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 t
QCD phases at high density and instantons
β Scribed by E. Shuryak
- Publisher
- Elsevier Science
- Year
- 1998
- Tongue
- English
- Weight
- 964 KB
- Volume
- 642
- Category
- Article
- ISSN
- 0375-9474
No coin nor oath required. For personal study only.
β¦ Synopsis
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 chiral symmetry: the work is not finished and we do not yet know which take place in real &CD. We also emphasize that specific diquark correlations play a significant role in baryon structure, in particular making that of a nucleon very different of a a (or other member of a decuplet).
This "small N," scenario based on comparison to QCD with two colors is contrasted with the "large N," one.
π SIMILAR VOLUMES
We study the thermal properties of QCD in the presence of a small quark chemical potential ,L Derivatives of the phase transition point with respect to p are computed at /.L = 0 for 2 and 3 flavors of p-4 improved staggered fermions on a 163 x 4 lattice. Moreover we contrast the case of isoscalar an
We study fermionic quasi-particles in QCD at very high baryon density. In the normal quark matter phase unscreened magnetic gluon exchanges lead to non-Fermi liquid behavior. Non-Fermi liquid effects manifest themselves in low energy Green functions that depend on logarithms and fractional powers of
We present results on the QCD phase diagram for small densities without reweighting. Our simulations are performed with an imaginary chemical potential ,LLI for which the fermion determinant is positive. On an 83 x 4 lattice with 2 flavors of staggered quarks, we map out the pseudo-critical temper