2023
DOI: 10.1007/s00013-023-01898-3
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Strichartz estimates for Maxwell equations in media: the structured case in two dimensions

Robert Schippa,
Roland Schnaubelt

Abstract: We prove Strichartz estimates for the two dimensional Maxwell equations with diagonal Lipschitz permittivity of special structure. The estimates have no loss in regularity that occurs in general for $$C^1$$ C 1 -coefficients. In the charge-free case, we recover Strichartz estimates local-in-time for Euclidean wave equations in two dimensions up to endpoints.

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Cited by 2 publications
(2 citation statements)
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“…It appears that in the present work the role of the Half-Laplacian is explicitly identified for the analysis of the Maxwell operator the first time. We note that in [27,28], in joint work with R. Schnaubelt, we apply a similar diagonalization to show Strichartz estimates for time-dependent Maxwell's equations with rough coefficients. In these works, due to variable permittivity and permeability, the diagonalization is carried out with pseudo-differential operators, and the present role of the Half-Laplacian is played by the Half-Wave operator.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…It appears that in the present work the role of the Half-Laplacian is explicitly identified for the analysis of the Maxwell operator the first time. We note that in [27,28], in joint work with R. Schnaubelt, we apply a similar diagonalization to show Strichartz estimates for time-dependent Maxwell's equations with rough coefficients. In these works, due to variable permittivity and permeability, the diagonalization is carried out with pseudo-differential operators, and the present role of the Half-Laplacian is played by the Half-Wave operator.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…are L p -bounded for 1 < p < ∞ with a constant only depending on p, ε, μ as the symbols are linear combinations of Riesz symbols after changes of variables. We find (see (27) for notations)…”
Section: Proof Of Theorem 11 D=2mentioning
confidence: 95%