The removal of the debugging code should also be in the commit message.

Cheers,

Edward



On 19 June 2014 20:52,  <[email protected]> wrote:
> Author: tlinnet
> Date: Thu Jun 19 20:52:53 2014
> New Revision: 24169
>
> URL: http://svn.gna.org/viewcvs/relax?rev=24169&view=rev
> Log:
> Made the function use the new multidimensional R_mat matrix.
>
> Systemtest: test_tp02_data_to_ns_r1rho_2site
> still passes.
>
> 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_r1rho_2site.py
>
> Modified: branches/disp_spin_speed/lib/dispersion/ns_r1rho_2site.py
> URL: 
> http://svn.gna.org/viewcvs/relax/branches/disp_spin_speed/lib/dispersion/ns_r1rho_2site.py?rev=24169&r1=24168&r2=24169&view=diff
> ==============================================================================
> --- branches/disp_spin_speed/lib/dispersion/ns_r1rho_2site.py   (original)
> +++ branches/disp_spin_speed/lib/dispersion/ns_r1rho_2site.py   Thu Jun 19 
> 20:52:53 2014
> @@ -136,17 +136,7 @@
>                  # Loop over the time points, back calculating the R2eff 
> values.
>                  for j in range(num_points_i):
>                      # The matrix that contains all the contributions to the 
> evolution, i.e. relaxation, exchange and chemical shift evolution.
> -                    rr1rho_3d(matrix=matrix, R1=r1_i, 
> r1rho_prime=r1rho_prime_i[j], pA=pA, pB=pB, wA=dA, wB=dB, 
> w1=spin_lock_fields_i[j], k_AB=k_AB, k_BA=k_BA)
> -
> -                    matrix_time = matrix*relax_time_i[j]
> -
>                      R_mat_i = R_mat[0, si, mi, oi, j]
> -                    diff = matrix_time - R_mat_i
> -                    if abs(sum(diff)) > 1.0e-13:
> -                        print sum(diff)
> -                        import sys
> -                        sys.exit()
> -
>
>                      # The following lines rotate the magnetization previous 
> to spin-lock into the weff frame.
>                      theta = atan2(spin_lock_fields_i[j], dA)
> @@ -154,7 +144,7 @@
>                      M0[2] = cos(theta)    # The A state initial Z 
> magnetisation.
>
>                      # This matrix is a propagator that will evolve the 
> magnetization with the matrix R.
> -                    Rexpo = matrix_exponential(matrix_time)
> +                    Rexpo = matrix_exponential(R_mat_i)
>
>                      # Magnetization evolution.
>                      MA = dot(M0, dot(Rexpo, M0))
>
>
> _______________________________________________
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>
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