Abstract
In this second paper of the series, the details are given of the calculation of the bare activity of the meron pairs described in the first paper. The instanton limit is computed and found to be consistent with the discussion presented in the first paper. The bulk of the calculation for the regime of physical interest is performed using one set of constraints. An outline is given of one possible treatment of an instability in the calculation in part of this regime. A detailed analysis of this instability, a more detailed consideration of other constraint systems, and some further numerical work are left for the third paper.
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