Experimental study of time reversal invariance and atomic final state effects in nuclear transitions

Experiments have been performed to test time reversal invariance in nuclei using gamma transitions of oriented <sup>191</sup>Ir and <sup>131</sup>Xe. The phase angle η associated with the imaginary part of the ratio of reduced matrix elements of the gamma transition was m...

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Main Author: Gimlett, James L.
Format: Others
Language:en
Published: 1980
Online Access:https://thesis.library.caltech.edu/9961/1/Gimlett_jl_1980.pdf
Gimlett, James L. (1980) Experimental study of time reversal invariance and atomic final state effects in nuclear transitions. Dissertation (Ph.D.), California Institute of Technology. doi:10.7907/n7sw-jy41. https://resolver.caltech.edu/CaltechTHESIS:10272016-131924862 <https://resolver.caltech.edu/CaltechTHESIS:10272016-131924862>
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spelling ndltd-CALTECH-oai-thesis.library.caltech.edu-99612021-04-17T05:02:07Z https://thesis.library.caltech.edu/9961/ Experimental study of time reversal invariance and atomic final state effects in nuclear transitions Gimlett, James L. Experiments have been performed to test time reversal invariance in nuclei using gamma transitions of oriented <sup>191</sup>Ir and <sup>131</sup>Xe. The phase angle η associated with the imaginary part of the ratio of reduced matrix elements of the gamma transition was measured through observation of the angular distribution of the linear polarization from oriented nuclei. Interaction of the gamma ray with the atomic electron cloud can cause an additional phase shift ξ which is indistinguishable from the time-reversal phase η. Such an atomic final state effect has been observed for the 129 keV transition in <sup>191</sup>Ir. Nuclear orientation was achieved with a large magnetic field (the hyperfine field of Ir in iron) and low temperature (20 to 30 mK obtained with a dilution refrigerator). A Compton polarimeter was used to measure linear polarization of the E2-Ml gamma ray. The matrix-element ratio was found to have an imaginary part corresponding to a phase angle (η+ξ) = (-4.8 ± 0.2) x 10<sup>-3</sup>. This measurement is in agreement with the most recent final state calculations which give ξ = (-4.3 ± 0.4) x 10<sup>-3</sup>. A limit |η| &#60; 10<sup>-3</sup> is deduced for the time-reversal phase. In another experiment a phase angle η = (-1.2 ± 1.1) x 10<sup>-3</sup> was measured for the E2-Ml 364 keV transition in <sup>131</sup>Xe, for which atomic final state effects are small. Both measurements are consistent with time reversal invariance. 1980 Thesis NonPeerReviewed application/pdf en other https://thesis.library.caltech.edu/9961/1/Gimlett_jl_1980.pdf Gimlett, James L. (1980) Experimental study of time reversal invariance and atomic final state effects in nuclear transitions. Dissertation (Ph.D.), California Institute of Technology. doi:10.7907/n7sw-jy41. https://resolver.caltech.edu/CaltechTHESIS:10272016-131924862 <https://resolver.caltech.edu/CaltechTHESIS:10272016-131924862> https://resolver.caltech.edu/CaltechTHESIS:10272016-131924862 CaltechTHESIS:10272016-131924862 10.7907/n7sw-jy41
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language en
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sources NDLTD
description Experiments have been performed to test time reversal invariance in nuclei using gamma transitions of oriented <sup>191</sup>Ir and <sup>131</sup>Xe. The phase angle η associated with the imaginary part of the ratio of reduced matrix elements of the gamma transition was measured through observation of the angular distribution of the linear polarization from oriented nuclei. Interaction of the gamma ray with the atomic electron cloud can cause an additional phase shift ξ which is indistinguishable from the time-reversal phase η. Such an atomic final state effect has been observed for the 129 keV transition in <sup>191</sup>Ir. Nuclear orientation was achieved with a large magnetic field (the hyperfine field of Ir in iron) and low temperature (20 to 30 mK obtained with a dilution refrigerator). A Compton polarimeter was used to measure linear polarization of the E2-Ml gamma ray. The matrix-element ratio was found to have an imaginary part corresponding to a phase angle (η+ξ) = (-4.8 ± 0.2) x 10<sup>-3</sup>. This measurement is in agreement with the most recent final state calculations which give ξ = (-4.3 ± 0.4) x 10<sup>-3</sup>. A limit |η| &#60; 10<sup>-3</sup> is deduced for the time-reversal phase. In another experiment a phase angle η = (-1.2 ± 1.1) x 10<sup>-3</sup> was measured for the E2-Ml 364 keV transition in <sup>131</sup>Xe, for which atomic final state effects are small. Both measurements are consistent with time reversal invariance.
author Gimlett, James L.
spellingShingle Gimlett, James L.
Experimental study of time reversal invariance and atomic final state effects in nuclear transitions
author_facet Gimlett, James L.
author_sort Gimlett, James L.
title Experimental study of time reversal invariance and atomic final state effects in nuclear transitions
title_short Experimental study of time reversal invariance and atomic final state effects in nuclear transitions
title_full Experimental study of time reversal invariance and atomic final state effects in nuclear transitions
title_fullStr Experimental study of time reversal invariance and atomic final state effects in nuclear transitions
title_full_unstemmed Experimental study of time reversal invariance and atomic final state effects in nuclear transitions
title_sort experimental study of time reversal invariance and atomic final state effects in nuclear transitions
publishDate 1980
url https://thesis.library.caltech.edu/9961/1/Gimlett_jl_1980.pdf
Gimlett, James L. (1980) Experimental study of time reversal invariance and atomic final state effects in nuclear transitions. Dissertation (Ph.D.), California Institute of Technology. doi:10.7907/n7sw-jy41. https://resolver.caltech.edu/CaltechTHESIS:10272016-131924862 <https://resolver.caltech.edu/CaltechTHESIS:10272016-131924862>
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