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name & dimensionality | kind | in/out | description |
---|---|---|---|
nsmax | I4B | IN | the Nside value of the map to analyse. |
nlmax | I4B | IN | the maximum l value for the analysis. |
nmmax | I4B | IN | the maximum m value for the analysis. |
iter_order | I4B | IN | the order of Jacobi iteration. Increasing that order
improves the accuracy of the final alm but increases the computation time
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map_TQU(0:12*nsmax**2-1, 1:p) | SP/ DP | INOUT | input map. p is 1 or 3 depending if temperature (T) only or temperature and polarisation (T, Q, U) are to be analysed. It will be altered on output if a mask is provided. |
alm_TGC(1:p, 0:nlmax, 0:nmmax) | SPC/ DPC | OUT | The alm values output from the analysis. p is 1 or 3 depending on whether polarisation is included or not. In the former case, the first index is (1,2,3) corresponding to (T,E,B). |
zbounds(1:2), OPTIONAL | DP | IN | section of the map on which to perform the alm
analysis, expressed in terms of
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w8ring_TQU(1:2*nsmax,1:p), OPTIONAL | DP | IN | ring weights for quadrature corrections. p is 1 for a temperature analysis and 3 for (T,Q,U). If absent, the ring weights are all set to 1. |
plm(0:,1:p), OPTIONAL | DP | IN | If this
optional matrix is passed, precomputed scalar (and tensor)
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mask(0:12*nsmax**2-1,1:q), OPTIONAL | SP/ DP | IN | pixel mask, assumed to have the same resolution (and RING ordering) as the map. The map map_TQU is multiplied by that mask before being analyzed, and will therefore be altered on output. q should be in {1,2,3}. If p=q=3, then each of the 3 masks is applied to the respective map. If p=3 and q=2, the first mask is applied to the first map, and the second mask to the second (Q) and third (U) map. If p=3 and q=1, the same mask is applied to the 3 maps. Note: the output alm are computed directly on the masked map, and are not corrected for the loss of power, correlation or leakage created by the mask. |
Analyses temperature and polarisation signals in the first 10000 pixels of map (as determined by mask). The map has an Nside of 256, and the analysis is supposed to be performed up to 512 in l and m. The resulting alm coefficients for temperature and polarisation are returned in alm. Uniform weights are assumed. In order to improve the allm accuracy, 2 Jacobi iterations are performed.
Eric Hivon 2010-06-18
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