presence of zirconium by thermal-neutron activation for Hf ta~ {TI/2 = 5.5 h) or Hf 181 (]71/2 = 46 days) requires very long periods of time [2, 3]. The results of the analysis are also affected by elements accompanying the hafnium, and this reduces the accuracy and reliability of the results. The sensitivity of analysis for the isotope Hf 179m when the neutron flux density is 1012-10 la neatrons/cm 2 �9 sec is no better than 0.03-0.04% [2-4], although a sensitivity of 5 �9 10-4% was achieved in [5] by the analysis of zirconium concentrates. The presence of zirconium (Zr 89m, Tt/2 = 4.4 min), silicon (Si 28 (n, p)A128, Ti/2 = 2.3 rain), and other elements [6] interferes with analysis using 14 MeV neutrons by the Hf 1~~ (n, 2n)Hf 179m reaction. The threshold sensitivity for the determination of hafnium at a flux of 1 �9 109 neutrons/era 2 �9 sec for a 0.1 g specimen is only 50/~g in the absence of interfering elements. The proposed activation method for determining hafnium from the (y, y') reaction is extreraely rapid, selective, and highly sensitive. One circumstance favoring the use of this interaction for determining the hafnium content of ores and ore-processing products is that when the bremsstrahlung boundary energy (Eymax) is below the thresholds for thermonuclear reactions, there is no possibility of activating any of the light elements up to arsenic. T hese elements are the principal rock-forming components of ore specimens. Moreover, there are only 21 nuclei, of 18 elements from selenium to mercury, which display ~someric activity in connection with the (y, 7') reaction with T1/2 ranging from seconds to days [7-9]. Zirconium, always found in association with hafnium, is not excited in this reaction. This substantially improves the selectivity of the analysis and considerably simplifies the interpretation of the Y-spectra. Another fact in favor of using this method is that there is practically no self-shielding effect, so that it is possible to analyze samples which are more representative than in the case of neutron-activati on analysis. The inelastic scattering of y-quanta by nuclei of the isotope Hf 179 leads to the formation of the rectastable state Hf 179m, with TI/2 = 19 see and Ey = 215 keV. The excitation of ttf 17ore was carried out by means of bremsstrahlung from a linear accelerator with an electron energy of 5 MeV.
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