Abstract
We study the decomposition A=AI+ASW of a U(1) lattice gauge field into instanton and spin wave parts. The action also decomposes, A=AI+ASW+R. Here AI is a Coulomb dipole gas, ASW is a zero mass free field, and R is a higher order remainder. We study AI in detail, for d≧4, in the dilute gas case (which corresponds to the low temperature limit of the gauge field theory). We establish the leading behavior of the free energy:f ∼ e{open}-daζ. Here e{open} is the lattice spacing, a is a geometrical constant and ζ is an activity defined in terms of a small number of instanton configurations. Our methods suggest the absence of screening in the dilute dipole gas, d≧4, in contrast to Debye screening for the dilute monopole gas.
| Original language | English |
|---|---|
| Pages (from-to) | 195-212 |
| Number of pages | 18 |
| Journal | Communications in Mathematical Physics |
| Volume | 56 |
| Issue number | 3 |
| DOIs | |
| State | Published - Oct 1977 |
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