronic address: [email protected] ... with the metric tensor ηIJ , I,

Dec 22, 2004 - The higher dimensional gravity theory of Lovelock[2] is an interesting generalisation of. General Relativity. In d ≥ 5 the Einstein-Hilbert Lagrangian is not the most .... there is a certain ambiguity about the solutions- in general,

Sep 16, 2004 - In ADM, the physical, propagating degrees of freedom of massless gravity are the space metric, gij i = 1,2,3 and its ... not change the fact that Ni,N are nondynamical, but makes them appear nonlinearly in the action of massive ... Fre

Oct 11, 2006 - make the theory different to the Einstein gravity. Higher co-dimension membranes may lie at the intersection of co-dimension 1 hypersurfaces in Lovelock gravity; the hypersurfaces are located at the discontinuities of the first derivat

Nov 15, 2008 - arXiv:0811.2523v1 [cond-mat.supr-con] 15 Nov 2008. Renormalized behavior and ... We report synthesis and single crystal measurements of magnetic, transport and thermal proper- ties of single crystalline BaCo2As2 as well ... croanalysis

May 27, 2014 - Department of Information and Communication Systems Engineering. University of the ... We show that the Ashtekar-Magnon-Das (AMD) mass and other conserved quanti- ties are equivalent to the ... defined on the anti-de Sitter (AdS) space

Aug 5, 2015 - 1 Dipartimento di Fisica dell'Universit`a di Roma “La Sapienza” and INFN,. Sezione .... massless regime, while for ˜t → ∞ we recover the weak-.

mn α† nmn αnmn ,. (5) being ǫp,ǫn the quasiparticle energies and α† p,α† ..... m m mm m m m m m m m m m m m mm m m m m m m mmmmm mmmmmmm m.

May 18, 2012 - is well known that in order to get finite results from AdS/CFT one needs to add counterterms to the bulk ... d-dimensional CFTs, they are also crucial to get a finite free energy when the theory is placed on .... a Schwarzschild black

We explore the connection between anti-deSitter supergravity and gauge theory, in the context of bound states of many D1 and D5 branes. The near-horizon AdS3 × S3 supergravity describes the identity sector of the conformal field theory produced by t

of this method to the traditional reference spacetime is discussed. For AdS ...... The Bekenstein-Hawking formula Sent = A/4G and the generalized Smarr formula:.

Jun 16, 2018 - drm. )−1 . (4.18). Figure 3: Penrose diagram for the non-rotating BH, with ..... by several authors in in [60, 61, 62, 63], but always in the late-time.

Apr 29, 2012 - cone gauge and dualize one index on the metric tensor by means of the epsilon tensor of the .... The epsilon symbol is defined by ε012··· = +1, i.e. as ..... ˜Λa1...aD−2. = 1. 2. (-1)D−3(D - 2)ǫa1...aD−2bc Λbc . (3.22). T