ar X iv : h ep - t h / 99 03 04 4 v 1 4 M ar 1 99 9 When radiative corrections are finite but undetermined

ar X iv : h ep - t h / 99 03 20 9 v 1 2 4 M ar 1 99 9 SMI - Th – 99 / 04 AdS 3 / CFT 2 correspondence at finite temperature

The AdS/CFT correspondence is established for the AdS 3 space compactified on a solid torus with the CFT field on the boundary. Correlation functions that correspond to the bulk theory at finite temperature are obtained in the regularization a'la Gubser, Klebanov, and Polyakov. The BTZ black hole solutions in AdS 3 are T-dual to the solution in the AdS 3 space without singularity.

ar X iv : h ep - p h / 99 03 44 4 v 1 2 2 M ar 1 99 9 RECOVERING CORRECTIONS IN THE ANALYSIS OF INTERMITTENT DATA ∗ Beata

The analysis of intermittent data is improved. The standard method of recovering the history of a particle cascade is proved in general not to reproduce the structure of the true cascade. The recovering corrections to the standard method are proposed and tested in the framework of multiplicative cascading models.

ar X iv : h ep - t h / 99 03 19 4 v 1 2 2 M ar 1 99 9 The Wess - Zumino Model and the AdS 4 / CFT 3 Correspondence

We consider the non-interacting massive Wess-Zumino model in four-dimensional anti-de Sitter space and show that the conformal dimensions of the corresponding boundary fields do not always satisfy the relation expected from superconformal invariance.

ar X iv : h ep - t h / 97 03 05 4 v 1 6 M ar 1 99 7 Symmetries and the Antibracket : The Batalin - Vilkovisky Method

ar X iv : h ep - p h / 95 12 36 9 v 3 1 3 M ar 1 99 6 Electroweak corrections to the muon anomalous magnetic moment

The bosonic two-loop electroweak radiative corrections to the muon’s anomalous magnetic moment, aμ ≡ (gμ − 2)/2, are presented. We find ∆a μ (2 loop bosonic)/a EW μ (1 loop) ≈ απ (