2004
DOI: 10.1103/physrevc.69.064609
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Light-ion production in the interaction of96MeVneutrons with silicon

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Cited by 21 publications
(29 citation statements)
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“…It is shown a relative good agreement between DHORIN and EXFOR experimental data in both the order of magnitude of the cross sections and the shape of the excitation functions. Notice however that the pre- [111][112][113] dicted shape for 24 Na is not quite the same that experimental data.…”
Section: Excitation Functions For Aluminiummentioning
confidence: 54%
“…It is shown a relative good agreement between DHORIN and EXFOR experimental data in both the order of magnitude of the cross sections and the shape of the excitation functions. Notice however that the pre- [111][112][113] dicted shape for 24 Na is not quite the same that experimental data.…”
Section: Excitation Functions For Aluminiummentioning
confidence: 54%
“…3. Double-differential cross sections at laboratory angles of 20 • , 40 • , 60 • , and 80 • for protons, deduced from the CH 2 targets in the present experiment (filled triangles) as well as the experiment (open squares) on oxygen and silicon [12,17]. Note that the small peaks around 9 and 22 MeV at laboratory angles of 20 • are np scatterings due to a low-energy neutron tail from the previous beam burst (wrap around; see Ref.…”
Section: A Pulse-height Discriminator Correctionmentioning
confidence: 69%
“…The experimental setup has been described in detail previously [17,18], and therefore only a brief summary is given here. The neutron beam facility at TSL uses the 7 Li(p, n) 7 Be reaction (Q = −1.64 MeV) to produce a quasi-monoenergetic neutron beam [19].…”
Section: Experimental Methodsmentioning
confidence: 99%
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