Abstract
Using a hopping parameter expansion, we demonstrate the decoupling of fermion doubler modes in the hypercharge U(1)Y lattice gauge theory. We also show analytically that it is possible to tune the bare Yukawa coupling to a value such that the fundamental physical fermion amf=0 (as is necessary in order to obtain a finite physical mass mf in the continuum limit), and we calculate this value. The appropriate special case of these results is compared with numerical simulations of the frozen-gauge limit of the U(1)Y theory, and good agreement is found. The role of the Yukawa coupling in a chiral lattice gauge theory is contrasted with that in a nonchiral Yukawa model.
| Original language | English |
|---|---|
| Pages (from-to) | 383-421 |
| Number of pages | 39 |
| Journal | Nuclear Physics, Section B |
| Volume | 355 |
| Issue number | 2 |
| DOIs | |
| State | Published - May 20 1991 |
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