Author: tlinnet
Date: Thu Jun 19 17:41:51 2014
New Revision: 24154
URL: http://svn.gna.org/viewcvs/relax?rev=24154&view=rev
Log:
Added intermediate step with for loops.
Task #7807 (https://gna.org/task/index.php?7807): Speed-up of dispersion
models for Clustered analysis.
Modified:
branches/disp_spin_speed/lib/dispersion/ns_cpmg_2site_3d.py
Modified: branches/disp_spin_speed/lib/dispersion/ns_cpmg_2site_3d.py
URL:
http://svn.gna.org/viewcvs/relax/branches/disp_spin_speed/lib/dispersion/ns_cpmg_2site_3d.py?rev=24154&r1=24153&r2=24154&view=diff
==============================================================================
--- branches/disp_spin_speed/lib/dispersion/ns_cpmg_2site_3d.py (original)
+++ branches/disp_spin_speed/lib/dispersion/ns_cpmg_2site_3d.py Thu Jun 19
17:41:51 2014
@@ -131,6 +131,25 @@
# The matrix R that contains all the contributions to the evolution,
i.e. relaxation, exchange and chemical shift evolution.
R_mat = rcpmg_3d_rankN(R1A=r10a, R1B=r10b, R2A=r20a, R2B=r20b, pA=pA,
pB=pB, dw=dw, k_AB=k_AB, k_BA=k_BA, tcp=tcp)
+ # Holds the Rexpo.
+ Rexpo_mat = R_mat * 0.0
+ # Loop over the spins
+ for si in range(NS):
+ # Loop over the spectrometer frequencies.
+ for mi in range(NM):
+ # Extract number of points.
+ num_points_si_mi = int(num_points[0, si, mi, 0])
+
+ # Loop over the time points, back calculating the R2eff values.
+ for di in range(num_points_si_mi):
+
+ # This matrix is a propagator that will evolve the
magnetization with the matrix R for a delay tcp.
+ R_mat_i = R_mat[0, si, mi, 0, di]
+
+ # Store the Rexpo. Is it not possible to find the matrix
exponential of higher dimensional data?
+ Rexpo = matrix_exponential(R_mat_i)
+ Rexpo_mat[0, si, mi, 0, di] = Rexpo
+
# Loop over the spins
for si in range(NS):
# Loop over the spectrometer frequencies.
@@ -150,9 +169,7 @@
Mint = M0
# This matrix is a propagator that will evolve the
magnetization with the matrix R for a delay tcp.
- R_mat_i = R_mat[0, si, mi, 0, di]
-
- Rexpo = matrix_exponential(R_mat_i)
+ Rexpo = Rexpo_mat[0, si, mi, 0, di]
# The essential evolution matrix.
# This is the first round.
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