Abstract:We propose a new spectral method for solving multi-dimensional second order elliptic equations with varying coefficients in the whole space. This method employs an orthogonal family of quasi-rational functions recently discovered by Arar and Boulmezaoud. After proving an error estimate, we present some computational tests which demonstrate the efficiency of the method and the significance of its developmental potential.
“…Let 𝜋 N be the orthogonal projector on H N with respect to the scalar product associated to the norm |.| W 1 0 (R 3 ) . The following result is due to Boulmezaoud et al [35]:…”
Section: Convergence Of the Methods And Error Estimatementioning
confidence: 86%
“…which is equivalent to the norm ||.|| W 1 0 (R 3 ) . The following lemma will play a prominent role in the sequel (see Arar & Boulmezaoud [34] and Boulmezaoud et al [35]):…”
Section: The First Main Result: the Formulasmentioning
confidence: 99%
“…In the three-dimensional situation (the only one that interests us here), special functions we need here are defined as follows (see Arar & Boulmezaoud [34] and Boulmezaoud et al [35]): for any 𝛼 ∈ Λ…”
Section: A Family Of Special Functions An Overviewmentioning
confidence: 99%
“…This is a general property as it is announced in the following proposition which summarizes some useful properties of the functions (W 𝛼 ) 𝛼∈Λ . We refer to Arar and Boulmezaoud [34] and Boulmezaoud et al [35] for the proofs.…”
Section: Its Inverse Is Given Bymentioning
confidence: 99%
“…where (W 𝛼 ) 𝛼 designates a special family of multidimensional functions introduced in Arar and Boulmezaoud [34] and in Boulmezaoud et al [35] (these functions will be presented along with their properties in Section 2). The index sets Λ k , k ⩾ 0, are defined hereafter by (16).…”
The primary aim of this paper is the derivation and a proof of a simple and tractable formula for the stray field energy in micromagnetic problems. The formula is based on an expansion in terms of a special family of recently discovered functions. It remains valid even if the magnetization is not of constant magnitude or if the sample is not geometrically bounded. The paper continues with a direct and important application which consists in a fast summation technique of the stray field energy. The convergence of this method is established, and its efficiency is proved by various numerical experiments.
“…Let 𝜋 N be the orthogonal projector on H N with respect to the scalar product associated to the norm |.| W 1 0 (R 3 ) . The following result is due to Boulmezaoud et al [35]:…”
Section: Convergence Of the Methods And Error Estimatementioning
confidence: 86%
“…which is equivalent to the norm ||.|| W 1 0 (R 3 ) . The following lemma will play a prominent role in the sequel (see Arar & Boulmezaoud [34] and Boulmezaoud et al [35]):…”
Section: The First Main Result: the Formulasmentioning
confidence: 99%
“…In the three-dimensional situation (the only one that interests us here), special functions we need here are defined as follows (see Arar & Boulmezaoud [34] and Boulmezaoud et al [35]): for any 𝛼 ∈ Λ…”
Section: A Family Of Special Functions An Overviewmentioning
confidence: 99%
“…This is a general property as it is announced in the following proposition which summarizes some useful properties of the functions (W 𝛼 ) 𝛼∈Λ . We refer to Arar and Boulmezaoud [34] and Boulmezaoud et al [35] for the proofs.…”
Section: Its Inverse Is Given Bymentioning
confidence: 99%
“…where (W 𝛼 ) 𝛼 designates a special family of multidimensional functions introduced in Arar and Boulmezaoud [34] and in Boulmezaoud et al [35] (these functions will be presented along with their properties in Section 2). The index sets Λ k , k ⩾ 0, are defined hereafter by (16).…”
The primary aim of this paper is the derivation and a proof of a simple and tractable formula for the stray field energy in micromagnetic problems. The formula is based on an expansion in terms of a special family of recently discovered functions. It remains valid even if the magnetization is not of constant magnitude or if the sample is not geometrically bounded. The paper continues with a direct and important application which consists in a fast summation technique of the stray field energy. The convergence of this method is established, and its efficiency is proved by various numerical experiments.
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