Definition. Plaquette transport and Wilson loops [fdip-006N]

Let \(G\) be a finite group on a square complex. A connection is \(U\in G^E\), with \(U_{\bar e}=U_e^{-1}\) on a reversed edge. For a traversed path \(C=(e_1^{\epsilon _1},\ldots ,e_k^{\epsilon _k})\), define \[U_C=U_{e_k}^{\epsilon _k}\cdots U_{e_1}^{\epsilon _1}.\] The first transport acts on the right. The plaquette holonomy is \(U_p=U_{\partial p}\). The gauge group \(\mathcal G=G^V\) acts by \[(gU)_e=g_{h(e)}U_eg_{s(e)}^{-1}.\] Cancellation at successive vertices gives \[(gU)_C=g_{h(C)}U_Cg_{s(C)}^{-1}.\] For a closed path based at \(v\), this is conjugation by \(g_v\).

Choose a unitary representation \(\rho :G\to U(d)\) with \(d>0\), and let \(\chi _\rho (g)=\operatorname {Tr}\rho (g)\) be its character. The Wilson loop of a closed path is the unnormalized trace \[W_\rho (C)=\chi _\rho (U_C).\] It is gauge invariant. Changing the starting vertex conjugates the holonomy, so it does not change this trace. Reversing the path replaces \(U_C\) by \(U_C^{-1}\), hence replaces \(W_\rho (C)\) by its complex conjugate. In particular \(\operatorname {Re}W_\rho (C)\) is independent of the chosen boundary orientation. These are the transport and trace conventions of [wingate2025lattice, equations (6.14)–(6.19), pp. 7–8].

The arrows show the chosen edge orientations and the labels are connection values, not scalar weights. The boundary traversal is \[v_0\to v_1\to v_2\to v_3\to v_0.\] It uses the top and left edges backwards, accounting for both inverses.