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* Make trapezoidal integration method available via parameterhinder2013-10-09
| | | | git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@98 4f5cb9a8-4dd8-4c2d-9bbd-173fa4467843
* Implement Driscoll&Healy integrationeschnett2012-06-16
| | | | | | | | | Implements a more accurate integration over the sphere using an algorithm by Driscoll & Healy. This algorithm uses Gaussian integration weights, leading (almost) to exponential convergence. git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@83 4f5cb9a8-4dd8-4c2d-9bbd-173fa4467843
* Add HDF5 output supporthinder2011-01-03
| | | | | | One HDF5 file per variable, and one extensible dataset per radius per mode. HDF5 is required only optionally, so this thorn can be compiled without it. git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@74 4f5cb9a8-4dd8-4c2d-9bbd-173fa4467843
* Use IO::out_dir parameter by sharing from implementation rather than via ↵hinder2011-01-03
| | | | | | CCTK_ParameterGet git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@73 4f5cb9a8-4dd8-4c2d-9bbd-173fa4467843
* Change default interpolator parameters to disable off-centering of stencilhinder2010-11-15
| | | | | | | | | | | | | | | AEILocalInterp by default will off-centre the interpolation stencil if there are insufficient points to perform the interpolation. In a parallel setting, this could happen due to there being insufficient ghost points for the interpolator chosen. The off-centering leads to an interpolation error which is of the correct order but larger than for a centered stencil. More importantly, it leads to different results on different numbers of processes. With this commit, Multipole will (by default) disable off-centering in the interpolator. git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@68 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
* 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
* use trunc structureknarf2010-03-26
git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/Multipole/trunk@53 4f5cb9a8-4dd8-4c2d-9bbd-173fa4467843