.fio-files and folders with -.nxs-files contain raw data.
The raw data includes delay times specific to the setup. 
They can be calculated into time before/after the laser pulse by substracting the measurement-specific delay and multiplying with -1.

Parameters to go with the raw data:

Fluence series (start temperature fixed to ~330 K)
NMG217_00553, deltaT=60K, delay=3.11855 E-4
NMG217_00555, deltaT=78K, delay=3.11879 E-4
NMG217_00557, deltaT=95K, delay=3.11896 E-4
NMG217_00559, deltaT=113K, delay=3.11909 E-4
NMG217_00563, deltaT=129K, delay=3.11917 E-4
NMG217_00565, deltaT=117K, delay=3.11933 E-4

Start temperature series (Fluence fixed to 60 mJ/cm-2)
NMG217_00515, T_0=312K, delay=3.11926 E-4
NMG217_00565, T_0=330K, delay=3.11933 E-4
NMG217_00607, T_0=336K, delay=3.11916 E-4
NMG217_00588, T_0=345K, delay=3.11925 E-4
NMG217_00629, T_0=354K, delay=3.11931 E-4

Temperature shift austenite (temperature fixed to ~413 K)

NMG217_00651,fixed tilting-angle, delay=3.11929 E-4
NMG217_00692,optimized tilting-angle, delay=3.11929 E-4, time step=3.11941 E-4
NMG217_00693,optimized tilting-angle, delay=3.11929 E-4, time step=3.11913 E-4
NMG217_00694,optimized tilting-angle, delay=3.11929 E-4, time step=3.11896 E-4
NMG217_00695,optimized tilting-angle, delay=3.11929 E-4, time step=3.11826 E-4

Static measurements (no time-dependence)
NMG217_509, T_0=305.8K, tilting-angle=20.196
NMG217_511, T_0=311.3K, tilting-angle=20.196
NMG217_584, T_0=335.2K, tilting-angle=20.36264
NMG217_603, T_0=343.7K, tilting-angle=20.33593
NMG217_624, T_0=354.2K, tilting-angle=20.23593
NMG217_635, T_0=365.6K, tilting-angle=20.26927
NMG217_636, T_0=371.1K, tilting-angle=20.26927
NMG217_637, T_0=376.7K, tilting-angle=20.24927
NMG217_638, T_0=382.2K, tilting-angle=20.22927
NMG217_639, T_0=387.6K, tilting-angle=20.22927
NMG217_640, T_0=393K, tilting-angle=20.22927
NMG217_641, T_0=398.5K, tilting-angle=20.22927


Raw Data was read and processed with Matlab code in folder "MATLAB_code".
Start with FitPeakZentrum.m - all other files will be called through that skript
The code extracts the intensity of the desired peak(s) for each image into the struct "DataTableComplete".
For the static measurement the calculation of detector parameters into reciprocal coordinates is necessary to access the lattice paramter.
Use Matlab code UmrDetInRez.m to get Q. 4*1/Q gives the lattice parameter of the austenite.

The processed data is given in .csv-files in each subfolder.