Abstract
The field-induced magnetic phase transitions in MnCl2·4H2O were investigated by measuring the differential magnetic susceptibility between 0.26 and 1.5°K in external magnetic fields up to 27 kOe. With the external field along the most preferred axis of the crystal (c direction), both the antiferromagnetic-to-spin-flop (AF-to-SP) and the spin-flop-to-paramagnetic (SF-to-P) transitions were observed below 1.3°K. The AF-to-SF transition appears to be a first-order transition, as predicted by molecular-field theory. The temperature dependence of the phase boundary is given by Hc=Hc0+bT, where Hc0=7550±10 Oe and b=434±10 Oe/deg. Within the spin-flop state χc is roughly constant and approximately equal to the value of χ in zero field. At the SF-to-P phase boundary, χc drops rapidly to zero. The temperature dependence of the SF-to-P transition is given by Hc=Hc0(1CTn) up to about 0.7°K, where Hc0=20.6±0.03 kOe, n=1.82±0.10, and c=0.228±0.002.