Rigorous Wilson loop observable existence conjecture

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Let LL satisfy Assumption, and let WLO⁡rig(L)\operatorname{WLO}_{rig}(L) be the regularized Wilson loop observable defined by

WLO⁡rig(L):=lim⁡n→∞lim⁡s→0lim⁡ϵ→0∑y∈I∫∼Ψ(Jb,y(s,ϵ,n)(L)) db.\operatorname{WLO}_{rig}(L):= \lim_{n \to \infty} \lim_{s \to 0} \lim_{\epsilon\to 0} \sum_{y \in I} \int_{\sim} \Psi\bigl( J^{(s,\epsilon,n)}_{b,y}(L)\bigr)\, db.

Here Jb,y(s,ϵ,n)(L)J^{(s,\epsilon,n)}_{b,y}(L) is the regularized integrand defined for b∈tb \in \mathfrak t, y∈Iy \in I, s∈(0,1)s \in (0,1), ϵ∈(0,ϵ(s))\epsilon \in (0,\epsilon(s)), and n∈Nn \in \mathbb N, while ∫∼\int_{\sim} denotes the mean-value integral over t\mathfrak t.

Existence conjecture. WLO⁡rig(L)\operatorname{WLO}_{rig}(L) is well-defined. In particular, all limits involved exist.

This conjecture asserts the existence of the regularized Chern–Simons Wilson loop observable obtained from the proposed infinite-dimensional path-integral construction. The source does not provide a resolution of the conjecture; its validity is used to motivate the subsequent comparison with the shadow invariant.

References

Primary source

Atle Hahn, “Infinite Dimensional Analysis and the Chern-Simons Path Integral”, arXiv:1506.06809 (2015).

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