1989
DOI: 10.1103/physrevc.39.766
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Structure ofC14via elastic and inelastic neutron scattering fromC

Abstract: Differential cross sections for neutrons elastically scattered from ' C and inelastically scattered to the first three excited states ' C*(3.09, 3.68, and 3.85 MeV} were measured at 69 incident energies for 4.5&E"&11 MeV. A multiple scattering code provided a simulation of the experimental scattering process allowing accurate corrections to the small measured inelastic cross sections. The integrated "C(n, n)' Be cross section was determined by subtracting the sum of the measured integrated cross sections from … Show more

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Cited by 19 publications
(29 citation statements)
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“…Analysis was performed of the breakup of the excited 14 C nuclei into 10 Be + α at forward angles in the projectiletarget center-of-mass frame. Here the dominant excitation mechanism was expected to be inelastic scattering.…”
Section: Analysis and Resultsmentioning
confidence: 99%
“…Analysis was performed of the breakup of the excited 14 C nuclei into 10 Be + α at forward angles in the projectiletarget center-of-mass frame. Here the dominant excitation mechanism was expected to be inelastic scattering.…”
Section: Analysis and Resultsmentioning
confidence: 99%
“…They believe those contributions are minimal. From Resler et al (1989), the only energies in which there are significant cross sections for the reaction are the region 6.05 to 9.35 MeV. The higher energy contribution is calculated to be much less significant.…”
Section: Comparison With Literature Valuesmentioning
confidence: 97%
“…2, NEA, 2005) are derived from very early work, which would be considerably improved if redone today. Errors can be several tens of percentage points, and in view of the paper of Resler et al (1989) cannot be considered accurate at high energies. Resler et al (1989) (Fig.…”
Section: Comparison With Literature Valuesmentioning
confidence: 98%
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