Commit | Date | |
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[r19388]
by
bugman
The spin parameters are now set up last by the relax_disp.select_model user function back end. |
2013-04-05 15:26:34 | Tree |
[r19387]
by
bugman
Converted all relaxation dispersion parameters to lowercase. This is so the variable names match the parameter names identically, avoiding problems with some of |
2013-04-05 15:25:48 | Tree |
2013-04-05 15:02:19 | Tree | |
[r19385]
by
bugman
The relaxation dispersion parameter errors from Monte Carlo simulations are now stored. Previously MC simulations could run, but the errors were not being calculated and stored. The In addition the set_error() method has been created for setting the parameter errors. And the |
2013-04-05 14:50:23 | Tree |
2013-04-05 10:37:38 | Tree | |
[r19383]
by
bugman
Modified the Relax_disp.test_exp_fit system test to be faster and not create plots which it cannot. |
2013-04-05 10:20:44 | Tree |
[r19382]
by
bugman
Activated Monte Carlo simulations for the relaxation dispersion analysis. This required a bit of work. The key parts weres renaming _block_loop() to the API method _back_calc(): This method has been modified to handle clustering and the returning of peak intensities _exp_curve_index_from_key(): This new method is used to convert exponential curve key into the _intensity_key(): This new method is for converting an exponential curve key and relaxation time create_mc_data(): This method is now functional and handles the data from the base_data_loop() method. return_error(): This method now handles the data from the base_data_loop() method. set_selected_sim(): This new method has been modified from the common _set_selected_sim_spin() sim_pack_data(): This method now handles the data from the base_data_loop() method. sim_return_param(): This new method has been modified from the common _sim_return_param_spin() sim_return_selected(): This new method has been modified from the common |
2013-04-05 10:18:09 | Tree |
[r19381]
by
bugman
Created a custom base_data_loop() method for the relaxation dispersion analysis. This defines the base data as the peak intensities of a single exponential curve and yields the spin |
2013-04-05 07:57:42 | Tree |
[r19380]
by
bugman
Fixes for the dispersion specific _back_calc() method. This method still has a long way to go before it is of any use. |
2013-04-05 07:40:32 | Tree |
[r19379]
by
bugman
The relaxation dispersion target function class back_calc variable now matches the values variable. Instead of being a temporary structure which is overwritten for each spin and each exponential |
2013-04-05 07:29:07 | Tree |