Fig. 3
From: Fulde–Ferrell–Larkin–Ovchinnikov and vortex phases in a layered organic superconductor
MCE as a function of the magnetic field. a MCE as a function of the magnetic field at various field angles θ. Three series of peaks are observed. b A broad peak at Hpeak1 is observed only in a limited angle region. c Other two series of peaks, sharp and broad ones, which are denoted by Hpeak2 and Hpeak3, respectively. All the peaks do not change the sign between the up and down sweeps, showing that supercooling and superheating effects are dominant at the transitions. d MCE as a function of the magnetic field at various temperatures. With increasing temperature, the peak field Hpeak1 indicated by arrows gradually decreases and the peak intensity is suppressed
