Sign conjecture for Hardy inequalities in globally twisted waveguides

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Let Ω\Omega be a globally twisted waveguide with twist derivative θ˙=β+ε\dot\theta=\beta+\varepsilon, where β\beta is the constant twisting rate and ε\varepsilon is a nonzero perturbation vanishing at infinity. Let −ΔDΩ-\Delta_D^{\Omega} be the Dirichlet Laplacian and let λ1\lambda_1 be the lowest eigenvalue of the transverse operator −ΔDω−β2∂τ2-\Delta_D^\omega-\beta^2\partial_\tau^2. A Hardy inequality is an estimate of the form

−ΔDΩ−λ1≥ρ(⋅),-\Delta_D^{\Omega}-\lambda_1\geq\rho(\cdot),

with a non-trivial function ρ:R→[0,∞)\rho:\mathbb{R}\to[0,\infty). Sign conjecture. The Hardy inequality holds if βε\beta\varepsilon is non-negative and ε\varepsilon is not identically equal to zero. This would exclude discrete eigenvalues below the essential-spectrum threshold λ1\lambda_1 in this regime, opposite to the locally slowed-down twisting regime.

References

Primary source

Philippe Briet, Hiba Hammedi and David Krejcirik, “Hardy inequalities in globally twisted waveguides”, arXiv:1406.2841 (2014).

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