relax SVN archive

The relax_disp.select_model user function now checks for the compiled C module when required.

Merged revisions 19498 via svnmerge from
svn+ssh://bugman@.../svn/relax/trunk

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r19498 | bugman | 2013-04-19 22:13:09 +0200 (Fri, 19 Apr 2013) | 3 lines

Renamed the new lib.stats module to lib.statistics.
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Merged revisions 19496 via svnmerge from
svn+ssh://bugman@.../svn/relax/trunk

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r19496 | bugman | 2013-04-19 20:08:05 +0200 (Fri, 19 Apr 2013) | 3 lines

The Monte Carlo error_analysis() function now handles dictionary type parameters.
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Renamed the new lib.stats module to lib.statistics.

The R2eff model now works for the variable time relaxation period and exponential curve-fitting.

The Monte Carlo error_analysis() function now handles dictionary type parameters.

Merged revisions 19494 via svnmerge from
svn+ssh://bugman@.../svn/relax/trunk

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r19494 | bugman | 2013-04-19 19:52:10 +0200 (Fri, 19 Apr 2013) | 7 lines

Shifted the standard deviation code from the Monte Carlo error_analysis() function to the lib package.

The new function lib.stats.std() is now used to simplify the error_analysis() function and allow the
code to be reused. This will be useful for expanding the pipe_control.monte_carlo.error_analysis()
function to handle parameters which are dictionaries, for example as in the relax_disp branch.
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Shifted the standard deviation code from the Monte Carlo error_analysis() function to the lib package.

The new function lib.stats.std() is now used to simplify the error_analysis() function and allow the
code to be reused. This will be useful for expanding the pipe_control.monte_carlo.error_analysis()
function to handle parameters which are dictionaries, for example as in the relax_disp branch.

The relaxation dispersion auto-analysis is now created plots of the exponential curves.

Created the relax_disp.plot_exp_curves user function.

This is to be used to create 2D graphs of the exponential curves (relaxation time verses peak
intensity) as the grace.write user function plots are not very nice - the curves from each
spectrometer field strength and dispersion point are mixed into one curve.