We investigate a generalization of the equation curl w→= g→ to an arbitrary number n of dimensions, which is based on the well-known Moisil–Teodorescu differential operator …
We introduce the spaces A α, β p (Ω) of L p-solutions to the Vekua equation (generalized monogenic functions) D w= α w¯+ β w in a bounded domain in R n, where D=∑ i= 1 nei∂ i …
A general solution of the equation curl\, ⃗ w+ λ ⃗ w= ⃗ g,\, λ ∈ C,\, λ ≠ 0 curl w→+ λ w→= g→, λ∈ C, λ≠ 0 is obtained for an arbitrary bounded domain Ω ⊂ R^ 3 Ω⊂ R 3 with a …
BB Delgado, A Guillén‐Villalobos… - … Methods in the …, 2023 - Wiley Online Library
In this manuscript, we characterize the kernel of the parabolic Dirac operator in an explicit way. More precisely, we will show that the members of this kernel equivalently satisfy a …
M Santacesaria - arXiv preprint arXiv:1803.06931, 2018 - arxiv.org
The unique determination of a measurable conductivity from the Dirichlet-to-Neumann map of the equation $\mathrm {div}(\sigma\nabla u)= 0$ is the subject of this note. A new strategy …
In this work, we investigate the system formed by the equations div w→= g 0 div\kern0. 3em w= g _0 and curl w→= g→ curl\kern0. 3em w= g in bounded star‐shaped domains of ℝ 3 R …
AM García, BB Delgado - Boletín de la Sociedad Matemática Mexicana, 2024 - Springer
The transmission boundary value problem for the three-dimensional Lamé–Navier system is formulated and solved in terms of surface Cauchy-type integral operators and layer …
BB Delgado, RM Porter - Topics in Clifford Analysis: Special Volume in …, 2019 - Springer
Let Ω be a bounded Lipschitz domain in ℝ 3 R^ 3. We introduce the Vekua-Hardy spaces H fp (Ω) H_f^ p (Ω) of solutions of the main Vekua equation DW=(D f∕ f) W¯ DW=(Df/f) W …
We consider functions of a vector variable in a domain in 3-dimensional space, taking values in the space of complex quaternions. Let D be the Moisil-Teodorescu differential …