2011
DOI: 10.1007/s13137-010-0011-9
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Spherical decompositions in a global and local framework: theory and an application to geomagnetic modeling

Abstract: This paper gives an overview on decompositions of vector fields on the sphere that are of importance in geoscientific modeling. Various versions of the Mie and Helmholtz decomposition are presented. A special emphasis is set to integral representations for the different contributions, which is of interest, e.g., in numerical applications. Furthermore, the decompositions are treated in a global framework on the entire sphere and in a local framework on regular subsurfaces. In the end, an application to the mode… Show more

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Cited by 37 publications
(25 citation statements)
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“…In order to be able to obtain a spherical version of Theorem 1.4(c), we reformulate the decomposition of Theorem 2.1 in terms of a set of pseudo-differential operatorsõ (1) ,õ (2) ,õ (3) as indicated in [8,10,11,12]. More precisely, 12) where D denotes the pseudo-differential operator…”
Section: Operator Representationmentioning
confidence: 99%
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“…In order to be able to obtain a spherical version of Theorem 1.4(c), we reformulate the decomposition of Theorem 2.1 in terms of a set of pseudo-differential operatorsõ (1) ,õ (2) ,õ (3) as indicated in [8,10,11,12]. More precisely, 12) where D denotes the pseudo-differential operator…”
Section: Operator Representationmentioning
confidence: 99%
“…By dω we denote the surface element on the sphere Ω R . The non-uniqueness of recovering a vertically integrated magnetization m from the knowledge of V in Ω ext R can be characterized by a fairly well-known decomposition (see, e.g., [1,8,11,12,13,18,19,22]) m =m (1) +m (2) +m (3) , (1.3) which has the property that V ≡ 0 in Ω ext R if and only ifm (2) ≡ 0 (in other words, any magnetization of the form m =m (1) +m (3) produces no magnetic potential in the exterior Ω ext R ). We call such a decomposition a Hardy-Hodge decomposition (cf.…”
Section: Introductionmentioning
confidence: 99%
“…4.2 requires G . I / to be three times continuously differentiable (for more details on higher-order regularizations, the reader is referred to Gerhards (2011a) and Freeden and Gerhards (2012)). At this point it should be emphasized that G. I / and its regularization only depend on the scalar product Á, so that they can be regarded as functions acting on the interval OE 1; 1/ and OE 1; 1, respectively.…”
Section: Green's Function For the Beltrami Operatormentioning
confidence: 99%
“…In geomagnetic applications they have been used in Freeden and Gerhards (2010) and Gerhards (2011aGerhards ( , 2012.…”
Section: Green's Function For the Beltrami Operatormentioning
confidence: 99%
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