Identify defect-anomaly interpretations of the four-dimensional class-D boundary invariant

Establish whether the difference of the three-dimensional \(\zeta\) invariants associated with the boundary restrictions of a four-dimensional class-D particle-hole symmetry can be identified with real-space defect anomalies.

Background

In four-dimensional class D, the paper relates the parity of the second Chern character to the difference ζ[C0;s]−ζ[Cπ;s]\zeta[C_0;\mathfrak s]-\zeta[C_\pi;\mathfrak s] of three-dimensional invariants of the symmetry matrices on the two boundary momentum slices. The paper also gives quasilocal odd-parity constructions and finite-range no-go results.

The authors compare these results with a real-space picture involving monopole-line-bound states and anomaly cancellation, but explicitly refrain from identifying the momentum-space invariant difference with a defect anomaly. Establishing that identification is left unresolved.

References

As in class C, we do not identify the model's symmetry action with a crystalline symmetry that simply maps each orbital to its geometric image. A general identification of the difference of $\zeta$ with real-space defect anomalies remains open.

— Symmetry-enforced topological parity: revisiting $2\mathbb{Z}$ classifications beyond cellwise symmetry actions  (2609.37106 - Shiozaki, 29 Sep 2026) in Section 7.3, \texorpdfstring{$(d,d_\tau)=(4,3)$}{(4,3)}, class D; Section 7.3.1, SPT--LSM constraints