The nullspace characterization of Bloch eigenvalues

Let EE be the linear operator in the layer-potential system for the unknown densities [η;ξ][\eta;\xi], where η=[τ;σ]\eta=[\tau;-\sigma], and let (ω,a,b)(\omega,a,b) denote the frequency and quasiperiodicity parameters. A nontrivial nullspace corresponds to a nontrivial field satisfying the matching, continuity, and quasi-periodicity conditions. Nullspace characterization conjecture. (ω,a,b)(\omega,a,b) is a Bloch eigenvalue if and only if

NullE{0}.\operatorname{Null} E \neq \{0\}.

This is presented as a stronger claim supported by numerical evidence, analogous to the preceding theorem, and its resolution is not established in the supplied text.

Sources & referencesView supporting material

Primary source

Alex H. Barnett and Leslie Greengard, “A new integral representation for quasiperiodic fields and its application to two-dimensional band structure calculations”, arXiv:1001.5464 (2010).

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