Parity mixed doublets in A=36 nuclei

Mihai Horoi

doi:10.1103/PhysRevC.50.2392

Parity mixed doublets in A=36 nuclei

Mihai Horoi

Physics

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3 Scopus citations

Abstract

The -circular polarizations (P) and asymmetries (A) of the parity forbidden M1+E2 decays, Cl*36(J=2-;T=1;Ex=1.95 MeV)36Cl(J=2+;T=1; g.s.) and Ar*36(J=2-;T=0;Ex=4.97 MeV) 36Ar*(J-2+;T=0;Ex=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 evaluationg the weak meson-hadron coupling constants. The results determine a range of P values from which we find the most probable values: P=1.1×10-4 for Cl36 and P=3.5×10-4 for Ar36.

Original language	English
Pages (from-to)	2392-2397
Number of pages	6
Journal	Physical Review C - Nuclear Physics
Volume	50
Issue number	5
DOIs	https://doi.org/10.1103/PhysRevC.50.2392
State	Published - 1994

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10.1103/PhysRevC.50.2392

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title = "Parity mixed doublets in A=36 nuclei",

abstract = "The -circular polarizations (P) and asymmetries (A) of the parity forbidden M1+E2 decays, Cl*36(J=2-;T=1;Ex=1.95 MeV)36Cl(J=2+;T=1; g.s.) and Ar*36(J=2-;T=0;Ex=4.97 MeV) 36Ar*(J-2+;T=0;Ex=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 evaluationg the weak meson-hadron coupling constants. The results determine a range of P values from which we find the most probable values: P=1.1×10-4 for Cl36 and P=3.5×10-4 for Ar36.",

author = "Mihai Horoi",

year = "1994",

doi = "10.1103/PhysRevC.50.2392",

language = "English",

volume = "50",

pages = "2392--2397",

journal = "Physical Review C - Nuclear Physics",

issn = "0556-2813",

number = "5",

}

TY - JOUR

T1 - Parity mixed doublets in A=36 nuclei

AU - Horoi, Mihai

PY - 1994

Y1 - 1994

N2 - The -circular polarizations (P) and asymmetries (A) of the parity forbidden M1+E2 decays, Cl*36(J=2-;T=1;Ex=1.95 MeV)36Cl(J=2+;T=1; g.s.) and Ar*36(J=2-;T=0;Ex=4.97 MeV) 36Ar*(J-2+;T=0;Ex=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 evaluationg the weak meson-hadron coupling constants. The results determine a range of P values from which we find the most probable values: P=1.1×10-4 for Cl36 and P=3.5×10-4 for Ar36.

AB - The -circular polarizations (P) and asymmetries (A) of the parity forbidden M1+E2 decays, Cl*36(J=2-;T=1;Ex=1.95 MeV)36Cl(J=2+;T=1; g.s.) and Ar*36(J=2-;T=0;Ex=4.97 MeV) 36Ar*(J-2+;T=0;Ex=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 evaluationg the weak meson-hadron coupling constants. The results determine a range of P values from which we find the most probable values: P=1.1×10-4 for Cl36 and P=3.5×10-4 for Ar36.

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DO - 10.1103/PhysRevC.50.2392

M3 - Article

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EP - 2397

JO - Physical Review C - Nuclear Physics

JF - Physical Review C - Nuclear Physics

SN - 0556-2813

IS - 5

ER -

Parity mixed doublets in A=36 nuclei

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