Quantum-layer bound-state conjecture for integrable Gauss curvature

Let Σ\varSigma be a complete, noncompact surface embedded in R3\mathbb R^3 satisfying the preceding hypotheses, and let κ\kappa be its Gauss curvature. Assume

ΣκdΣ<+.\int_\varSigma |\kappa|\,d\varSigma<+\infty.

Quantum-layer bound-state conjecture. There exists α=α(Σ)\alpha=\alpha(\varSigma) such that, for every a(0,α)a\in(0,\alpha), the discrete spectrum of the quantum layer over Σ\varSigma of width 2a2a is non-empty. This conjecture was proved under the condition ΣκdΣ0\int_\varSigma\kappa\,d\varSigma\leq0 through work of Duclos, Exner and Krejčiřík and of Carron, Exner and Krejčiřík; the remaining positive-total-curvature case is addressed by later results in the paper.

Sources & referencesView supporting material

Primary source

Zhiqin Lu and Julie Rowlett, “On the discrete spectrum of quantum layers”, arXiv:1110.6807 (2012).

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