H. Ferdinande
Ghent University
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Featured researches published by H. Ferdinande.
Nuclear Instruments and Methods | 1975
R. Carchon; E. Van Camp; G. Knuyt; R. Van de Vyver; J. Devos; H. Ferdinande
Abstract A procedure is described for calculating the solid angle in a general source-to-detector geommetry, by a Monte Carlo method.
Nuclear Physics | 1991
A. De Graeve; A. Zieger; R. Van de Vyver; C. Van den Abeele; H. Ferdinande; L. Van Hoorebeke; D. Ryckbosch; F. De Smet; B. Ziegler
Abstract The 0° and 180°, as well as the 90° differential cross sections for the 2 H(γ, p)n reaction have been measured at lab photon energies between 7 and 19 MeV. Special attention was paid to the accuracy, in particular by measuring the forward Compton electron yield. For the extreme angles, the statistical error on our results amounts to 4–5% (0°) and 7–8% (180°), respectively, while the systematic uncertainty is at most 3%. The data confirm the existence of a minimum in the forward cross section and indicate beyond any doubt that the fore/aft ratio is larger than unity. Comparison shows reasonable agreement with the results from recent “conventional” theoretical approaches, including meson exchange and relativistic corrections, although the description of the c -coefficient, appearing in the Partovi expansion of the differential cross section, remains unsatisfactory. A possible source for this discrepancy could be the inadequate description of the El and/or the E2 transition operator.
Nuclear Physics | 1972
R. Van de Vyver; H. Ferdinande; G. Knuyt; R. Carchon; J. Devos
Abstract The total photoneutron cross sections for 12 C and 19 F were measured from threshold to 33 and 19 MeV respectively, with the use of bremsstrahlung from a linac and by direct detection of the neutrons. The yield curves were analysed using the variable-bin Penfold and Leiss unfolding technique, and the least-structure method of Cook. The 12 C data are in good agreement with available results; the 19 F ( γ , χ n) cross section shows considerable fine structure, not observed in neighbouring odd-mass nuclei.
Few-body Systems | 1991
A. De Graeve; A. Zieger; R. Van de Vyver; C. Van den Abeele; H. Ferdinande; L. Van Hoorebeke; D. Ryckbosch; F. De Smet; B. Ziegler
The forward2H(γ,p)n cross section was measured at 7.2 and 8.5 MeV photon energy. The new absolute values confirm the theoretically predicted presence of a minimum in this cross section. A discrimination is made between the results from various theoretical descriptions.
Physics Letters B | 1989
A. De Graeve; A. Zieger; R. Van de Vyver; H. Ferdinande; L. Van Hoorebeke; D. Ryckbosch; P. Van Otten; B. Ziegler
Abstract The 2 H(γ, p)n cross section was measured absolutely at 0° for the outgoing proton, for photon energies between 8 and 18 MeV. The rising trend observed in the cross section in this energy region indicates the existence of the theoretically predicted minimum. Our results at E γ ≈10 MeV are well described by recent relativistic calculations, the data around 15 MeV, on the contrary, are commonly underestimated.
Nuclear Instruments and Methods | 1976
J. Devos; R. Van de Vyver; E. Van Camp; R. Carchon; H. Ferdinande
Abstract The use of a recoil-proton spectrometer as a tool for the measurement of absolute differential photoneutron cross sections is described. The efficiency of the stilbene scintillator was calculated by means of a Monte Carlo method. The test measurements of the photoneutron spectra from 16 O and 12 C show that this simple device may prove very valuable in photonuclear research.
European Physical Journal A | 1978
R. Van de Vyver; J. Devos; H. Ferdinande; R. Carchon; E. Van Camp
The total photoneutron cross section of208Pb was measured between 8 and 13 MeV using the bremsstrahlung photon facility from a 35 MeV linac. Considerable resonance structure was observed in the cross section, of which the peak around 9 MeV, as well as the structure around 10.8 MeV may be due toE2 excitations.
Nuclear Physics | 1988
D. Ryckbosch; E. Van Camp; R. Van de Vyver; A. De Graeve; L. Van Hoorebeke; H. Ferdinande
Abstract The unified exciton model, based on a master-equation approach, is extended to describe also the coupling between exciton states of different isospin. This allows the determination of the time evolution of the isospin mixing coefficient μ 2 ( t ). The equilibration of the excited nucleus, both in exciton number and isospin space, is discussed. It is shown that the nucleus essentially decays before full equilibrium is established.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1988
P. Van Otten; R. Van de Vyver; E. Van Camp; E. Kerkhove; P. Berkvens; H. Ferdinande; D. Ryckbosch; A. De Graeve; L. Van Hoorebeke
A general Monte Carlo procedure is described for calculating the geometrical efficiency of a detection system with regard to a beam of particles impinging on a gaseous target or on a plane parallel target plate with finite thickness, while the detected particles are emitted with an isotropic angular distribution or one of the form [1−0.5P2 (cos θ)], with P2 (cos θ) the second Legendre polynomial. This method was successfully applied to the analysis of the 16O(γ, P0)15N data.
Nuclear Physics | 1987
E. Kerkhove; P. Berkvens; R. Van de Vyver; H. Ferdinande; P. Van Otten; D. Ryckbosch; E. Van Camp
Abstract Spectra of protons and alpha-particles, emitted from the giant electric dipole resonance of 28 Si excited by quasi-monochromatic photons from in-flight annihilation of accelerated positrons, were measured. Cross sections for six charged-particle decay channels were extracted in the energy region from 16.8 to 25.7 MeV. While the ( γ , α 0 ) cross section is completely statistical in nature, the (γ, p) process was found to have a 65% semidirect component, mainly in the ( γ , p 0 ) and ( γ , p 1+2 ) channels.