Final state interactions in the reaction T(He3, He4) np

Triple correlation cross sections have been measured for the reaction T(He³,He⁴)np in a complete experiment at a He³ bombarding energy of 1.5 MeV. Three similar experimental geometries were used which allow the observation of low relative energies in the n-p system, and energies of 0.96 MeV in...

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Main Author: Beveridge, John Leslie
Language:English
Published: University of British Columbia 2011
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Online Access:http://hdl.handle.net/2429/34699
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spelling ndltd-UBC-oai-circle.library.ubc.ca-2429-346992018-01-05T17:47:39Z Final state interactions in the reaction T(He3, He4) np Beveridge, John Leslie Nuclear reactions Triple correlation cross sections have been measured for the reaction T(He³,He⁴)np in a complete experiment at a He³ bombarding energy of 1.5 MeV. Three similar experimental geometries were used which allow the observation of low relative energies in the n-p system, and energies of 0.96 MeV in the He⁴-n system. Therefore the n-p singlet and He⁵ (g.s.) final state interactions were observed. Events from the two body reaction channel T(He³,d)He⁴ and overlapping kinematic contours were eliminated by particle identification. A least squares fit to the experimental triple correlation cross section for one geometry was made using two approximate theories for three body reactions. These were the Watson, and Phillips, Griffy and Biedenharn (P.G.B.) final state interaction theories. Both theories give the theoretical cross section to be proportional to a density of states (D.O.S.) function. The P.G.B. theory gives two forms for this function (P.G.B.1 and P.G.B.2). The D.O.S. functions for the state of He⁵ and Li⁵ were calculated using only the P.G.B. 1 and Watson forms. The P.G.B.1 form gives an inadequate description of both the n-p singlet and He⁵(g.s.) final state enhancements. The He⁵(g.s.) enhancement is well described by the Watson form of the D.O.S. function. The triple correlation cross section, for high proton energies, was dominated by a sequential breakup through the ground state of He⁵ and by direct three body breakup. No evidence for contributions from the states of Li⁵ or for any well defined contributions from the first excited state of He⁵ were observed. The Watson and P.G.B.2 forms of the singlet n-p D.O.S. function gave indistinguishable predictions of the n-p singlet enhancement. The P.G.B. 2 form was used, for seven values of the n-p singlet scattering length, to fit the experimental data. The value of the singlet n-p scattering length extracted in the fitting procedure was [formula omitted]. The large experimental errors assigned were caused by the sensitivity of the extracted value on the background terms included in each fit. Science, Faculty of Physics and Astronomy, Department of Graduate 2011-05-19T18:26:33Z 2011-05-19T18:26:33Z 1970 Text Thesis/Dissertation http://hdl.handle.net/2429/34699 eng For non-commercial purposes only, such as research, private study and education. Additional conditions apply, see Terms of Use https://open.library.ubc.ca/terms_of_use. University of British Columbia
collection NDLTD
language English
sources NDLTD
topic Nuclear reactions
spellingShingle Nuclear reactions
Beveridge, John Leslie
Final state interactions in the reaction T(He3, He4) np
description Triple correlation cross sections have been measured for the reaction T(He³,He⁴)np in a complete experiment at a He³ bombarding energy of 1.5 MeV. Three similar experimental geometries were used which allow the observation of low relative energies in the n-p system, and energies of 0.96 MeV in the He⁴-n system. Therefore the n-p singlet and He⁵ (g.s.) final state interactions were observed. Events from the two body reaction channel T(He³,d)He⁴ and overlapping kinematic contours were eliminated by particle identification. A least squares fit to the experimental triple correlation cross section for one geometry was made using two approximate theories for three body reactions. These were the Watson, and Phillips, Griffy and Biedenharn (P.G.B.) final state interaction theories. Both theories give the theoretical cross section to be proportional to a density of states (D.O.S.) function. The P.G.B. theory gives two forms for this function (P.G.B.1 and P.G.B.2). The D.O.S. functions for the state of He⁵ and Li⁵ were calculated using only the P.G.B. 1 and Watson forms. The P.G.B.1 form gives an inadequate description of both the n-p singlet and He⁵(g.s.) final state enhancements. The He⁵(g.s.) enhancement is well described by the Watson form of the D.O.S. function. The triple correlation cross section, for high proton energies, was dominated by a sequential breakup through the ground state of He⁵ and by direct three body breakup. No evidence for contributions from the states of Li⁵ or for any well defined contributions from the first excited state of He⁵ were observed. The Watson and P.G.B.2 forms of the singlet n-p D.O.S. function gave indistinguishable predictions of the n-p singlet enhancement. The P.G.B. 2 form was used, for seven values of the n-p singlet scattering length, to fit the experimental data. The value of the singlet n-p scattering length extracted in the fitting procedure was [formula omitted]. The large experimental errors assigned were caused by the sensitivity of the extracted value on the background terms included in each fit. === Science, Faculty of === Physics and Astronomy, Department of === Graduate
author Beveridge, John Leslie
author_facet Beveridge, John Leslie
author_sort Beveridge, John Leslie
title Final state interactions in the reaction T(He3, He4) np
title_short Final state interactions in the reaction T(He3, He4) np
title_full Final state interactions in the reaction T(He3, He4) np
title_fullStr Final state interactions in the reaction T(He3, He4) np
title_full_unstemmed Final state interactions in the reaction T(He3, He4) np
title_sort final state interactions in the reaction t(he3, he4) np
publisher University of British Columbia
publishDate 2011
url http://hdl.handle.net/2429/34699
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