Nuclear matrix elements of the first forbidden beta transitions in the decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2
The ratio of the coordinate type matrix elements involved in the beta decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 have been computed with the help of the jj coupling of the shell model. The theoretical functions for the observable quantities are compared with the available experimental data a...
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1965 |
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| Reproduktion: |
Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 |
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| Übergeordnetes Werk: |
in: Nuclear Physics - Amsterdam : Elsevier, 65(1965), 1, Seite 21-32 |
| Übergeordnetes Werk: |
volume:65 ; year:1965 ; number:1 ; pages:21-32 |
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| 245 | 1 | 0 | |a Nuclear matrix elements of the first forbidden beta transitions in the decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 |
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| 520 | |a The ratio of the coordinate type matrix elements involved in the beta decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 have been computed with the help of the jj coupling of the shell model. The theoretical functions for the observable quantities are compared with the available experimental data and exhibit a qualitative agreement. The ratio Λ"0 = -∫iγ"5/ξ∫σ . r is computed to be Λ"0 ~ 1 for the Ce^1^4^172^-(β)Pr^1^4^172^+ transition and 1.3 Λ"0 2 for the Pr^1^4^22^-(β)Nd^1^4^22^+ transition; these values are obtained from the comparison between the measured polarization of the β and circularly γ correlation and the theoretical function. | ||
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(DE-627)NLEJ180631926 (DE-599)GBVNLZ180631926 DE-627 ger DE-627 rakwb eng Nuclear matrix elements of the first forbidden beta transitions in the decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 1965 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The ratio of the coordinate type matrix elements involved in the beta decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 have been computed with the help of the jj coupling of the shell model. The theoretical functions for the observable quantities are compared with the available experimental data and exhibit a qualitative agreement. The ratio Λ"0 = -∫iγ"5/ξ∫σ . r is computed to be Λ"0 ~ 1 for the Ce^1^4^172^-(β)Pr^1^4^172^+ transition and 1.3 Λ"0 2 for the Pr^1^4^22^-(β)Nd^1^4^22^+ transition; these values are obtained from the comparison between the measured polarization of the β and circularly γ correlation and the theoretical function. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Lipnik, P. oth Sunier, J.W. oth in Nuclear Physics Amsterdam : Elsevier 65(1965), 1, Seite 21-32 (DE-627)NLEJ177048727 (DE-600)2242383-7 0029-5582 nnns volume:65 year:1965 number:1 pages:21-32 http://linkinghub.elsevier.com/retrieve/pii/0029-5582(65)90291-9 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 65 1965 1 21-32 |
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(DE-627)NLEJ180631926 (DE-599)GBVNLZ180631926 DE-627 ger DE-627 rakwb eng Nuclear matrix elements of the first forbidden beta transitions in the decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 1965 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The ratio of the coordinate type matrix elements involved in the beta decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 have been computed with the help of the jj coupling of the shell model. The theoretical functions for the observable quantities are compared with the available experimental data and exhibit a qualitative agreement. The ratio Λ"0 = -∫iγ"5/ξ∫σ . r is computed to be Λ"0 ~ 1 for the Ce^1^4^172^-(β)Pr^1^4^172^+ transition and 1.3 Λ"0 2 for the Pr^1^4^22^-(β)Nd^1^4^22^+ transition; these values are obtained from the comparison between the measured polarization of the β and circularly γ correlation and the theoretical function. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Lipnik, P. oth Sunier, J.W. oth in Nuclear Physics Amsterdam : Elsevier 65(1965), 1, Seite 21-32 (DE-627)NLEJ177048727 (DE-600)2242383-7 0029-5582 nnns volume:65 year:1965 number:1 pages:21-32 http://linkinghub.elsevier.com/retrieve/pii/0029-5582(65)90291-9 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 65 1965 1 21-32 |
