Abstract
In the absence of any forcing and rotational effects, the 1D linearized Boussinesq’s equation for the evolution of a surface gravity wave propagating in a random bottom has been studied. The time-dependent evolution of plane-wave-like modes of gravity waves in the presence of weak disorder and for Fourier number outside the localized gap are shown to be well approximated by monochromatic telegrapher’s waves. For strong disorder the one-to-one correspondence for any Fourier number has been revisited (Cáceres in AIP Adv 11:045218, 2021).
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Notes
Space stationary in the sense that any \(n-\)moment of the random field \(\xi \left( x\right) \) fulfills translational invariance: \(\left\langle \xi \left( x_{1}-X\right) \xi \left( x_{2}-X\right) \cdots \xi \left( x_{n-1}-X\right) \xi \left( x_{n}-X\right) \right\rangle \) \( =\left\langle \xi \left( x_{1}\right) \xi \left( x_{2}\right) \cdots \xi \left( x_{n-1}\right) \xi \left( x_{n}\right) \right\rangle ,\forall X\). We note here that for the present symmetric binary disorder any \(2n-\)moment breaks in the form: \(\left\langle \xi \left( x_{1}\right) \xi \left( x_{2}\right) \right\rangle \cdots \left\langle \xi \left( x_{2n-1}\right) \xi \left( x_{2n}\right) \right\rangle \) if the sequence is ordered: \( x_{2}\ge \cdots \ge x_{2n-1}\ge x_{2n}\). This is the key ingredient to prove that Terwiel’s cumulants, for the present binary disorder, cancel for order higher than the second one, see [14].
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Acknowledgements
M.O.C. thanks to funding provided by CONICET (Grant no. PIP 112-201501-00216, CO), and Grant: Secretaría de Ciencia Técnica y Postgrado: 06/C565. U. N. Cuyo (2019).
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Cáceres, M.O. Localization of gravity waves on a random floor: weak and strong disorder analysis. Eur. Phys. J. Spec. Top. 231, 513–519 (2022). https://doi.org/10.1140/epjs/s11734-021-00401-9
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DOI: https://doi.org/10.1140/epjs/s11734-021-00401-9