Nuclear-Structure Effects on Parity Nonconservation in Light Nuclei

Brown, Bruce A.; Richter, W. A.; Godwin, N.S.

doi:10.1103/physrevlett.45.1681.2

Phys. Rev. Lett.

1980

DOI: 10.1103/physrevlett.45.1681.2

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Nuclear-Structure Effects on Parity Nonconservation in Light Nuclei

Bruce A. Brown

W. A. Richter

N.S. Godwin

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1994

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“…The calculation of the PNC matrix element which included both the core (inactive) and active orbitals has been performed as described in Ref. [27].…”

mentioning

confidence: 99%

Parity mixed doublets inA=36 nuclei

Horoi

1994

Phys. Rev. C

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The γ-circular polarizations (P γ ) and asymmetries (A γ ) of the parity forbidden M1 + E2 γ-decays: 36 Cl * (J π = 2 − ; T = 1; E x = 1.95 MeV) → 36 Cl(J π = 2 + ; T = 1; g.s.) and 36 Ar * (J π = 2 − ; T = 0; E x = 4.97 MeV) → 36 Ar * (J π = 2 + ; T = 0; E x = 1.97 MeV) are investigated theoretically. We use the recently proposed Warburton-Becker-Brown shell-model interaction.For the weak forces we discuss comparatively different weak interaction models based on different assumptions for evaluating the weak meson-hadron coupling constants. The results determine a range of P γ values from which we find the most probable values: P γ = 1.1 · 10 −4 for 36 Cl and P γ = 3.5 · 10 −4 for 36 Ar.

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“…The calculation of the PNC matrix element which included both the core (inactive) and active orbitals has been performed as described in Ref. [27].…”

mentioning

confidence: 99%

Parity mixed doublets inA=36 nuclei

Horoi

1994

Phys. Rev. C

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show abstract

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Nuclear-Structure Effects on Parity Nonconservation in Light Nuclei

Cited by 1 publication

References 0 publications

Parity mixed doublets inA=36 nuclei

Parity mixed doublets inA=36 nuclei

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