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(DE-627)NLEJ180631926 (DE-599)GBVNLZ180631926 DE-627 ger DE-627 rakwb eng Nuclear matrix elements of the first forbidden beta transitions in the decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 1965 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The ratio of the coordinate type matrix elements involved in the beta decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 have been computed with the help of the jj coupling of the shell model. The theoretical functions for the observable quantities are compared with the available experimental data and exhibit a qualitative agreement. The ratio Λ"0 = -∫iγ"5/ξ∫σ . r is computed to be Λ"0 ~ 1 for the Ce^1^4^172^-(β)Pr^1^4^172^+ transition and 1.3 Λ"0 2 for the Pr^1^4^22^-(β)Nd^1^4^22^+ transition; these values are obtained from the comparison between the measured polarization of the β and circularly γ correlation and the theoretical function. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Lipnik, P. oth Sunier, J.W. oth in Nuclear Physics Amsterdam : Elsevier 65(1965), 1, Seite 21-32 (DE-627)NLEJ177048727 (DE-600)2242383-7 0029-5582 nnns volume:65 year:1965 number:1 pages:21-32 http://linkinghub.elsevier.com/retrieve/pii/0029-5582(65)90291-9 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 65 1965 1 21-32 |
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(DE-627)NLEJ180631926 (DE-599)GBVNLZ180631926 DE-627 ger DE-627 rakwb eng Nuclear matrix elements of the first forbidden beta transitions in the decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 1965 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The ratio of the coordinate type matrix elements involved in the beta decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 have been computed with the help of the jj coupling of the shell model. The theoretical functions for the observable quantities are compared with the available experimental data and exhibit a qualitative agreement. The ratio Λ"0 = -∫iγ"5/ξ∫σ . r is computed to be Λ"0 ~ 1 for the Ce^1^4^172^-(β)Pr^1^4^172^+ transition and 1.3 Λ"0 2 for the Pr^1^4^22^-(β)Nd^1^4^22^+ transition; these values are obtained from the comparison between the measured polarization of the β and circularly γ correlation and the theoretical function. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Lipnik, P. oth Sunier, J.W. oth in Nuclear Physics Amsterdam : Elsevier 65(1965), 1, Seite 21-32 (DE-627)NLEJ177048727 (DE-600)2242383-7 0029-5582 nnns volume:65 year:1965 number:1 pages:21-32 http://linkinghub.elsevier.com/retrieve/pii/0029-5582(65)90291-9 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 65 1965 1 21-32 |
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(DE-627)NLEJ180631926 (DE-599)GBVNLZ180631926 DE-627 ger DE-627 rakwb eng Nuclear matrix elements of the first forbidden beta transitions in the decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 1965 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The ratio of the coordinate type matrix elements involved in the beta decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 have been computed with the help of the jj coupling of the shell model. The theoretical functions for the observable quantities are compared with the available experimental data and exhibit a qualitative agreement. The ratio Λ"0 = -∫iγ"5/ξ∫σ . r is computed to be Λ"0 ~ 1 for the Ce^1^4^172^-(β)Pr^1^4^172^+ transition and 1.3 Λ"0 2 for the Pr^1^4^22^-(β)Nd^1^4^22^+ transition; these values are obtained from the comparison between the measured polarization of the β and circularly γ correlation and the theoretical function. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Lipnik, P. oth Sunier, J.W. oth in Nuclear Physics Amsterdam : Elsevier 65(1965), 1, Seite 21-32 (DE-627)NLEJ177048727 (DE-600)2242383-7 0029-5582 nnns volume:65 year:1965 number:1 pages:21-32 http://linkinghub.elsevier.com/retrieve/pii/0029-5582(65)90291-9 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 65 1965 1 21-32 |
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Nuclear matrix elements of the first forbidden beta transitions in the decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 |
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nuclear matrix elements of the first forbidden beta transitions in the decay of ba^1^3^9, ce^1^4^1, la^1^4^0 and pr^1^4^2 |
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Nuclear matrix elements of the first forbidden beta transitions in the decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 |
| abstract |
