ar X iv : h ep - t h / 02 07 26 0 v 2 3 1 Ju l 2 00 2 SNUTP 02 / 024 More self - tuning solutions with H MNPQ

ar X iv : h ep - t h / 02 07 26 0 v 1 3 0 Ju l 2 00 2 SNUTP 02 / 024 More self - tuning solutions with H MNPQ

We find more self-tuning solutions by introducing a general form for Lagrangian of a 3-index antisymmetric tensor field AMNP in the RS II model. In particular, for the logarithmic Lagrangian, ∝ log(−H2), we obtained a closed form weak self-tuning solution. [

ar X iv : h ep - t h / 02 07 26 0 v 3 2 1 A ug 2 00 2 SNUTP 02 / 024 More self - tuning solutions with H MNPQ

We find more self-tuning solutions by introducing a general form for Lagrangian of a 3-index antisymmetric tensor field AMNP in the RS II model. In particular, for the logarithmic Lagrangian, ∝ log(−H2), we obtained a closed form weak self-tuning solution.

ar X iv : h ep - t h / 03 02 18 9 v 3 2 3 Ju l 2 00 3 Ring - shaped exact Hopf solitons

The existence of ring-like structures in exact hopfion solutions is shown.

ar X iv : h ep - p h / 02 07 17 0 v 1 1 4 Ju l 2 00 2 1 Measurement of | V ub | in semi - inclusive charmless B → πX decays

ar X iv : h ep - p h / 00 07 19 4 v 3 2 0 Ju n 20 02 Theoretical Issues in the Tevatron Era 1

The Fermilab Tevatron’s operation for fixed-target physics from its start in 1983 until the end of fixed-target running in 2000 was marked by extraordinary productivity and variety. Some of the changing theoretical issues associated with this program are reviewed.