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* Add tests for symmetry of integrationhinder2013-10-09
| | | | | | 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
* Rename integration convergence test function and run tests only if ↵hinder2013-10-09
| | | | | | Multipole::enable_test = yes git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@96 4f5cb9a8-4dd8-4c2d-9bbd-173fa4467843
* Add convergence test for Simpson integration methodhinder2013-10-09
| | | | git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@94 4f5cb9a8-4dd8-4c2d-9bbd-173fa4467843
* Schedule after Accelerator_CopyBackhinder2012-04-30
| | | | git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@81 4f5cb9a8-4dd8-4c2d-9bbd-173fa4467843
* Remove single mode extraction methodhinder2010-06-13
| | | | | | | | | | | | 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
* use trunc structureknarf2010-03-26
git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@53 4f5cb9a8-4dd8-4c2d-9bbd-173fa4467843