Microscopic band-mixing calculations $ in^{154,156} $Gd
Abstract A many-body microscopic band-mixing formulation of variation after projection of angular momentum and conservation of nucleon number is used to study the yrast band and first excitedKπ=$ 0^{+} $ band in the doubly even $ nuclei^{154,156} $Gd. The computed energy spectra and the interband an...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Moholkar, S V [verfasserIn] |
|---|
| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1980 |
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| Schlagwörter: |
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| Anmerkung: |
© Indian Academy of Sciences 1980 |
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| Übergeordnetes Werk: |
Enthalten in: Pramāna - Springer India, 1973, 15(1980), 5 vom: Nov., Seite 449-461 |
|---|---|
| Übergeordnetes Werk: |
volume:15 ; year:1980 ; number:5 ; month:11 ; pages:449-461 |
| Links: |
|---|
| DOI / URN: |
10.1007/BF02847883 |
|---|
| Katalog-ID: |
OLC2076007911 |
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| 520 | |a Abstract A many-body microscopic band-mixing formulation of variation after projection of angular momentum and conservation of nucleon number is used to study the yrast band and first excitedKπ=$ 0^{+} $ band in the doubly even $ nuclei^{154,156} $Gd. The computed energy spectra and the interband and intra-band B (E2) values are in good agreement with corresponding experimental data. Connection with the phenomenological model of Stephens and Simon is discussed, bringing out the role played by thei13/2 neutron pair in the microscopic formalism. | ||
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10.1007/BF02847883 doi (DE-627)OLC2076007911 (DE-He213)BF02847883-p DE-627 ger DE-627 rakwb eng 530 VZ Moholkar, S V verfasserin aut Microscopic band-mixing calculations $ in^{154,156} $Gd 1980 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1980 Abstract A many-body microscopic band-mixing formulation of variation after projection of angular momentum and conservation of nucleon number is used to study the yrast band and first excitedKπ=$ 0^{+} $ band in the doubly even $ nuclei^{154,156} $Gd. The computed energy spectra and the interband and intra-band B (E2) values are in good agreement with corresponding experimental data. Connection with the phenomenological model of Stephens and Simon is discussed, bringing out the role played by thei13/2 neutron pair in the microscopic formalism. Nuclear structure Gd yrast band first excited band energy spectra interband and intraband B(E2) values band-mixing angular momentum projection conservation of nucleon number Warke, C S aut Gunye, M R aut Enthalten in Pramāna Springer India, 1973 15(1980), 5 vom: Nov., Seite 449-461 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:15 year:1980 number:5 month:11 pages:449-461 https://doi.org/10.1007/BF02847883 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_21 GBV_ILN_24 GBV_ILN_40 GBV_ILN_70 GBV_ILN_179 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4309 AR 15 1980 5 11 449-461 |
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10.1007/BF02847883 doi (DE-627)OLC2076007911 (DE-He213)BF02847883-p DE-627 ger DE-627 rakwb eng 530 VZ Moholkar, S V verfasserin aut Microscopic band-mixing calculations $ in^{154,156} $Gd 1980 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1980 Abstract A many-body microscopic band-mixing formulation of variation after projection of angular momentum and conservation of nucleon number is used to study the yrast band and first excitedKπ=$ 0^{+} $ band in the doubly even $ nuclei^{154,156} $Gd. The computed energy spectra and the interband and intra-band B (E2) values are in good agreement with corresponding experimental data. Connection with the phenomenological model of Stephens and Simon is discussed, bringing out the role played by thei13/2 neutron pair in the microscopic formalism. Nuclear structure Gd yrast band first excited band energy spectra interband and intraband B(E2) values band-mixing angular momentum projection conservation of nucleon number Warke, C S aut Gunye, M R aut Enthalten in Pramāna Springer India, 1973 15(1980), 5 vom: Nov., Seite 449-461 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:15 year:1980 number:5 month:11 pages:449-461 https://doi.org/10.1007/BF02847883 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_21 GBV_ILN_24 GBV_ILN_40 GBV_ILN_70 GBV_ILN_179 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4309 AR 15 1980 5 11 449-461 |
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10.1007/BF02847883 doi (DE-627)OLC2076007911 (DE-He213)BF02847883-p DE-627 ger DE-627 rakwb eng 530 VZ Moholkar, S V verfasserin aut Microscopic band-mixing calculations $ in^{154,156} $Gd 1980 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1980 Abstract A many-body microscopic band-mixing formulation of variation after projection of angular momentum and conservation of nucleon number is used to study the yrast band and first excitedKπ=$ 0^{+} $ band in the doubly even $ nuclei^{154,156} $Gd. The computed energy spectra and the interband and intra-band B (E2) values are in good agreement with corresponding experimental data. Connection with the phenomenological model of Stephens and Simon is discussed, bringing out the role played by thei13/2 neutron pair in the microscopic formalism. Nuclear structure Gd yrast band first excited band energy spectra interband and intraband B(E2) values band-mixing angular momentum projection conservation of nucleon number Warke, C S aut Gunye, M R aut Enthalten in Pramāna Springer India, 1973 15(1980), 5 vom: Nov., Seite 449-461 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:15 year:1980 number:5 month:11 pages:449-461 https://doi.org/10.1007/BF02847883 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_21 GBV_ILN_24 GBV_ILN_40 GBV_ILN_70 GBV_ILN_179 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4309 AR 15 1980 5 11 449-461 |
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10.1007/BF02847883 doi (DE-627)OLC2076007911 (DE-He213)BF02847883-p DE-627 ger DE-627 rakwb eng 530 VZ Moholkar, S V verfasserin aut Microscopic band-mixing calculations $ in^{154,156} $Gd 1980 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1980 Abstract A many-body microscopic band-mixing formulation of variation after projection of angular momentum and conservation of nucleon number is used to study the yrast band and first excitedKπ=$ 0^{+} $ band in the doubly even $ nuclei^{154,156} $Gd. The computed energy spectra and the interband and intra-band B (E2) values are in good agreement with corresponding experimental data. Connection with the phenomenological model of Stephens and Simon is discussed, bringing out the role played by thei13/2 neutron pair in the microscopic formalism. Nuclear structure Gd yrast band first excited band energy spectra interband and intraband B(E2) values band-mixing angular momentum projection conservation of nucleon number Warke, C S aut Gunye, M R aut Enthalten in Pramāna Springer India, 1973 15(1980), 5 vom: Nov., Seite 449-461 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:15 year:1980 number:5 month:11 pages:449-461 https://doi.org/10.1007/BF02847883 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_21 GBV_ILN_24 GBV_ILN_40 GBV_ILN_70 GBV_ILN_179 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4309 AR 15 1980 5 11 449-461 |
