Abstract
We show that when the induced parity breaking part of the effective action for the low-momentum region of U(1) × ⋯ × U(1) Maxwell gauge field theory with massive fermions in 3 dimensions is coupled to a φ4 scalar field theory, it is not possible to eliminate the screening of the long-range Coulomb interactions and get external charges confined in the broken Higgs phase. This result is valid for non-zero temperature as well.
| Original language | English |
|---|---|
| Pages (from-to) | 112-116 |
| Number of pages | 5 |
| Journal | Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics |
| Volume | 445 |
| Issue number | 1-2 |
| DOIs | |
| Publication status | Published - 31 Dec 1998 |
| Externally published | Yes |
Keywords
- Chern-Simons
- Confinement
- Finite temperature field theory
- Screening
- Spontaneous symmetry breaking