ar X iv : h ep - p h / 04 02 07 9 v 1 7 F eb 2 00 4 UH – 511 – 1043 – 04 LBL – 54494 February 2004

ar X iv : h ep - p h / 04 02 07 9 v 2 2 7 Fe b 20 04 UH – 511 – 1043 – 04 LBL – 54494 February 2004

If the narrow exotic baryon resonances Θ+(1540) and Ξ 3 2 (1862) are members of the JP = 12 + antidecuplet with N∗(1710), the octet-antidecuplet mixing is required not only by the mass spectrum but also by the decay pattern of N∗(1710). This casts doubt on validity of the Θ+ mass prediction by the chiral soliton model. While all pieces of the existing experimental information point to a small o...

ar X iv : h ep - p h / 04 02 19 0 v 2 2 6 M ay 2 00 4 1 Pentaquarks in the 10 F - and 10 F - plets

ar X iv : h ep - p h / 04 02 09 2 v 1 9 F eb 2 00 4 Precision Electroweak Constraints and the Mixed Radion - Higgs Sector ∗

Adding radion perturbations (up to second order) to the static (RS) metric allows us to calculate the general first and second order interactions of the radion field with the electroweak vector bosons. We use these interactions to compute precision electroweak observables in the case of Higgs-radion mixing and compare with experiment.

ar X iv : h ep - p h / 04 02 07 9 v 3 5 M ay 2 00 4 UH – 511 – 1043 – 04

If the narrow exotic baryon resonances Θ+(1540) and Ξ 3 2 (1862) are members of the JP = 12 + antidecuplet with N∗(1710), the octet-antidecuplet mixing is required not only by the mass spectrum but also by the decay pattern of N∗(1710). This casts doubt on validity of the Θ+ mass prediction by the chiral soliton model. While all pieces of the existing experimental information point to a small o...

ar X iv : h ep - p h / 04 05 11 9 v 1 1 3 M ay 2 00 4 The Lorentz and CPT violating effects on the charged