130Teの二重ベーター崩壊半減期
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The half-life of <SUP>130</SUP>Te double β-decay was determined by a mass-spectrometric method. The samples were old tellurium ores (such as tetradymite: Bi<SUB>2</SUB>Te<SUB>2</SUB>S), obtained from Oya gold mine in Japan. The amount of <SUP>130</SUP>Xe, which was occluded in the tellurium ores as the daughter of <SUP>130</SUP>Te double β-decay, was measured by isotope dilution method using <SUP>128</SUP>Xe as a spike. The mass spectrometer used is 20 cm radius, 90° single focusing type. The detection limit for xenon under static operation is about 10<SUP>5</SUP>-10<SUP>6</SUP> atoms by using a 12-stages Cu-Be electron multiplier followed by a vibrating reed electrometer as a measuring system of ion currents. Th spike <SUP>128</SUP>Xe used was prepared by neutron irradiation of KI in a nuclear reactor. The amount of four samples used were 17.5g (33.8% Te), 10.9g (13.2% Te), 22.3g (22.4% Te) and 12.4g (22.4% Te) .<BR> The decay products: <SUP>130</SUP>Xe, occluded in tellurium ores, were extracted by heating them in an electric furnace at about 700-1200 °C. Pure calcium metal, titanium-filament, tangsten-filament and a dry ice trap were used to remove impurity gas components. In the mass spectra, excesses of <SUP>129</SUP>Xe, <SUP>130</SUP>Xe and <SUP>131</SUP>Xe over normal xenon were found, and the excess of <SUP>130</SUP>Xe was predominant among them. The excess amount of <SUP>130</SUP>Xe obtained were(2.09±0.27) × 10<SUP>-11</SUP> ccSTP, (1.01±0.18) × 10<SUP>-11</SUP> ccSTP, (2.65±0.08) × 10<SUP>-11</SUP> ccSTP and(1.27±0.06) × 10<SUP>-11</SUP> ccSTP for above each sample, respectively. On the assumption that the <SUP>130</SUP>Xe excesses obtained above were entirely due to the <SUP>130</SUP>Te doubleβ-decay, the half-lives of <SUP>130</SUP> Te doubleβ-decay were calculated to be10.7 × 10<SUP>20</SUP> years, 5.38 × 10<SUP>20</SUP> years, 7.29 × 10<SUP>20</SUP> years and 8.27 × 10<SUP>20</SUP> years for the above each case. The half-life of <SUP>130</SUP>Te double β-decay is(7.91±1.11) × 10<SUP>20</SUP> years on the average. This value agrees fairly with the result(1.4×10<SUP>21</SUP> years)of Inghram-Reynolds, the result(3.3×10<SUP>21</SUP> years)of Hayden-Inghram and the theoretical value(2×10<SUP>21±2</SUP> years)of Primakoff-Rosen, based on two neutrino theory. The xenon age of the tellurium ores, which was used for calculation of the above half-lives, was determined from the age of porphyrite, of which the age is expected to be about the same as that of the tellurium ores. The age of porphyrite was determined to be(9.06±0.29)×10<SUP>7</SUP> years by K-Ar method with the same mass spectrometer as used for the above <SUP>130</SUP>Xe measurement.<BR> The ratio of <SUP>129</SUP>Xe excess to <SUP>131</SUP>Xe excess is obtained about 1.6, and the ratio, estimated from the neutron absorption cross sections for<SUP>128</SUP>Te and<SUP>130</SUP>Te and their abundance ratios, is about 0.6. These ratios are not in agreement one another. So these excesses in <SUP>129</SUP>Xe and <SUP>131</SUP>Xe seem to be produced, in part, by neutron absorptions of <SUP>128</SUP>Te and<SUP>130</SUP>Te and, in part, by different processes.
- 日本質量分析学会の論文
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