ar X iv : h ep - t h / 05 03 22 3 v 1 2 9 M ar 2 00 5 Probing the 5 th Dimension with the QCD String ∗

ar X iv : h ep - t h / 06 03 12 5 v 1 1 5 M ar 2 00 6 hep - th / 0603125 ITP – UH – 05 / 06 Noncommutative Instantons on C

We construct explicit solutions of the Hermitian Yang-Mills equations on the noncommutative space C θ . In the commutative limit they coincide with the standard instantons on CP written in local coordinates.

ar X iv : h ep - p h / 04 05 03 5 v 1 5 M ay 2 00 4 Determination of the mass of the ΛΛ dibaryon by the method of QCD sum rules

ar X iv : h ep - p h / 04 05 03 9 v 1 5 M ay 2 00 4 η , η ′ → π + π − γ with coupled channels

ar X iv : h ep - t h / 05 11 10 5 v 1 9 N ov 2 00 5 QCD partition function in the external field in the covariant gauge

The QCD partition function in the external stationary gluomag-netic field is computed in the third order in external field invariants in arbitrary dimension and arbitrary covariant gauge. The contributions proportional to third order invariants in gluon field strength are shown to be dependent on covariant quantum gauge fixing parameter α.

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.