{\rtf1\ansi\ansicpg1252\cocoartf2761 \cocoatextscaling0\cocoaplatform0{\fonttbl\f0\fswiss\fcharset0 Helvetica;\f1\fnil\fcharset0 HelveticaNeue;} {\colortbl;\red255\green255\blue255;} {\*\expandedcolortbl;;} \paperw11900\paperh16840\margl1440\margr1440\vieww11520\viewh8400\viewkind0 \pard\tx566\tx1133\tx1700\tx2267\tx2834\tx3401\tx3968\tx4535\tx5102\tx5669\tx6236\tx6803\pardirnatural\partightenfactor0 \f0\fs24 \cf0 ___________________________________README______________________________\ \ \ \pard\pardeftab560\slleading20\partightenfactor0 \f1\fs26 \cf0 Here you can find the magnetotropic susceptibility data from Figure 2c\'96d corresponding to the ac and bc plane, respectively. Each file corresponds to the data for a certain angle at which the magnetic field is applied to the sample. The first column represents the magnetic field B in units of tesla (T), and the second column corresponds to the magnetotropic susceptibility k in units of kilojoules per mole per radians squared (kJ\'b7mol^-1\'b7rad^-2). \ From the raw data, we have performed a sliding window analysis to calculate the Fourier transform, obtaining frequency as a function of magnetic field. The frequency was then multiplied by the calibration factor of the sample to convert it into k with its respective units, as explained in the Supplementary Information (SI).}