This folder contains 12 files corresponding to the diffraction map panels A-L of Fig. 1.

A: RuCl3_80K_h0l.dat		80K data, h0l plane
B: RuCl3_80K_0kl.dat		80K data, 0kl plane
C: RuCl3_80K_1kl.dat		80K data, 1kl plane
D: RuCl3_300K_h0l.dat		300K data, h0l plane
E: RuCl3_300K_0kl.dat		300K data, 0kl plane
F: RuCl3_300K_1kl.dat		300K data, 1kl plane
G: RuCl3_sim_mC_h0l.dat		simulation for C2/m, h0l plane
H: RuCl3_sim_mC_0kl.dat		simulation for C2/m, 0kl plane
I: RuCl3_sim_mC_1kl.dat		simulation for C2/m, 1kl plane
J: RuCl3_sim_hex_h0l.dat	simulation for P3_112, h0l plane
K: RuCl3_sim_hex_0kl.dat	simulation for P3_112, 0kl plane
L: RuCl3_sim_hex_1kl.dat	simulation for P3_112, 1kl plane

The files list every pixel in the colormaps in the paper according to two reciprocal space indices and an intensity.
The format of the files is [varying_index_1   varying_index_2   intensity]; the fixed index is clear from the filename.
For example, in '*_0kl.dat' the format is [k   l   intensity]; all points listed are at h=0. 

Note that the a* and c* axes are not orthogonal. Thus, in the 'h0l' plots, the vertical axis is not parallel to c*, but 
is rather the approximate (-1/3 0 1) direction (i.e. -a*/3+c*). This means that while the value given in the second column 
is the true value of l, the 'h' index given in the first column is only the true h value for the l=0 line. The correct 
value of h is given by h = h_plot - 1/3*l, where l is the second index, h_plot is the first index, and the factor of 1/3 
is approximate.

In the Figure, the intensity I is plotted on a log scale, as log_2(1+I/255).


