ar X iv : h ep - p h / 03 03 23 0 v 3 10 S ep 2 00 3 Color superconductor with a color - sextet condensate

ar X iv : h ep - p h / 03 11 02 8 v 1 3 N ov 2 00 3 RHIC Physics : The Quark Gluon Plasma and The Color Glass Condensate : 4 Lectures ∗

The purpose of these lectures is to provide an introduction to the physics issues which are being studied in the RHIC heavy ion program. These center around the production of new states of matter. The Quark Gluon Plasma is thermal matter which once existed in the big bang which may be made at RHIC. The Color Glass Condensate is a universal form of matter which controls the high energy limit of ...

ar X iv : h ep - p h / 03 07 12 5 v 2 1 5 Ju l 2 00 3 RU 03 - 02 - B Color Superconductivity in a Dense Quark Matter Hai - cang

The color superconductivity of a dense quark matter is reviewed with emphasis on the long range nature of the pairing force and the multiplicity of the order parameter. The former gives rise to a non BCS behavior of the superconducting energy scale and the latter modifies the critical value of the Ginzburg-Landau parameter that separates the superconductivity of type I and that of type II.

ar X iv : h ep - p h / 03 10 27 3 v 1 2 3 O ct 2 00 3 The Constant Background Bag Model of Hadron

The motion of quark is studied in a confining bag having central color field. The Dirac equation is solved for a quark in such bag and its energy spectrum is found. It is pointed out the possibility to identify the external color field with the background field of gluon condensation. This makes the received energy spectrum of quark useful for comparison with the energy spectrum of hadrons.

ar X iv : h ep - p h / 03 07 03 8 v 1 2 J ul 2 00 3 1 Scalar meson exchange in Φ → P 0 P 0 γ decays ∗

ar X iv : h ep - p h / 01 06 32 4 v 2 3 J ul 2 00 1 Anderson Theorem for Color Superconductor

Ginzburg-Landau functional is derived for a system possessing both chiral and diquark condensates. Anderson theorem for such a system is formulated and proved.