The 12C(d, n)13N reaction between Ed = 7.0 and 13.0 MeV
References (18)
- et al.
Nucl. Phys.
(1971) - et al.
Nucl. Phys.
(1972) Nucl. Instr.
(1981)- et al.
Nucl. Instr.
(1979) - et al.
Nucl. Instr.
(1981) - et al.
Nucl. Phys.
(1967) - et al.
Nucl. Phys.
(1967) - et al.
Nucl. Phys.
(1972) Nuclear reactions and nuclear structure
(1971)
There are more references available in the full text version of this article.
Cited by (10)
RESONEUT: A detector system for spectroscopy with (d,n) reactions in inverse kinematics
2018, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentCitation Excerpt :In both cases the simulated peak-shapes show a very good fit, including the detector resolution and a slightly asymmetric peak shape with a tail towards longer flight times, which is caused by scattering off the vacuum chamber material into the detectors. In the simulations of both spectra we used the relative cross section for the ground state and the 2.365 MeV state from Schelin et al. [7]. The reproduction of the peak size in the upper- and lower-panel spectrum also implies that the absolute detection efficiency is well reproduced over the relevant energy range.
New approach to description of (d, xn) spectra at energies below 50 MeV in Monte Carlo simulation by intra-nuclear cascade code with Distorted Wave Born Approximation
2014, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsNucleon Transfer Reactions in Few-Body Nuclear Systems
2017, Few-Body SystemsModelling and analysis of nucleon emission from deuteron-induced reactions at incident energies up to 100 MeV
2016, EPJ Web of Conferences
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