ar X iv : h ep - p h / 96 02 36 9 v 1 2 2 Fe b 19 96 hep - ph / 9602369 Neutrino Properties

ar X iv : h ep - p h / 96 02 40 1 v 1 2 6 Fe b 19 96 UG - FT - 57 / 96 hep - ph / 9602401 February 1996 CHIRAL PERTURBATION THEORY

An introduction to the methods and ideas of Chiral Perturbation Theory is presented in this talk. The discussion is illustrated with some phenomenological predictions that can be compared with available experimental results.

ar X iv : h ep - p h / 96 02 28 5 v 1 1 3 Fe b 19 96 hep - ph / 9602285 INP 1715 / PH QCD : Quantum

The first measurements of the diffractive structure function F D(3) 2 at HERA are discussed. A factorisable interpretation in which a partonic structure is assigned to the pomeron is investigated through QCD analyses in which both the quark and gluon densities are permitted to vary freely. A method of measuring the longitudinal structure function of the pomeron without changing the ep centre of...

ar X iv : h ep - t h / 96 02 14 9 v 1 2 7 Fe b 19 96 UAHEP - 9603 DSFNA - T - 9606 ESI - 310 February 1996

Integrability of the Wess–Zumino–Witten model as a non–ultralocal theory * Abstract We consider the 2–dimensional Wess–Zumino–Witten (WZW) model in the canon-ical formalism introduced in [5]. Using an r–s matrix approach to non–ultralocal field theories we find the Poisson algebra of monodromy matrices and of conserved quantities with a new, non–

ar X iv : h ep - p h / 96 02 38 0 v 1 2 3 Fe b 19 96 Electroweak Theory

In these lectures we give a discussion of the structure of the electroweak Standard Model and its quantum corrections for tests of the electroweak theory. The predictions for the vector boson masses, neutrino scattering cross sections and the Z resonance observables are presented in some detail. We show comparisons with the recent experimental data and their implications for the present status ...

ar X iv : h ep - p h / 98 02 41 9 v 1 2 5 Fe b 19 98 COURSE LARGE N QCD