THE REACTOR NEUTRON CAPTURE CROSS SECTION OF Ag110m

1963 ◽  
Vol 41 (8) ◽  
pp. 1321-1331
Author(s):  
R. G. Hart ◽  
R. L. Graham

Natural silver has been irradiated for 75.3 days in a thermal neutron flux of 2.42 × 1014 cm−2 sec−1 and the complex beta-ray spectrum of the resulting activities of 249-day Ag110m and 7.5-day Ag111 have been studied with a magnetic spectrometer. From the measured ratio of the respective beta-ray intensities and using the currently accepted decay schemes of these nuclides a value of 82 ± 11 barns is obtained for the reactor neutron capture cross section of Ag110m. Possible causes of systematic error are discussed.

1970 ◽  
Vol 48 (6) ◽  
pp. 716-724 ◽  
Author(s):  
R. W. Durham ◽  
F. Molson

The neutron capture cross section of 242Pu has been measured by determining the 243Am product. Samples were irradiated in a neutron flux having essentially a Maxwellian distribution defined by the temperature (37.5 °C) of a water annulus around the sample tube. Plutonium and americium were separated from each other chemically and their concentrations and isotopic compositions obtained by low-geometry α counting and α spectrometry. A value for gσ0 of 18.7 ± 0.7 b was obtained where g represents the deviation from 1/v behavior.


1960 ◽  
Vol 38 (12) ◽  
pp. 1690-1701
Author(s):  
Gwen M. Milton ◽  
W. E. Grummitt

A high specific activity source of Y91, freed from natural uranium and rare earths, was irradiated in a high flux position in the NRX reactor. After further chemical purification, 3.6-hour Y92 was identified in the sample by measurement of the 3.6-Mev β-particle associated with its decay, using a scintillation spectrometer. Two such measurements have established the reactor neutron capture cross section of Y91 to be 1.4 ± 0.3 barns.


1966 ◽  
Vol 44 (11) ◽  
pp. 2956-2959 ◽  
Author(s):  
R. Courtemanche ◽  
T. A. Eastwood ◽  
R. D. Werner

1956 ◽  
Vol 34 (8) ◽  
pp. 1023-1026 ◽  
Author(s):  
L. P. Roy ◽  
L. Yaffe

The cross section of Ce142 has been determined by the activation method and found to be 0.95 ± 0.05 barns relative to a value of σCo59 = 36.3 barns. Disintegration rates were determined by a 4π counter. The value obtained agrees with that of Katcoff etal. (1949) also obtained by the activation method but differs markedly from that of Pomerance (1952).


1956 ◽  
Vol 34 (3) ◽  
pp. 238-245 ◽  
Author(s):  
L. P. Roy ◽  
L. Yaffe

Ce144 has been produced by the successive neutron capture reaction Ce142 (n, γ)Ce143(n, γ)Ce144. The pile neutron capture cross section of the 33 hr. Ce143 was determined by separating Pr144, the daughter of Ce144, from the rigorously-purified cerium at frequent intervals. The amount of Pr144 formed increased linearly with the square of the neutron flux in a manner consistent with that of a successive neutron capture reaction. The value for the pile neutron capture cross section of Ce143 was found to be 6.0 ± 0.7 barns.


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