Cumulative Fission Yield and Half-Life of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">Sb</mml:mi></mml:mrow><mml:mprescripts /><mml:mrow /><mml:mrow><mml:mn>134</mml:mn></mml:mrow><mml:mrow /><mml:mrow /></mml:mmultiscripts></mml:mrow></mml:math>

Delucchi, A.A.; Greendale, A. E.; Strom, Peter O.

doi:10.1103/physrev.173.1159

Cited by 23 publications

(5 citation statements)

References 16 publications

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“…The measured half-life of 11.3(3) s is in agreement with the currently accepted half-life of 10.07(5) s. The reference to Strom et al mentioned in the quote listed as "to be published" was submitted two months later [85]. 135 135 Sb in the 1964 article "Half life of 135 Sb and evidence on the half life of 134 Sb" [86].…”

Section: Sbsupporting

confidence: 80%

Discovery of palladium, antimony, tellurium, iodine, and xenon isotopes

Kathawa

Fry

Thoennessen

2013

Atomic Data and Nuclear Data Tables

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Section: Sbsupporting

confidence: 80%

Discovery of palladium, antimony, tellurium, iodine, and xenon isotopes

Kathawa

Fry

Thoennessen

2013

Atomic Data and Nuclear Data Tables

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“…(4) The non-shell-corrected continuous mass equation of Green" satisfactorily correlated with the MNPE treatment, but the results are similar to the ECD hypothesis. ACKNOWLEDGMENTS I wish to thank the U. S. Atomic Energy Commission for the support of this work under Contract No.…”

Section: Discussionmentioning

confidence: 60%

Charge Distribution in the Fission ofTh232

Rao

1972

Phys. Rev. C

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p, ny)"5th reaction, implies the spin sequence for the (wg», )(vd, ») ' multiplet to be 6', 5', 4', 3', 7', 2' for the corresponding states at energies 0-, 43-, 142-, 180-, (233-), 630-MeV, respectively. Because these spin assignments depend on the structure of the states as previously identified, ' the assignments cannot be viewed as most definite. Except for the 7' 233~5-keV state, the level energies were obtained from the y measurements to within uncertainties of 1 to 2 keV. The above spin assignments are in accord with the tentative spin assignments made by Comfort et al. 'The results also agree with those predicted by the Pandya transformation from the known (wgz, )(vd",) multiplet in~Nb. The 2 and 3 states associated with the (wp",}(vd", ) ' configuration are expected at a low excitation energy in Nb. The present y measurements suggest that the state at 506 keV is 2 and the 687-keV state is 3; however, more experiments, such as an internal-conversion measurement, are needed to verify that the 687-506-keV dipole transition is an M1 transition and that the 506-180-keV y transition is El.Independent-fission yields of Nba~~, Nbse, Tce~, Rh~, Ag In 5~, Cs~, and Cs 3~~, and fission yields of four mass chains in the symmetric region A =111-115have been determined in the fission of Th232 induced by 14.8-MeV neutrons. Various postulates of charge distribution were tested to correlate the experimental data. It was found that the equalcharge-displacement hypothesis agreed well for the fission products produced by the asymmetric mode of fission, and the constant-charge-ratio postulate showed the best correlation for the fission products produced by the symmetric mode of fission. Evidence for 40and 50-proton shell effects on the fission yields has been found in this work.

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“…For 134 Sb refs. [2,48,49] give an average value of 0.40 ±0.07%. The contribution from 134 Sn is expected to be very small, and the value can be used both as independent and cumulative yield.…”

Section: Indium Isotopesmentioning

confidence: 99%

Yields of Products from Thermal Neutron-Induced Fission of ²³⁵U

et al. 1990

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A comprehensive study has been carried out of the yield pattern of fission products formed in thermal neutron-induced fission of 235 U. An isotope separator on-line a nuclear reactor was used for rapid separation of the fission products. At a target temperature of 2400 Q C all fission elements, with the exception of the little volatile transition elements zirconium, niobium, molybdenum, technetium, ruthenium, and rhodium, are released. Their isotopes are then available for study which means that a very complete mapping of the yield distribution is within reach. In the analysis the delay between production and measurement and the overall separator efficiency for three consecutive elements -the one under study and its parent and grandparentare taken into account. Independent and/or cumulative yields have been obtained for 195 nuclear species, among them 83 isomeric states.

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Cumulative Fission Yield and Half-Life ofSb134

Cited by 23 publications

References 16 publications

Discovery of palladium, antimony, tellurium, iodine, and xenon isotopes

Discovery of palladium, antimony, tellurium, iodine, and xenon isotopes

Charge Distribution in the Fission ofTh232

Yields of Products from Thermal Neutron-Induced Fission of ²³⁵U

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Cumulative Fission Yield and Half-Life ofSb134

Cited by 23 publications

References 16 publications

Discovery of palladium, antimony, tellurium, iodine, and xenon isotopes

Discovery of palladium, antimony, tellurium, iodine, and xenon isotopes

Charge Distribution in the Fission ofTh232

Yields of Products from Thermal Neutron-Induced Fission of 235U

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Product

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Yields of Products from Thermal Neutron-Induced Fission of ²³⁵U