Understand
In the first part of this paper, we present a set of simple arguments to show that the two-dimensional gauge anomaly and the (2+1)-dimensional Lorentz symmetry determine the leading Gaussian term in the vacuum wave function of (2+1)-dimensional Yang-Mills theory.
- This is to highlight the robustness of the wave function and its relative insensitivity to the choice of regularizations.
- We then comment on the correspondence with the explicit calculations done in earlier papers.
- We also make some comments on the nature of the gauge-invariant configuration space for Euclidean three-dimensional gauge fields (relevant to (3+1)-dimensional Yang-Mills theory).
Built on
Nothing clear enough to list yet.
Similar
Nothing clear enough to list yet.
Then
Nothing clear enough to list yet.
Beyond the bibliography
alphaXiv searches the wider corpus for related work and actual follow-ups.
alphaXiv is searching for related work…