Confinement, Screening, and Mass Gaps in Controlled Regimes
Confinement, screening, and a spectral mass gap are distinct properties of gauge theories. This chapter compares their observables, develops mechanisms in compact Abelian and small-circle regimes, and explains what must be established before extending a controlled example to a more general theory.
Enter this chapter
Section titled “Enter this chapter”Begin with Confinement Definitions and Their Non-Equivalence to state exactly which confinement proposition is being tested.
Helpful background. Review Coulomb, Higgs, and Confining Regimes and Gauge-Phase Diagnostics from Line Operators for gauge-invariant phase and line-operator diagnostics.
Topics
Section titled “Topics”- Confinement Definitions and Their Non-Equivalence — Separates inequivalent uses of confinement.
- Line Operators, Screening, and Generalized-Symmetry Diagnostics — Tests which genuine probes dynamical matter can screen.
- Static Potentials, Flux Tubes, and Effective Strings — Extracts static energies and long-string behavior.
- Compact U(1) in 2+1 Dimensions and the Monopole Plasma — Derives a confinement mechanism in a dilute monopole regime.
- Small-Circle Abelianization, Bions, and Adiabatic Continuity — States the assumptions behind weakly coupled compactification.
- Proposed Confinement Mechanisms and Discriminating Observables — Connects proposed mechanisms to discriminating observables.
- The Non-Abelian Mass Gap as a Spectral Statement — Defines a gap in the physical spectrum.
- Confinement Evidence, Mechanisms, and Open Problems — Separates controlled results from wider unresolved claims.
- Low-Dimensional Confinement and Screening Laboratories — Uses lower-dimensional examples to test supposed equivalences.
How the ideas fit together
Section titled “How the ideas fit together”A gap does not imply an unscreened confining force. The massless Schwinger model has a massive gauge-invariant excitation while dynamical charged matter screens external probes. Conversely, pure two-dimensional Yang–Mills theory has an area law without local propagating gauge particles. These examples show why line behavior and spectral statements require separate definitions. Controlled monopole or small-circle calculations supply mechanisms in their own regimes; extending them needs additional dynamical arguments, not just the same vocabulary. Coleman 1985, ch. 8.
Where to go next
Section titled “Where to go next”Continue to Large-N Dynamics to fix the index family, normalization, and quantities held constant.
References
Section titled “References”- Coleman, Sidney. Aspects of Symmetry: Selected Erice Lectures. Cambridge University Press, 1985, ch. 8. DOI.