E1 transitions in F17. II. The region of the giant resonances
The giant dipole resonance of F17 was studied by radiative proton capture. An observed integrated strength of 10 MeV mb, presumably mostly T=12, is centered at 22 MeV with a width of ~ 5 MeV. Calculations were performed for odd-parity 2p-1h, 1p excitations in a basis of good isospin. These calculati...
Ausführliche Beschreibung
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1975 |
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Online-Ressource 7 |
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Enthalten in: Physical review / C - Woodbury, NY : Inst., 1970, 11(1975), 3, Seite 1008-1014 |
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volume:11 ; year:1975 ; number:3 ; pages:1008-1014 ; extent:7 |
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520 | |a The giant dipole resonance of F17 was studied by radiative proton capture. An observed integrated strength of 10 MeV mb, presumably mostly T=12, is centered at 22 MeV with a width of ~ 5 MeV. Calculations were performed for odd-parity 2p-1h, 1p excitations in a basis of good isospin. These calculations predict correctly the observed strength distribution. Some general rules for the T components of the E1 collective state are consistent with the microscopic calculation. The f72→d52 strength was located near 18 MeV, in agreement with other experimental evidence.NUCLEAR REACTIONS F17, O16(p, γ), Ep=15.75-31.66 MeV. Measured dσdΩ(90°). Measured angular distributions deduced ET=12 of GDR. Calculated 1p and 2p-1h states of F17. Compared with experimental results. | ||
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(DE-627)NLEJ24990215X (DE-601)aps:9c05f74a758a7bb95bd8f4951f001f7281c7d100 DE-627 ger DE-627 rakwb E1 transitions in F17. II. The region of the giant resonances 1975 Online-Ressource 7 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The giant dipole resonance of F17 was studied by radiative proton capture. An observed integrated strength of 10 MeV mb, presumably mostly T=12, is centered at 22 MeV with a width of ~ 5 MeV. Calculations were performed for odd-parity 2p-1h, 1p excitations in a basis of good isospin. These calculations predict correctly the observed strength distribution. Some general rules for the T components of the E1 collective state are consistent with the microscopic calculation. The f72→d52 strength was located near 18 MeV, in agreement with other experimental evidence.NUCLEAR REACTIONS F17, O16(p, γ), Ep=15.75-31.66 MeV. Measured dσdΩ(90°). Measured angular distributions deduced ET=12 of GDR. Calculated 1p and 2p-1h states of F17. Compared with experimental results. APS Digital Backfile Archive 1893-2003 Harakeh, M. N. oth Paul, P. oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 11(1975), 3, Seite 1008-1014 Online-Ressource (DE-627)NLEJ24823787X (DE-600)1461161-2 1089-490X nnns volume:11 year:1975 number:3 pages:1008-1014 extent:7 https://www.tib.eu/de/suchen/id/aps%3A9c05f74a758a7bb95bd8f4951f001f7281c7d100 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 11 1975 3 1008-1014 7 |
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(DE-627)NLEJ24990215X (DE-601)aps:9c05f74a758a7bb95bd8f4951f001f7281c7d100 DE-627 ger DE-627 rakwb E1 transitions in F17. II. The region of the giant resonances 1975 Online-Ressource 7 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The giant dipole resonance of F17 was studied by radiative proton capture. An observed integrated strength of 10 MeV mb, presumably mostly T=12, is centered at 22 MeV with a width of ~ 5 MeV. Calculations were performed for odd-parity 2p-1h, 1p excitations in a basis of good isospin. These calculations predict correctly the observed strength distribution. Some general rules for the T components of the E1 collective state are consistent with the microscopic calculation. The f72→d52 strength was located near 18 MeV, in agreement with other experimental evidence.NUCLEAR REACTIONS F17, O16(p, γ), Ep=15.75-31.66 MeV. Measured dσdΩ(90°). Measured angular distributions deduced ET=12 of GDR. Calculated 1p and 2p-1h states of F17. Compared with experimental results. APS Digital Backfile Archive 1893-2003 Harakeh, M. N. oth Paul, P. oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 11(1975), 3, Seite 1008-1014 Online-Ressource (DE-627)NLEJ24823787X (DE-600)1461161-2 1089-490X nnns volume:11 year:1975 number:3 pages:1008-1014 extent:7 https://www.tib.eu/de/suchen/id/aps%3A9c05f74a758a7bb95bd8f4951f001f7281c7d100 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 11 1975 3 1008-1014 7 |
