ar X iv : h ep - t h / 94 01 16 2 v 1 3 1 Ja n 19 94 NCL 94 - TP 3 When q = 0 , The Forced Harmonic Oscillator Isn

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 / 94 06 43 3 v 1 3 0 Ju n 19 94 UdeM – GPP – TH – 04

I summarize the prospects for discovering Higgs bosons at future pp and e + e − colliders both in the Standard Model and its Minimal Supersymmetric extension.

ar X iv : h ep - p h / 94 11 26 3 v 1 1 0 N ov 1 99 4 ISU – NP – 94 – 14 Massive Schwinger Model for Small Fermion Mass

We examine QED 1+1 (the massive Schwinger model) to extend existing perturbation results in m f /m b , and compare our results with lattice and DLCQ calculations.

ar X iv : h ep - p h / 94 05 28 5 v 1 1 3 M ay 1 99 4 TUTP – 94 - 10

We consider dyon configurations in the standard electroweak model. In the presence of a θ term and no fermions, the usual result q = (n+ θ/2π)e is obtained for the electric charge spectrum. The effect of including standard model fermions is discussed qualitatively.

ar X iv : h ep - t h / 94 02 02 0 v 1 3 F eb 1 99 4 PERTURBATIVE BOSONIC END ANYON SPECTRA AND CONTACT INTERACTIONS

Bosonic end perturbative calculations for quantum mechanical anyon systems require a regularization. I regularize by adding a specific δ-function potential to the Hamiltonian. The reliability of this regularization procedure is verified by comparing its results for the 2-anyon in harmonic potential system with the known exact solutions. I then use the δ-function regularized bosonic end perturba...