The ratio of the coordinate type matrix elements involved in the beta decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 have been computed with the help of the jj coupling of the shell model. The theoretical functions for the observable quantities are compared with the available experimental data and exhibit a qualitative agreement. The ratio Λ"0 = -∫iγ"5/ξ∫σ . r is computed to be Λ"0 ~ 1 for the Ce^1^4^172^-(β)Pr^1^4^172^+ transition and 1.3 Λ"0 2 for the Pr^1^4^22^-(β)Nd^1^4^22^+ transition; these values are obtained from the comparison between the measured polarization of the β and circularly γ correlation and the theoretical function. |
| abstractGer |
The ratio of the coordinate type matrix elements involved in the beta decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 have been computed with the help of the jj coupling of the shell model. The theoretical functions for the observable quantities are compared with the available experimental data and exhibit a qualitative agreement. The ratio Λ"0 = -∫iγ"5/ξ∫σ . r is computed to be Λ"0 ~ 1 for the Ce^1^4^172^-(β)Pr^1^4^172^+ transition and 1.3 Λ"0 2 for the Pr^1^4^22^-(β)Nd^1^4^22^+ transition; these values are obtained from the comparison between the measured polarization of the β and circularly γ correlation and the theoretical function. |
| abstract_unstemmed |
The ratio of the coordinate type matrix elements involved in the beta decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 have been computed with the help of the jj coupling of the shell model. The theoretical functions for the observable quantities are compared with the available experimental data and exhibit a qualitative agreement. The ratio Λ"0 = -∫iγ"5/ξ∫σ . r is computed to be Λ"0 ~ 1 for the Ce^1^4^172^-(β)Pr^1^4^172^+ transition and 1.3 Λ"0 2 for the Pr^1^4^22^-(β)Nd^1^4^22^+ transition; these values are obtained from the comparison between the measured polarization of the β and circularly γ correlation and the theoretical function. |
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Nuclear matrix elements of the first forbidden beta transitions in the decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">NLEJ180631926</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20210706132512.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">070505s1965 xx |||||o 00| ||eng c</controlfield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)NLEJ180631926</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)GBVNLZ180631926</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Nuclear matrix elements of the first forbidden beta transitions in the decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1965</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zzz</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">z</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zu</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">The ratio of the coordinate type matrix elements involved in the beta decay of Ba^1^3^9, Ce^1^4^1, La^1^4^0 and Pr^1^4^2 have been computed with the help of the jj coupling of the shell model. The theoretical functions for the observable quantities are compared with the available experimental data and exhibit a qualitative agreement. The ratio Λ"0 = -∫iγ"5/ξ∫σ . r is computed to be Λ"0 ~ 1 for the Ce^1^4^172^-(β)Pr^1^4^172^+ transition and 1.3 Λ"0 2 for the Pr^1^4^22^-(β)Nd^1^4^22^+ transition; these values are obtained from the comparison between the measured polarization of the β and circularly γ correlation and the theoretical function.</subfield></datafield><datafield tag="533" ind1=" " ind2=" "><subfield code="f">Elsevier Journal Backfiles on ScienceDirect 1907 - 2002</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Lipnik, P.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Sunier, J.W.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">in</subfield><subfield code="t">Nuclear Physics</subfield><subfield code="d">Amsterdam : Elsevier</subfield><subfield code="g">65(1965), 1, Seite 21-32</subfield><subfield code="w">(DE-627)NLEJ177048727</subfield><subfield code="w">(DE-600)2242383-7</subfield><subfield code="x">0029-5582</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:65</subfield><subfield code="g">year:1965</subfield><subfield code="g">number:1</subfield><subfield code="g">pages:21-32</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">http://linkinghub.elsevier.com/retrieve/pii/0029-5582(65)90291-9</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_H</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">ZDB-1-SDJ</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_NL_ARTICLE</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">65</subfield><subfield code="j">1965</subfield><subfield code="e">1</subfield><subfield code="h">21-32</subfield></datafield></record></collection>
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