TY - JOUR
T1 - Holography and compactification
AU - Verlinde, Herman
N1 - Funding Information:
This work is supported by NSF-grant 98-02484, a Pionier fellowship of NWO, and the Packard foundation. I would like to thank Costas Bachas, Micha Berkooz, Jan de Boer, Robbert Dijkgraaf, Savas Dimopoulos, Lisa Randall, Savdeep Sethi, Raman Sundrum, Erik Verlinde, and E. Witten for very helpful discussions.
PY - 2000/7/31
Y1 - 2000/7/31
N2 - Following a recent suggestion by Randall and Sundrum, we consider string compactification scenarios in which a compact slice of AdS-space arises as a subspace of the compactification manifold. A specific example is provided by the type II orientifold equivalent to type I theory on (orbifolds of) T6, upon taking into account the gravitational backreaction of the D3-branes localized inside the T6. The conformal factor of the four-dimensional metric depends exponentially on one of the compact directions, which, via the holographic correspondence, becomes identified with the renormalization group scale in the uncompactified world. This set-up can be viewed as a generalization of the AdS/CFT correspondence to boundary theories that include gravitational dynamics. A striking consequence is that, in this scenario, the fundamental Planck size string and the large N QCD string appear as (two different wavefunctions of) one and the same object.
AB - Following a recent suggestion by Randall and Sundrum, we consider string compactification scenarios in which a compact slice of AdS-space arises as a subspace of the compactification manifold. A specific example is provided by the type II orientifold equivalent to type I theory on (orbifolds of) T6, upon taking into account the gravitational backreaction of the D3-branes localized inside the T6. The conformal factor of the four-dimensional metric depends exponentially on one of the compact directions, which, via the holographic correspondence, becomes identified with the renormalization group scale in the uncompactified world. This set-up can be viewed as a generalization of the AdS/CFT correspondence to boundary theories that include gravitational dynamics. A striking consequence is that, in this scenario, the fundamental Planck size string and the large N QCD string appear as (two different wavefunctions of) one and the same object.
UR - http://www.scopus.com/inward/record.url?scp=0000125525&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=0000125525&partnerID=8YFLogxK
U2 - 10.1016/S0550-3213(00)00224-8
DO - 10.1016/S0550-3213(00)00224-8
M3 - Article
AN - SCOPUS:0000125525
SN - 0550-3213
VL - 580
SP - 264
EP - 274
JO - Nuclear Physics B
JF - Nuclear Physics B
IS - 1-2
ER -