PIRSA:12030113

Video URL

https://pirsa.org/12030113

Mass gap, topological molecules, and strong gauge dynamics

Unsal, M. (2012). Mass gap, topological molecules, and strong gauge dynamics. Perimeter Institute for Theoretical Physics. https://pirsa.org/12030113

Unsal, Mithat. Mass gap, topological molecules, and strong gauge dynamics. Perimeter Institute for Theoretical Physics, Mar. 21, 2012, https://pirsa.org/12030113 

          @misc{ scivideos_PIRSA:12030113,
            doi = {10.48660/12030113},
            url = {https://pirsa.org/12030113},
            author = {Unsal, Mithat},
            keywords = {},
            language = {en},
            title = {Mass gap, topological molecules, and strong gauge dynamics},
            publisher = {Perimeter Institute for Theoretical Physics},
            year = {2012},
            month = {mar},
            note = {PIRSA:12030113 see, \url{https://scivideos.org/index.php/pirsa/12030113}}
          }

Mithat Unsal San Francisco State University

Talk numberPIRSA:12030113
DOI10.48660/12030113
Source RepositoryPIRSA
Collection
Talk Type Scientific Series

Abstract

Mass, a concept familiar to all of us, is also one of the deepest
mysteries in nature.  Almost all of the mass in the visible universe,
you, me and any other stuff  that we see around us, emerges from a
quantum field theory, called QCD, which  has a completely negligible
microscopic mass content. How does QCD and the family of gauge
theories it belongs to  generate a mass?

This class of non-perturbative problems remained largely elusive despite much
effort over the years. Recently, new ideas based on compactification have been
shown useful to address some of these. Two such inter-related ideas are circle
compactifications, which avoid  phase transitions and  large-N volume
independence. Through the first one, we realized the existence of a
large-class of  "topological molecules", e.g. magnetic bions, which
generate mass gap in a class of compactified gauge theories. The inception of the
second, the idea  of  large-N volume independence is old. The new
progress is the realization of its first working examples. This property allows us to
map a four dimensional gauge theory (including pure Yang-Mills) to a quantum  mechanics at large-N.