Commit | Date | |
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[r21368]
by
bugman
The dispersion target function num_disp_points structure is now variable. The number of points can now be different for each experiment type and each magnetic field strength. |
2013-10-31 19:50:20 | Tree |
[r21367]
by
bugman
The return_cpmg_frqs() and return_spin_lock_nu1() dispersion functions now return lists of lists of arrays. The dispersion data structures are now experiment and spectrometer frequency dependent. Therefore |
2013-10-31 19:35:54 | Tree |
[r21366]
by
bugman
Conversion of the format of the relaxation dispersion R2eff/R1rho data structures. These are now lists of lists of lists of numpy arrays instead of pure numpy rank-4 arrays. This |
2013-10-31 18:49:54 | Tree |
[r21365]
by
bugman
Better MMQ data support for the dispersion specific loop_cluster() function. For the models using proton-heteronuclear multi-multiple quantum data, proton spin containers are |
2013-10-31 14:46:20 | Tree |
[r21364]
by
bugman
Merged revisions 21363 via svnmerge from ........ |
2013-10-31 14:30:49 | Tree |
2013-10-31 14:30:11 | Tree | |
2013-10-31 11:09:53 | Tree | |
[r21361]
by
bugman
Merged revisions 21359-21360 via svnmerge from ........ |
2013-10-31 10:21:49 | Tree |
2013-10-31 10:20:23 | Tree | |
2013-10-31 10:18:16 | Tree |