was impractical to imbed thermocouples in the crystals for each run, the oven temperature was monitored, and later ji calibration curve of crystal temperature versus oven temperature was obtained. Although this produces some uncertainty, the reproducibility of the data indicates that changes in thermal contacts were small and had little effect upon the data.The thermocouple imbedded in the oven, which was of Pt vs Pt 10 percent Rh, was checked against a Leeds and Northrup optical pyrometer at 960°C. Using an emissivity of 0.37 for molybdenum and an estimated glass transmission factor of 90 percent, the two readings differed by only 4°C.T HE coherent neutron scattering cross sections of nitrogen and vanadium have been evaluated from neutron diffraction patterns of vanadium nitride VN and confirmed by similar data from potassium azide KN3 and vanadium carbide VC. Vanadium nitride was prepared by the reaction of pure V2O5 with NH 3 gas at 1100°C for 6 to 8 hours. Neutron diffraction patterns with neutron wavelength 1.16A were obtained from samples sealed in aluminum cells shortly after preparation. The technique for making neutron diffraction measurements will be described elsewhere. FIG. 1. A plot of observed neutron diffraction values of 1^/16 against sin 2 0 for vanadium nitride and vanadium carbide. The vertical lines indicate the estimated precision of the individual values.In the calibration experiments, the crystal temperature was found both by imbedding 4-mil thermocouples in holes in the crystal arid also by using small platinum plates, in thermal contact with the crystal, to transfer heat to the thermocouples; the two methods gave similar results. The temperature gradient along the crystal was measured by two thermocouples, one at the end and one in the middle of the crystal. This gradient will produce an exponential conductivity gradient along the crystal, and the electric field in the crystal will hence be non-uniform, thus affecting the Hall voltage. An appropriate correction factor has been calculated and is plotted in Fig. 3.VN crystallizes with the rocksalt structure, for which structure factors are of two types, corresponding to even-index and odd-index reflections. Integrated reflections of three odd-index and four even-index reflections were measured and converted to absolute structure-factor values by comparison with the (111) reflection from nickel powder, for which the coherent cross section was taken as 13.4 barns. 1 The (311) reflection was corrected for contamination by (222) by computing the intensity of the latter from its interpolated structure factor. The resulting values of F 2 /16 are plotted in Fig. 1 against sin 2 0. Extrapolation of each family to zero angle yields values proportional to the squares of the structure factors corrected for the effect of temperature and zero-point motion in the crystal and equal, respectively, to the sum (even reflections) and difference (odd reflections) of the scattering amplitudes of V and N. It is immediately apparent that the amplitude of vanadium...