ar X iv : h ep - t h / 99 11 16 7 v 1 2 2 N ov 1 99 9 The Finiteness Requirement for Six - Dimensional

ar X iv : h ep - t h / 99 11 02 7 v 1 4 N ov 1 99 9 Holography and the Future Tube

The Future Tube T + n of n-dimensional Minkowski spacetime may be identified with the reduced phase space P , or " space of motions " of a particle moving in (n + 1)-dimensional Anti-de-Sitter Spacetime. Both are isomorphic to a homogeneous bounded domain in C n whose Shilov boundary may be identified with n-dimensional conformally compactified Minkowski spacetime.

ar X iv : h ep - p h / 94 11 23 2 v 1 7 N ov 1 99 4 CHIRAL PERTURBATION THEORY 1

ar X iv : h ep - t h / 94 10 11 8 v 2 2 2 N ov 1 99 4 WILSON LOOPS , qq̄ and 3 q POTENTIALS , BETHE – SALPETER EQUATION

ar X iv : h ep - p h / 99 11 40 8 v 1 19 N ov 1 99 9 Quark Matter 99 Summary : Hadronic Signals

ar X iv : h ep - t h / 99 11 16 3 v 2 3 0 N ov 1 99 9 hep - th / 9911163 Logarithmic Operators in AdS 3 / CFT 2

We discuss the relation between singletons in AdS 3 and logarithmic operators in the CFT on the boundary. In 2 dimensions there can be more logarithmic operators apart from those which correspond to singletons in AdS, because logarithmic operators can occur when the dimensions of primary fields differ by an integer instead of being equal. These operators may be needed to account for the greybod...