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It is desirable that integrands with exact pi-antisymmetry integrate to zero; we add measures of this here. This is the case for all but the midpoint method.
git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@102 4f5cb9a8-4dd8-4c2d-9bbd-173fa4467843
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Multipole::enable_test = yes
git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@96 4f5cb9a8-4dd8-4c2d-9bbd-173fa4467843
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git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@94 4f5cb9a8-4dd8-4c2d-9bbd-173fa4467843
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git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@81 4f5cb9a8-4dd8-4c2d-9bbd-173fa4467843
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To simplfy the API, and because the common use case is to extract
multiple modes, this commit removes support for extracting only a
single mode. All modes up to l = l_max (a new parameter) are now
computed always. The old parameter l_mode is now deprecated, but if
it is used, it is a synonym for l_max. It will eventually be removed.
git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@57 4f5cb9a8-4dd8-4c2d-9bbd-173fa4467843
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git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@53 4f5cb9a8-4dd8-4c2d-9bbd-173fa4467843
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