Reaction He# (He3, 2p)He4 and the diproton state

The processes by which the three particle final state is formed in the He³(He³,2p)He⁴ reaction were investigated by observing the angular distribution of coincidence events between the two protons as a function of the angle between the protons. The reaction mechanism was determined by comparing...

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Main Author: Blackmore, Ewart William
Language:English
Published: University of British Columbia 2011
Subjects:
Online Access:http://hdl.handle.net/2429/37930
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spelling ndltd-UBC-oai-circle.library.ubc.ca-2429-379302018-01-05T17:49:04Z Reaction He# (He3, 2p)He4 and the diproton state Blackmore, Ewart William Particles (Nuclear physics) Helium -- Isotopes The processes by which the three particle final state is formed in the He³(He³,2p)He⁴ reaction were investigated by observing the angular distribution of coincidence events between the two protons as a function of the angle between the protons. The reaction mechanism was determined by comparing the experimental distribution with those predicted for the various possible processes obtained from kinematic and phase space arguments. The reaction was found to proceed predominantly by sequential decays through unbound intermediate states and to a lesser extent by a direct instantaneous three body breakup. The majority of the two stage decays passed through the ground state of Li⁵ , The mean lifetime of this state was measured and found to be (1.0 ± .3) x 10⁻²¹ sec There was also good evidence of a sequential decay through the diproton state. In order to fit the shape of the observed distribution it was necessary to assume that a diproton system exists which is unbound by 600 keV and has a mean lifetime of 1.5 x 10⁻²² sec However another possible interpretation is that a direct breakup occurs and the angular distribution of the protons is distorted by an attractive final state two proton interaction similar to the scattering interaction, although whether this interaction would be strong enough to produce the observed distribution is not known. A more quantitative three body decay theory is therefore necessary in order to draw any firm conclusions about the existence of the diproton state. Science, Faculty of Physics and Astronomy, Department of Graduate 2011-10-13T16:02:07Z 2011-10-13T16:02:07Z 1965 Text Thesis/Dissertation http://hdl.handle.net/2429/37930 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 Particles (Nuclear physics)
Helium -- Isotopes
spellingShingle Particles (Nuclear physics)
Helium -- Isotopes
Blackmore, Ewart William
Reaction He# (He3, 2p)He4 and the diproton state
description The processes by which the three particle final state is formed in the He³(He³,2p)He⁴ reaction were investigated by observing the angular distribution of coincidence events between the two protons as a function of the angle between the protons. The reaction mechanism was determined by comparing the experimental distribution with those predicted for the various possible processes obtained from kinematic and phase space arguments. The reaction was found to proceed predominantly by sequential decays through unbound intermediate states and to a lesser extent by a direct instantaneous three body breakup. The majority of the two stage decays passed through the ground state of Li⁵ , The mean lifetime of this state was measured and found to be (1.0 ± .3) x 10⁻²¹ sec There was also good evidence of a sequential decay through the diproton state. In order to fit the shape of the observed distribution it was necessary to assume that a diproton system exists which is unbound by 600 keV and has a mean lifetime of 1.5 x 10⁻²² sec However another possible interpretation is that a direct breakup occurs and the angular distribution of the protons is distorted by an attractive final state two proton interaction similar to the scattering interaction, although whether this interaction would be strong enough to produce the observed distribution is not known. A more quantitative three body decay theory is therefore necessary in order to draw any firm conclusions about the existence of the diproton state. === Science, Faculty of === Physics and Astronomy, Department of === Graduate
author Blackmore, Ewart William
author_facet Blackmore, Ewart William
author_sort Blackmore, Ewart William
title Reaction He# (He3, 2p)He4 and the diproton state
title_short Reaction He# (He3, 2p)He4 and the diproton state
title_full Reaction He# (He3, 2p)He4 and the diproton state
title_fullStr Reaction He# (He3, 2p)He4 and the diproton state
title_full_unstemmed Reaction He# (He3, 2p)He4 and the diproton state
title_sort reaction he# (he3, 2p)he4 and the diproton state
publisher University of British Columbia
publishDate 2011
url http://hdl.handle.net/2429/37930
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