ar X iv : h ep - t h / 95 09 16 7 v 3 6 O ct 1 99 5 SU 3 isoscalar factors

ar X iv : h ep - p h / 99 10 24 8 v 1 6 O ct 1 99 9 1 Effect of σ ( 600 ) - Production in pp̄ → 3 π 0 at rest

ar X iv : h ep - t h / 96 10 18 5 v 1 2 3 O ct 1 99 6 A Functional Approach to the Heat Kernel in Curved Space

ar X iv : h ep - t h / 95 07 17 2 v 1 3 1 Ju l 1 99 5 Quantum Corrections to the Semiclassical Quantization of the SU ( 3 ) Shell Model

ar X iv : h ep - t h / 96 07 09 1 v 3 3 O ct 1 99 6 A Non - Perturbative Superpotential With E 8 − Symmetry

We compute the non-perturbative superpotential in F -theory compactification to four dimensions on a complex three-fold P×S, where S is a rational elliptic surface. In contrast to examples considered previously, the superpotential in this case has interesting modular properties; it is essentially an E8 theta function. §

ar X iv : h ep - t h / 97 09 16 8 v 2 1 1 O ct 1 99 7 Zero curvature representation for classical lattice sine - Gordon equation via quantum R - matrix

Local M-operators for the classical sine-Gordon model in discrete space-time are constructed by convolution of the quantum trigonometric 4×4 R-matrix with certain vectors in its " quantum " space. Components of the vectors are identified with τ-functions of the model. This construction generalizes the known representation of M-operators in continuous time models in terms of Lax operators and cl...