ar X iv : h ep - p h / 02 05 33 3 v 1 3 0 M ay 2 00 2 DO WE UNDERSTAND WHAT IS DECONFINEMENT ?

ar X iv : h ep - p h / 02 05 01 6 v 1 2 M ay 2 00 2 Scalar a 0 ( 980 ) meson in φ → π 0 ηγ decay

ar X iv : h ep - p h / 03 04 05 2 v 2 9 M ay 2 00 3 Fluctuations and Deconfinement Phase Transition in Nucleus – Nucleus Collisions

The ratio of properly filtered multiplicity to energy fluctuations is shown to be sensitive to the equation of state of strongly interacting matter. Within a statistical approach to the early stage of nucleus–nucleus collisions, the ratio manifests a non–monotonic collision energy dependence with a maximum in the domain where the onset of deconfinement occurs.

ar X iv : h ep - p h / 00 05 02 8 v 1 3 M ay 2 00 0 Off - forward gluonometry .

We explore the deeply virtual Compton scattering process at NLO with the emphasis on the measurement of the tensor gluon skewed distributions. We recalculate the one-loop coefficient function and give two-loop results for anomalous dimensions and exclusive evolution kernels required for studying the logarithmic scaling violation. We evaluate weighted cross sections which give direct access to t...

ar X iv : h ep - p h / 03 05 02 3 v 2 9 M ay 2 00 3 Is Quark Saturation Related to the Pauli Principle ? ∗

Below the saturation momentum the sea quark occupation number reaches a pure number, independent of any parameters in QCD, reminiscent of a Pauli Principle result. We argue, however, that the Pauli Principle plays no role in this result.

ar X iv : h ep - p h / 02 05 13 2 v 1 1 3 M ay 2 00 2 Jet Production at CDF ∗

In this talk I present the results from the measurement of the inclusive jet cross section and strong coupling constant based on the CDF Run 1B data, and discuss prospects for Run 2.