The talk is an introduction into diquark condensation phenomena which occur in QCD at high energy density. They are driven by instantons and instanton-antiinstanton pairs (or "molecules"), which generate attraction in some qq channels. A number of phases is possible, with or without restoration of
High-Density QCD and Instantons
✍ Scribed by R. Rapp; T. Schäfer; E.V. Shuryak; M. Velkovsky
- Publisher
- Elsevier Science
- Year
- 2000
- Tongue
- English
- Weight
- 715 KB
- Volume
- 280
- Category
- Article
- ISSN
- 0003-4916
No coin nor oath required. For personal study only.
✦ Synopsis
Instantons generate strong nonperturbative interactions between quarks. In vacuum, these interactions lead to chiral symmetry breaking and generate constituent quark masses on the order of 300 400 MeV. The observation that the same forces also provide attraction in the scalar diquark channel leads to the prediction that cold quark matter is a color superconductor, with gaps as large as t100 MeV. We provide a systematic treatment of color superconductivity in the instanton model. We show that the structure of the superconductor depends on the number of flavors. In the case of two flavors, we verify the standard scenario, and provide an improved calculation of the mass gap. For three flavors, we show that the ground state is color flavor locked and calculate the chiral condensate in the high-density phase. We show that as a function of the strange quark mass, there is a sharp transition between the two phases. Finally, we go beyond the mean-field approximation and investigate the role of instantonÂanti-instanton molecules, which in addition to superconducting gap formation provide a competitive mechanism for chiral restoration at finite density. 2000
📜 SIMILAR VOLUMES
We study the rôle of semiclassical QCD vacuum solutions in high-energy scattering by considering the instanton contribution to hadronic cross sections. We propose a new type of instanton-induced interactions ("instanton ladder") that leads to the rising with energy cross section σ ∼ s ∆ of Regge typ