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10.1007/BF02847883 doi (DE-627)OLC2076007911 (DE-He213)BF02847883-p DE-627 ger DE-627 rakwb eng 530 VZ Moholkar, S V verfasserin aut Microscopic band-mixing calculations $ in^{154,156} $Gd 1980 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 1980 Abstract A many-body microscopic band-mixing formulation of variation after projection of angular momentum and conservation of nucleon number is used to study the yrast band and first excitedKπ=$ 0^{+} $ band in the doubly even $ nuclei^{154,156} $Gd. The computed energy spectra and the interband and intra-band B (E2) values are in good agreement with corresponding experimental data. Connection with the phenomenological model of Stephens and Simon is discussed, bringing out the role played by thei13/2 neutron pair in the microscopic formalism. Nuclear structure Gd yrast band first excited band energy spectra interband and intraband B(E2) values band-mixing angular momentum projection conservation of nucleon number Warke, C S aut Gunye, M R aut Enthalten in Pramāna Springer India, 1973 15(1980), 5 vom: Nov., Seite 449-461 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:15 year:1980 number:5 month:11 pages:449-461 https://doi.org/10.1007/BF02847883 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_11 GBV_ILN_21 GBV_ILN_24 GBV_ILN_40 GBV_ILN_70 GBV_ILN_179 GBV_ILN_2014 GBV_ILN_2020 GBV_ILN_4309 AR 15 1980 5 11 449-461 |
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microscopic band-mixing calculations $ in^{154,156} $gd |
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Abstract A many-body microscopic band-mixing formulation of variation after projection of angular momentum and conservation of nucleon number is used to study the yrast band and first excitedKπ=$ 0^{+} $ band in the doubly even $ nuclei^{154,156} $Gd. The computed energy spectra and the interband and intra-band B (E2) values are in good agreement with corresponding experimental data. Connection with the phenomenological model of Stephens and Simon is discussed, bringing out the role played by thei13/2 neutron pair in the microscopic formalism. © Indian Academy of Sciences 1980 |
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Abstract A many-body microscopic band-mixing formulation of variation after projection of angular momentum and conservation of nucleon number is used to study the yrast band and first excitedKπ=$ 0^{+} $ band in the doubly even $ nuclei^{154,156} $Gd. The computed energy spectra and the interband and intra-band B (E2) values are in good agreement with corresponding experimental data. Connection with the phenomenological model of Stephens and Simon is discussed, bringing out the role played by thei13/2 neutron pair in the microscopic formalism. © Indian Academy of Sciences 1980 |
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Abstract A many-body microscopic band-mixing formulation of variation after projection of angular momentum and conservation of nucleon number is used to study the yrast band and first excitedKπ=$ 0^{+} $ band in the doubly even $ nuclei^{154,156} $Gd. The computed energy spectra and the interband and intra-band B (E2) values are in good agreement with corresponding experimental data. Connection with the phenomenological model of Stephens and Simon is discussed, bringing out the role played by thei13/2 neutron pair in the microscopic formalism. © Indian Academy of Sciences 1980 |
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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">OLC2076007911</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230402042316.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200820s1980 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/BF02847883</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2076007911</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)BF02847883-p</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="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Moholkar, S V</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Microscopic band-mixing calculations $ in^{154,156} $Gd</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1980</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Indian Academy of Sciences 1980</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract A many-body microscopic band-mixing formulation of variation after projection of angular momentum and conservation of nucleon number is used to study the yrast band and first excitedKπ=$ 0^{+} $ band in the doubly even $ nuclei^{154,156} $Gd. The computed energy spectra and the interband and intra-band B (E2) values are in good agreement with corresponding experimental data. Connection with the phenomenological model of Stephens and Simon is discussed, bringing out the role played by thei13/2 neutron pair in the microscopic formalism.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Nuclear structure</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Gd</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">yrast band</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">first excited band</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">energy spectra</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">interband and intraband B(E2) values</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">band-mixing</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">angular momentum projection</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">conservation of nucleon number</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Warke, C S</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Gunye, M R</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Pramāna</subfield><subfield code="d">Springer India, 1973</subfield><subfield code="g">15(1980), 5 vom: Nov., Seite 449-461</subfield><subfield code="w">(DE-627)129403342</subfield><subfield code="w">(DE-600)186949-8</subfield><subfield code="w">(DE-576)014785102</subfield><subfield code="x">0304-4289</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:15</subfield><subfield code="g">year:1980</subfield><subfield code="g">number:5</subfield><subfield code="g">month:11</subfield><subfield code="g">pages:449-461</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/BF02847883</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_11</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_21</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_24</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_179</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2020</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4309</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">15</subfield><subfield code="j">1980</subfield><subfield code="e">5</subfield><subfield code="c">11</subfield><subfield code="h">449-461</subfield></datafield></record></collection>
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