Abstract
The metamagnetic (spin-flop) transition is studied in single crystals of FeCl2 and FeBr2 using the Mössbauer effect and external magnetic fields up to 40 kG. From the changes which take place in the m=12m*=32 and m=12m*=32 transitions when FeBr2 passes through the spin-flop, the sign of the internal field at the nucleus is found to be positive. In addition, the difference between the interionic dipolar fields above and below the spin-flop transition is determined as -6.7 kG for FeBr2. The interionic dipolar fields are also calculated for FeCl2, FeBr2, and FeI2 above and below the spin-flop. The calculated difference for FeBr2 is -6.8 kG, in good agreement with the experimental difference. The internal magnetic field at the iron nucleus in FeCl2 is found to be -5.0 kG above the spin-flop. This result is used with the calculated lattice sums to determine the internal field below the spin-flop. A value of +2.8 kG is found for this field, in agreement with earlier observations. The sign of the internal field in FeI2 is predicted to be positive. Increasingly positive internal fields going down the series FeCl2, FeBr2, and FeI2 are consistent with the interpretation that the iron-halogen bond is increasingly covalent. This is manifested in an increasing fraction of 4s electron character in the Fe2+ electronic configuration.