Hi,

It does look like there is a bug somewhere in one version of
numpy.dot().  I'll look into this!

Regards,

Edward



On 15 June 2014 16:43, Troels Emtekær Linnet <[email protected]> wrote:
> I am using 1.8
>
> I am stopping here with more search for this holy grail.
>
> There is clearly some bug somewhere.
>
>
> 2014-06-15 16:25 GMT+02:00 Edward d'Auvergne <[email protected]>:
>
>> Which numpy version are you using?  There is a damn good reason why I
>> am pushing this.  I know that all of the competition software (at
>> least cpmg_fit and CATIA) uses exactly this storage concept, though in
>> C rather than Python, and for exactly the reason why I am pushing
>> this.  We really have to get this working for you!
>>
>> Regards,
>>
>> Edward
>>
>>
>>
>> On 15 June 2014 16:21, Troels Emtekær Linnet <[email protected]>
>> wrote:
>> > Hi Ed.
>> >
>> > I can see that you are pushing for this.
>> >
>> > It wont work!
>> >
>> >
>> >
>> > 2014-06-15 16:12 GMT+02:00 Edward d'Auvergne <[email protected]>:
>> >>
>> >> Hi Troels,
>> >>
>> >> In this change, only in one line have you used the numpy.dot() out
>> >> argument:
>> >>
>> >> +                dot(Rexpo, r180x, evolution_matrix)
>> >>
>> >> So it must be working.  You can do this for all others, replacing:
>> >>
>> >> -                evolution_matrix = dot(evolution_matrix, Rexpo)
>> >> +                 dot(evolution_matrix, Rexpo, evolution_matrix)
>> >>
>> >> and:
>> >>
>> >> -                evolution_matrix = dot(evolution_matrix,
>> >> evolution_matrix)
>> >> +                dot(evolution_matrix, evolution_matrix,
>> >> evolution_matrix)
>> >>
>> >> and:
>> >>
>> >> -                    Mint = evolution_matrix.dot(Mint)
>> >> +                    dot(evolution_matrix, Mint, Mint)
>> >>
>> >> This should give an observable speed increase of 2 or more.
>> >>
>> >> Regards,
>> >>
>> >> Edward
>> >>
>> >>
>> >> On 15 June 2014 15:15,  <[email protected]> wrote:
>> >> > Author: tlinnet
>> >> > Date: Sun Jun 15 15:15:23 2014
>> >> > New Revision: 23963
>> >> >
>> >> > URL: http://svn.gna.org/viewcvs/relax?rev=23963&view=rev
>> >> > Log:
>> >> > Made the dot evolution structure faster for NS CPMG 2site 3D.
>> >> >
>> >> > 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=23963&r1=23962&r2=23963&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 Sun
>> >> > Jun
>> >> > 15 15:15:23 2014
>> >> > @@ -54,7 +54,7 @@
>> >> >  """
>> >> >
>> >> >  # Python module imports.
>> >> > -from numpy import dot, fabs, isfinite, log, min, sum
>> >> > +from numpy import asarray, dot, fabs, isfinite, log, min, sum
>> >> >  from numpy.ma import fix_invalid, masked_where
>> >> >
>> >> >
>> >> > @@ -141,6 +141,9 @@
>> >> >              # The matrix R that contains all the contributions to
>> >> > the
>> >> > evolution, i.e. relaxation, exchange and chemical shift evolution.
>> >> >              R = rcpmg_3d(R1A=r10a, R1B=r10b, R2A=R2A_si_mi,
>> >> > R2B=R2B_si_mi, pA=pA, pB=pB, dw=dw_si_mi, k_AB=k_AB, k_BA=k_BA)
>> >> >
>> >> > +            # The essential evolution matrix. This initialises the
>> >> > structure.
>> >> > +            evolution_matrix = asarray(R) * 0.0
>> >> > +
>> >> >              # Loop over the time points, back calculating the R2eff
>> >> > values.
>> >> >              for di in range(num_points_si_mi):
>> >> >                  # Extract the values from the higher dimensional
>> >> > arrays.
>> >> > @@ -155,12 +158,18 @@
>> >> >                  # This matrix is a propagator that will evolve the
>> >> > magnetization with the matrix R for a delay tcp.
>> >> >                  Rexpo = matrix_exponential(R*tcp_si_mi_di)
>> >> >
>> >> > -                # Temp matrix.
>> >> > -                t_mat =
>> >> >
>> >> > Rexpo.dot(r180x).dot(Rexpo).dot(Rexpo).dot(r180x).dot(Rexpo).dot(Rexpo).dot(r180x).dot(Rexpo).dot(Rexpo).dot(r180x).dot(Rexpo)
>> >> > +                # The essential evolution matrix.
>> >> > +                # This is the first round.
>> >> > +                dot(Rexpo, r180x, evolution_matrix)
>> >> > +                evolution_matrix = dot(evolution_matrix, Rexpo)
>> >> > +                # The second round.
>> >> > +                evolution_matrix = dot(evolution_matrix,
>> >> > evolution_matrix)
>> >> > +                # The third and fourth round,
>> >> > +                evolution_matrix = dot(evolution_matrix,
>> >> > evolution_matrix)
>> >> >
>> >> >                  # Loop over the CPMG elements, propagating the
>> >> > magnetisation.
>> >> >                  for j in range(power_si_mi_di/2):
>> >> > -                    Mint = t_mat.dot(Mint)
>> >> > +                    Mint = evolution_matrix.dot(Mint)
>> >> >
>> >> >                  # The next lines calculate the R2eff using a
>> >> > two-point
>> >> > approximation, i.e. assuming that the decay is mono-exponential.
>> >> >                  Mx = Mint[1] / pA
>> >> >
>> >> >
>> >> > _______________________________________________
>> >> > relax (http://www.nmr-relax.com)
>> >> >
>> >> > This is the relax-commits mailing list
>> >> > [email protected]
>> >> >
>> >> > To unsubscribe from this list, get a password
>> >> > reminder, or change your subscription options,
>> >> > visit the list information page at
>> >> > https://mail.gna.org/listinfo/relax-commits
>> >>
>> >> _______________________________________________
>> >> relax (http://www.nmr-relax.com)
>> >>
>> >> This is the relax-devel mailing list
>> >> [email protected]
>> >>
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>> >
>> >
>
>

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