Neutron Production from the Deuteron Breakup Reaction on Deuterium

Cabral, S.; Börker, G.; Klein, H.; Mannhart, W.

doi:10.13182/nse90-a29059

Cited by 35 publications

(9 citation statements)

References 10 publications

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“…This code takes into account the energy loss, energy spread, and angular straggling of the deuterons in the entrance window of the cell, the neutron production within the volume of the gas cell, the angular distribution of the 2 H(d, n) 3 He reaction, the breakup of the deuterons in the D 2 gas according to the results from [19], and the activation geometry.…”

Section: Mean Neutron Energy and Flux Densitiesmentioning

confidence: 99%

Neutron induced reaction cross sections for the radioactive target nucleus 99Tc

et al. 2009

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Section: Mean Neutron Energy and Flux Densitiesmentioning

confidence: 99%

Neutron induced reaction cross sections for the radioactive target nucleus 99Tc

et al. 2009

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“…The breakup of the deuteron on the deuterium gas was determined according to the results of Cabral et al [22]. NEUT was also used to calculate the whole neutron spectrum which is divided into a breakup part and a monoenergetic part.…”

Section: B Neutron Energies and Flux Densitiesmentioning

confidence: 99%

Cross sections and isomeric cross-section ratios in the interactions of fast neutrons with isotopes of mercury

et al. 2006

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3 He reaction using a deuterium gas target at the Jülich variable energy compact cyclotron CV 28. Use was made of the activation technique in combination with high-resolution, high-purity Ge detector γ -ray spectroscopy. All the data were measured for the first time over the investigated energy range. The transition from the present low-energy data to the literature data around 14 MeV is generally good. Nuclear model calculations using the codes STAPRE and EMPIRE-2.19, which employ the statistical and precompound model formalisms, were undertaken to describe the formation of both the isomeric and ground states of the products. The total reaction cross section of a particular channel is reproduced fairly well by the model calculations, with STAPRE giving slightly better results. Regarding the isomeric cross sections, the agreement between the experiment and theory is only in approximate terms. A description of the isomeric cross-section ratio by the model was possible only with a very low value of η, i.e., the eff / rig ratio.

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“…Another effect, caused by the breakup of deuterons on the D2 gas, had, however, to be estimated. For this purpose we used the results of Cabral et al [24]. Those authors studied the ratio of activity induced by breakup neutrons to that caused by monoenergetic neutrons as a function of neutron energy and reaction threshold.…”

Section: (B) Effect Of Background Neutronsmentioning

confidence: 99%

Excitation Functions of some Neutron Threshold Reactions on ⁸⁹Y in the Energy Range of 7.8 to 14.7 MeV

Klopries¹,

Dóczi²,

Sudár³

et al. 1997

Radiochimica Acta

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Neutron Production from the Deuteron Breakup Reaction on Deuterium

Cited by 35 publications

References 10 publications

Neutron induced reaction cross sections for the radioactive target nucleus 99Tc

Neutron induced reaction cross sections for the radioactive target nucleus 99Tc

Cross sections and isomeric cross-section ratios in the interactions of fast neutrons with isotopes of mercury

Excitation Functions of some Neutron Threshold Reactions on ⁸⁹Y in the Energy Range of 7.8 to 14.7 MeV

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Neutron Production from the Deuteron Breakup Reaction on Deuterium

Cited by 35 publications

References 10 publications

Neutron induced reaction cross sections for the radioactive target nucleus 99Tc

Neutron induced reaction cross sections for the radioactive target nucleus 99Tc

Cross sections and isomeric cross-section ratios in the interactions of fast neutrons with isotopes of mercury

Excitation Functions of some Neutron Threshold Reactions on 89Y in the Energy Range of 7.8 to 14.7 MeV

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Excitation Functions of some Neutron Threshold Reactions on ⁸⁹Y in the Energy Range of 7.8 to 14.7 MeV