Fig. 2.

SST in Mn(taa) as a function of pulsed magnetic field. a Magnetic field range of the magnets used in this work: superconducting (up to 14T), resistive DC (up to 45T), and pulsed (up to 60T). b The magnetic field vs time for the pulsed magnet. c ΔM relative to M (H = 0) as a function of H up to 60 T for different T on a randomly oriented collection of single crystals. Data is taken after zero field cooling (electric and magnetic fields) from room temperature. The SST is evident as a broad jump in the magnetization. For a given temperature, the jump in SST occurs at a higher H for the upsweep than the downsweep. The standard errors due to random noise are smaller than the line widths. A systemic error due to mechanical vibrations yields oscillations, and their maximum amplitude is indicated by an error bars in the plot