ﻻ يوجد ملخص باللغة العربية
In this talk I give a preliminary account of original results, obtained in collaboration with John Ellis. Details and further elaboration will be presented in a forthcoming publication. We present a proposal for a non-critical (Liouville) string approach to confinement of four-dimensional (non-abelian) gauge theories, based on recent developments on the subject by Witten and Maldacena. We discuss the effects of vortices and monopoles on the open world-sheets whose boundaries are Wilson loops of the target-space (non Abelian) Gauge theory. By appropriately employing `D-particles, associated with the target-space embedding of such defects, we argue that the apprearance of five-dimensional Anti-De-Sitter (AdS) space times is quite natural, as a result of Liouville dressing.We isolate the world-sheet defect contributions to the Wilson loop by constructing an appropriate observable, which is the same as the second observable in the supersymmetric U(1) theory of Awada and Mansouri, but in our approach supersymmetry is not necessary.When vortex condensation occurs, we argue in favour of a (low-temperature) confining phase, in the sense of an area law, for a large-$N_c$ (conformal) gauge theory at finite temperatures. A connection of the Berezinski-Kosterlitz-Thouless (BKT) transitions on the world-sheet with the critical temperatures in the thermodynamics of Black Holes in the five-dimensional AdS space is made.
We investigate the mathematical structure of the world sheet in two-dimensional conformal field theories.
We relate quark confinement, as measured by the Polyakov-loop order parameter, to color confinement, as described by the Kugo-Ojima/Gribov-Zwanziger scenario. We identify a simple criterion for quark confinement based on the IR behaviour of ghost and
The color-flavor locking phenomenon in the magnetic picture can be the microscopic description of the quark confinement in QCD. We demonstrate it in an N=2 supersymmetric SU(Nc)xSU(Nc) quiver gauge theory coupled to Nf flavors of quarks (Nf<Nc). This
Using the BF version of pure Yang-Mills, it is possible to find a covariant representation of the t Hooft magnetic flux operator. In this framework, t Hoofts pioneering work on confinement finds an explicit realization in the continuum. Employing the
The quantum theory of a massless spin two particle is strongly constrained by diffeomorphism invariance, which is in turn implied by unitarity. We explicitly exhibit the space-time diffeomorphism algebra of string theory, realizing it in terms of wor