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authorThomas White <taw@physics.org>2011-02-03 10:40:18 +0100
committerThomas White <taw@physics.org>2012-02-22 15:27:13 +0100
commit20e6c9e8f6055d4c98cc32f8e4dd59e6180b416c (patch)
tree84378acdacf1e8031ddebcf6f971f26dc55a0312 /src/hrs-scaling.c
parent6854d52ef4e7268d50e90ea112af73e42a34a829 (diff)
Solve the diagonalised equation the easy way
Diffstat (limited to 'src/hrs-scaling.c')
-rw-r--r--src/hrs-scaling.c18
1 files changed, 8 insertions, 10 deletions
diff --git a/src/hrs-scaling.c b/src/hrs-scaling.c
index 30af5a61..73321afb 100644
--- a/src/hrs-scaling.c
+++ b/src/hrs-scaling.c
@@ -242,21 +242,20 @@ static double iterate_scale(struct image *images, int n,
gsl_eigen_symmv_free(work);
val = gsl_eigen_symmv_sort(e_val, e_vec, GSL_EIGEN_SORT_ABS_DESC);
- /* Set up the diagonalised normal equations */
- gsl_matrix *D;
+ /* Rotate the "solution vector" */
gsl_vector *rprime;
- D = gsl_matrix_calloc(n, n);
- for ( a=0; a<n; a++ ) {
- gsl_matrix_set(D, a, a, gsl_vector_get(e_val, a));
- }
rprime = gsl_vector_alloc(n);
val = gsl_blas_dgemv(CblasTrans, 1.0, e_vec, v, 0.0, rprime);
- show_matrix_eqn(D, rprime, n);
- /* Solve */
+ /* Solve (now easy) */
gsl_vector *sprime;
sprime = gsl_vector_alloc(n);
- gsl_linalg_HH_solve(D, rprime, sprime);
+ for ( a=0; a<n-1; a++ ) {
+ double num, den;
+ num = gsl_vector_get(rprime, a);
+ den = gsl_vector_get(e_val, a);
+ gsl_vector_set(sprime, a, num/den);
+ }
gsl_vector_set(sprime, n-1, 0.0); /* Set last shift to zero */
/* Rotate back */
@@ -281,7 +280,6 @@ static double iterate_scale(struct image *images, int n,
gsl_vector_free(sprime);
gsl_matrix_free(e_vec);
gsl_vector_free(e_val);
- gsl_matrix_free(D);
gsl_matrix_free(M);
gsl_vector_free(v);