This is a minor feature release with improvements to the automatic
relaxation dispersion protocol for repeated CPMG data, support for
Monte Carlo or Bootstrap simulating RDC and PCS Q factors, a huge
speedup of Monte Carlo simulations in the N-state model analysis, and
geometric mean and standard deviation functions added to the relax
library.

For the official, easy to navigate release notes, please see
http://wiki.nmr-relax.com/Relax_3.3.9.

The new relax versions can be downloaded from
http://www.nmr-relax.com/download.html. If binary distributions are
not yet available for your platform and you manage to compile the
binary modules, please consider contributing these to the relax
project (described in section 3.6 of the relax manual,
http://www.nmr-relax.com/manual/relax_distribution_archives.html).

The full list of changes is:

    Features:
        * Improvements to the automatic relaxation dispersion protocol
for repeated CPMG data.
        * Support for Monte Carlo or Bootstrap simulating the RDC and
PCS Q factors.
        * Huge speedup of Monte Carlo simulations in the N-state model analysis.
        * Geometric mean and standard deviation functions added to the
relax library.


    Changes:
        * Wrote a method to store parameter data and dispersion
curves, for the protocol of repeated CPMG analysis.  This is to
prepare for analysis in other programs.  The method loops through the
data pipes, and writes the data out.  It then writes a bash script
that will concatenate the data in an matrix array style, for reading
and processing in other programs.  Task #7826
(https://gna.org/task/?7826): Write an Python class for the repeated
analysis of dispersion data.
        * Added to write out a collection script for chi2 and rate
parameters.  Task #7826 (https://gna.org/task/?7826): Write an Python
class for the repeated analysis of dispersion data.
        * In the collection bash script, removes spins which have not
been fitted.  Task #7826 (https://gna.org/task/?7826): Write an Python
class for the repeated analysis of dispersion data.
        * Fix for use of " instead of ' in bash script.  Task #7826
(https://gna.org/task/?7826): Write an Python class for the repeated
analysis of dispersion data.
        * Adding option to minimise class function, to perform Monte
Carlo error analysis.  Task #7826 (https://gna.org/task/?7826): Write
an Python class for the repeated analysis of dispersion data.
        * Printout when minimising Monte Carlo simulations.  Task
#7826 (https://gna.org/task/?7826): Write an Python class for the
repeated analysis of dispersion data.
        * Added additional test to system test
Relax_disp.test_bug_23186_cluster_error_calc_dw() to prove that Bug
#23619 is invalid.  Bug #23619:
(https://gna.org/bugs/index.php?23619): Stored chi2 sim values from
Monte Carlo simulations does not equal normal chi2 values.
        * Small fix for the shell script to collect data files, and
not use the program "column" in the end.  The line width becomes to
large to handle for column.  Task #7826 (https://gna.org/task/?7826):
Write an Python class for the repeated analysis of dispersion data.
        * Added a unit test that triggers the bug.  Test added in
test_delete_spin_all, and can be accessed with: relax -u
_pipe_control.test_spin.  Bug #23642
(https://gna.org/bugs/index.php?23642): When deleting all spins for a
residue, an empty placeholder is where select=True.
        * Added sample data and analysis script, that will eventually
show that there is not much difference in the sample statistics used
for comparing the output of two very similar datasets.  This is a
multiple comparison test with many T-tests at once, where the
familywise error is controlled by the Holm method.  Even if the values
are close to equal, and within the standard deviation, this procedure
will reject up to 20% of the null hypothesis.  This is not deemed as a
suitable method.  Bug #23644 /https://gna.org/bugs/?23644):
monte_carlo.error_analysis() does not update the mean
value/expectation value from simulations.
        * Added Monte Carlo simulations to the
N_state_model.test_absolute_T system test.  This is to demonstrate a
failure of the simulations in certain N-state model setups.
        * Added a missing call to monte_carlo.initial_values in the
N_state_model.test_absolute_T system test.  This fixes the
N_state_model.test_absolute_T system test, showing that there is not a
problem with the Monte Carlo simulations.
        * Added Monte Carlo and Bootstrap simulation support for the
RDC and PCS Q factor calculations.  The pipe_control.rdc.q_factors()
and pipe_control.pcs.q_factors() functions have been modified to
support Monte Carlo and Bootstrap simulations.  The sim_index argument
has been added to allow the Q factor for the given simulation number
to be calculated.  All of the Q factor data structures in the base
data pipe now have *_sim equivalents for permanently storing the
simulation values.  For the simulation values, all the warnings have
been silenced.
        * Added simulation support for the RDC and PCS Q factors in
the N-state model analysis.  This is for both Monte Carlo and
Bootstrap simulation.  The simulation RDC and PCS values, as well as
the simulation back calculated values are now stored via the
minimise_bc_data() function of
specific_analyses.n_state_model.optimisation in the respective spin or
interatomic data containers. The analysis specific API methods now
send the sim_index value into minimise_bc_data(), as well as the
pipe_control.rdc.q_factors() and pipe_control.pcs.q_factors()
functions.
        * Silenced a warning in the N-state model optimisation if the
verbosity is set to zero.  This removes a repetitive warning from the
Monte Carlo or Bootstrap simulations.
        * Huge speed up for the Monte Carlo simulations in the N-state
model analyses.  This speed up is also for Bootstrap simulations and
the frame order analysis.  The change affects the
monte_carlo.initial_values user function.  The alignment tensor
_update_object() method was very inefficient when updating the Monte
Carlo simulation data structures.  For each simulation, each of the
alignment tensor data structures were being updated for all
simulations.  Now only the current simulations is being updated.  This
speeds up the user function by many orders of magnitude.
        * Added functions for calculating the geometric mean and
standard deviation to the relax library.  These are the
geometric_mean() and geometric_std() functions of the lib.statistics
module.  The implementation is designed to be fast, using numpy array
arithmetic rather than Python loops.
        * Created a simple unit test for the new
lib.statistics.geometric_mean() function.
        * Added a unit test for the new lib.statistics.geometric_std() function.
        * Made a summarize function to compare results.  Task #7826
(https://gna.org/task/?7826): Write an Python class for the repeated
analysis of dispersion data.


    Bugfixes:
        * Fix committed, where an empty spin placeholder has the
select flag set to False.  Bug #23642
(https://gna.org/bugs/index.php?23642): When deleting all spins for a
residue, an empty placeholder is where select=True.

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