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* Remove default fallback value for "variables" stringhinder2010-09-10
| | | | | | | Now if no variables are supplied, none will be decomposed git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@66 4f5cb9a8-4dd8-4c2d-9bbd-173fa4467843
* Corrects parameter ranges and their descriptioneschnett2010-06-15
| | | | git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@63 4f5cb9a8-4dd8-4c2d-9bbd-173fa4467843
* Fix 1D output filename in the case that the variable to be decomposed is realhinder2010-06-14
| | | | git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@60 4f5cb9a8-4dd8-4c2d-9bbd-173fa4467843
* Add testing code for making grid function harmonic coefficient proportional ↵hinder2010-06-14
| | | | | | to radius git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@58 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
* Remove debugging printf statementshinder2010-06-13
| | | | git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@55 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