old personal page at Princeton (archived screenshot)
“My main interests this year [1993?] were directed towards string theory of quark confinement. The problem is to find the string Lagrangian for the Faraday’s ”lines of force“, which would reproduce perturbative corrections from the Yang-Mills theory to the Coulomb law at small distances and would give permanent confinement of quarks at large distances.”
Valery Pokrovsky, Hidden Sasha Polyakov’s life in Statistical and Condensed Matter Physics, in: Polyakov’s String: Twenty Five Years After, Proceedings of an International Workshop at Chernogolovka (2005) 2-15 [arXiv:hep-th/0510214]
Discussing what came to be called the Polyakov action for the bosonic string and the resulting Liouville theory, in the non-critical case:
and for the superstring:
Introducing conformal field theory:
Early discussion of Wilson loop quantum observables in -Chern-Simons theory:
Proposing the identification of flux tubes in confined QCD with the strings of string theory, hence of the holographic principle in what came to be known as the AdS-QCD correspondence (see Polyakov gauge-string duality):
Alexander Polyakov, String representations and hidden symmetries for gauge fields, Physics Letters B 82 2 (1979) 247-250 [doi:10.1016/0370-2693(79)90747-0]
Alexander Polyakov, Gauge fields as rings of glue, Nuclear Physics B 164 (1980) 171-188 [doi:10.1016/0550-3213(80)90507-6]
Alexander Polyakov, Gauge Fields and Strings, Routledge, Taylor and Francis (1987, 2021) [doi:10.1201/9780203755082, oapen:20.500.12657/50871]
Alexander Polyakov, String Theory and Quark Confinement, Nucl. Phys. Proc. Suppl. 68 (1998) 1-8 [arXiv:hep-th/9711002, doi:10.1016/S0920-5632(98)00135-2]
Alexander Polyakov, The wall of the cave, Int. J. Mod. Phys. A 14 (1999) 645-658 [arXiv:hep-th/9809057, doi:10.1142/S0217751X99000324]
eventually leading to the rules of the AdS-CFT correspondence:
Relations between gauge fields and strings present an old, fascinating and unanswered question. The full answer to this question is of great importance for theoretical physics. It will provide us with a theory of quark confinement by explaining the dynamics of color-electric fluxes.
and specifically between single trace operators and superstring-excitations:
The picture which slowly arises from the above considerations is that of the space-time gradually disappearing in the regions of large curvature. The natural description in this case is provided by a gauge theory in which the basic objects are the texts formed from the gauge-invariant words. The theory provides us with the expectation values assigned to the various texts, words and sentences.
These expectation values can be calculated either from the gauge theory or from the strongly coupled 2d sigma model. The coupling in this model is proportional to the target space curvature. This target space can be interpreted as a usual continuous space-time only when the curvature is small. As we increase the coupling, this interpretation becomes more and more fuzzy and finally completely meaningless.
Historical reminiscences:
Alexander Polyakov, Confinement and Liberation, in Gerardus ’t Hooft (ed.) 50 Years of Yang-Mills Theory (2005) 311-329 [arXiv:hep-th/0407209, doi:10.1142/9789812567147_0013, doi:10.1142/5601]
Alexander M. Polyakov, Beyond Space-Time, in The Quantum Structure of Space and Time, Proceedings of the 23rd Solvay Conference on Physics, World Scientific (2007) [arXiv:hep-th/0602011, pdf]
Alexander M. Polyakov, From Quarks to Strings [arXiv:0812.0183]
published as Quarks, strings and beyond, section 44 in: Paolo Di Vecchia et al. (ed.), The Birth of String Theory, Cambridge University Press (2012) 544-551 [doi:10.1017/CBO9780511977725.048]
“By the end of ’77 it was clear to me that I needed a new strategy [for understanding confinement] and I became convinced that the way to go was the gauge/string duality. […]”
“I kept thinking about gauge/strings dualities. Soon after the Liouville mode was discovered it became clear to many people including myself that its natural interpretation is that random surfaces in 4d are described by the strings flying in 5d with the Liouville field playing the role of the fifth dimension. The precise meaning of this statement is that the wave function of the general string state depends on the four center of mass coordinates and also on the fifth, the Liouville one. In the case of minimal models this extra dimension is related to the matrix eigenvalues and the resulting space is flat.”
“Since this 5d space must contain the flat 4d subspace in which the gauge theory resides, the natural ansatz for the metric is just the Friedman universe with a certain warp factor. This factor must be determined from the conditions of conformal symmetry on the world sheet. Its dependence on the Liouville mode must be related to the renormalization group flow. As a result we arrive at a fascinating picture – our 4d world is a projection of a more fundamental 5d string theory. […]”
“At this point I was certain that I have found the right language for the gauge/string duality. I attended various conferences, telling people that it is possible to describe gauge theories by solving Einstein-like equations (coming from the conformal symmetry on the world sheet) in five dimensions. The impact of my talks was close to zero. That was not unusual and didn’t bother me much. What really caused me to delay the publication (Polyakov 1998) for a couple of years was my inability to derive the asymptotic freedom from my equations. At this point I should have noticed the paper of Klebanov 1997 in which he related D3 branes described by the supersymmetric Yang Mills theory to the same object described by supergravity. Unfortunately I wrongly thought that the paper is related to matrix theory and I was skeptical about this subject. As a result I have missed this paper which would provide me with a nice special case of my program. This special case was presented little later in full generality by Juan Maldacena (Maldacena 1997) and his work opened the flood gates.”
Last revised on July 25, 2024 at 19:13:41. See the history of this page for a list of all contributions to it.
