1990
DOI: 10.1016/0375-9474(90)90384-x
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Parity assignments in nuclear resonance fluorescence experiments using compton polarimeters

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Cited by 39 publications
(2 citation statements)
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“…where 0 1,1' and O~'I' are the two-body terms (11 ) (12) (13) with (15) Introducing el:=ajd, Xl := ap./ajd and X~ := adp/ajd, the T(El)-operator is finally written as: (16) The parameter el is the "effective charge". The structural parameters Xl and X~ weighing the different two-body terms depend (from our assumption) only on the total number of bosons.…”
Section: El·transitions In Well Deformed Nuclei In the Framework Of Tmentioning
confidence: 99%
“…where 0 1,1' and O~'I' are the two-body terms (11 ) (12) (13) with (15) Introducing el:=ajd, Xl := ap./ajd and X~ := adp/ajd, the T(El)-operator is finally written as: (16) The parameter el is the "effective charge". The structural parameters Xl and X~ weighing the different two-body terms depend (from our assumption) only on the total number of bosons.…”
Section: El·transitions In Well Deformed Nuclei In the Framework Of Tmentioning
confidence: 99%
“…Measurements of the linear polarization using the polarization dependence of Compton scattering (generally denoted as Compton polarimetry) have proven to be a reliable tool for model-independent parity assignments at energies up to about 4 MeV [12][13][14][15][16][17][18]. At these energies the analyzing power of the Compton effect has dropped already significantly and reliable parity assignments become difficult [19].…”
Section: Introductionmentioning
confidence: 98%