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(DE-627)NLEJ24990215X (DE-601)aps:9c05f74a758a7bb95bd8f4951f001f7281c7d100 DE-627 ger DE-627 rakwb E1 transitions in F17. II. The region of the giant resonances 1975 Online-Ressource 7 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The giant dipole resonance of F17 was studied by radiative proton capture. An observed integrated strength of 10 MeV mb, presumably mostly T=12, is centered at 22 MeV with a width of ~ 5 MeV. Calculations were performed for odd-parity 2p-1h, 1p excitations in a basis of good isospin. These calculations predict correctly the observed strength distribution. Some general rules for the T components of the E1 collective state are consistent with the microscopic calculation. The f72→d52 strength was located near 18 MeV, in agreement with other experimental evidence.NUCLEAR REACTIONS F17, O16(p, γ), Ep=15.75-31.66 MeV. Measured dσdΩ(90°). Measured angular distributions deduced ET=12 of GDR. Calculated 1p and 2p-1h states of F17. Compared with experimental results. APS Digital Backfile Archive 1893-2003 Harakeh, M. N. oth Paul, P. oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 11(1975), 3, Seite 1008-1014 Online-Ressource (DE-627)NLEJ24823787X (DE-600)1461161-2 1089-490X nnns volume:11 year:1975 number:3 pages:1008-1014 extent:7 https://www.tib.eu/de/suchen/id/aps%3A9c05f74a758a7bb95bd8f4951f001f7281c7d100 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 11 1975 3 1008-1014 7 |
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(DE-627)NLEJ24990215X (DE-601)aps:9c05f74a758a7bb95bd8f4951f001f7281c7d100 DE-627 ger DE-627 rakwb E1 transitions in F17. II. The region of the giant resonances 1975 Online-Ressource 7 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The giant dipole resonance of F17 was studied by radiative proton capture. An observed integrated strength of 10 MeV mb, presumably mostly T=12, is centered at 22 MeV with a width of ~ 5 MeV. Calculations were performed for odd-parity 2p-1h, 1p excitations in a basis of good isospin. These calculations predict correctly the observed strength distribution. Some general rules for the T components of the E1 collective state are consistent with the microscopic calculation. The f72→d52 strength was located near 18 MeV, in agreement with other experimental evidence.NUCLEAR REACTIONS F17, O16(p, γ), Ep=15.75-31.66 MeV. Measured dσdΩ(90°). Measured angular distributions deduced ET=12 of GDR. Calculated 1p and 2p-1h states of F17. Compared with experimental results. APS Digital Backfile Archive 1893-2003 Harakeh, M. N. oth Paul, P. oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 11(1975), 3, Seite 1008-1014 Online-Ressource (DE-627)NLEJ24823787X (DE-600)1461161-2 1089-490X nnns volume:11 year:1975 number:3 pages:1008-1014 extent:7 https://www.tib.eu/de/suchen/id/aps%3A9c05f74a758a7bb95bd8f4951f001f7281c7d100 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 11 1975 3 1008-1014 7 |
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(DE-627)NLEJ24990215X (DE-601)aps:9c05f74a758a7bb95bd8f4951f001f7281c7d100 DE-627 ger DE-627 rakwb E1 transitions in F17. II. The region of the giant resonances 1975 Online-Ressource 7 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The giant dipole resonance of F17 was studied by radiative proton capture. An observed integrated strength of 10 MeV mb, presumably mostly T=12, is centered at 22 MeV with a width of ~ 5 MeV. Calculations were performed for odd-parity 2p-1h, 1p excitations in a basis of good isospin. These calculations predict correctly the observed strength distribution. Some general rules for the T components of the E1 collective state are consistent with the microscopic calculation. The f72→d52 strength was located near 18 MeV, in agreement with other experimental evidence.NUCLEAR REACTIONS F17, O16(p, γ), Ep=15.75-31.66 MeV. Measured dσdΩ(90°). Measured angular distributions deduced ET=12 of GDR. Calculated 1p and 2p-1h states of F17. Compared with experimental results. APS Digital Backfile Archive 1893-2003 Harakeh, M. N. oth Paul, P. oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 11(1975), 3, Seite 1008-1014 Online-Ressource (DE-627)NLEJ24823787X (DE-600)1461161-2 1089-490X nnns volume:11 year:1975 number:3 pages:1008-1014 extent:7 https://www.tib.eu/de/suchen/id/aps%3A9c05f74a758a7bb95bd8f4951f001f7281c7d100 Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 11 1975 3 1008-1014 7 |
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E1 transitions in F17. II. The region of the giant resonances |
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E1 transitions in F17. II. The region of the giant resonances |
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e1 transitions in f17. ii. the region of the giant resonances |
title_auth |
E1 transitions in F17. II. The region of the giant resonances |
abstract |
The giant dipole resonance of F17 was studied by radiative proton capture. An observed integrated strength of 10 MeV mb, presumably mostly T=12, is centered at 22 MeV with a width of ~ 5 MeV. Calculations were performed for odd-parity 2p-1h, 1p excitations in a basis of good isospin. These calculations predict correctly the observed strength distribution. Some general rules for the T components of the E1 collective state are consistent with the microscopic calculation. The f72→d52 strength was located near 18 MeV, in agreement with other experimental evidence.NUCLEAR REACTIONS F17, O16(p, γ), Ep=15.75-31.66 MeV. Measured dσdΩ(90°). Measured angular distributions deduced ET=12 of GDR. Calculated 1p and 2p-1h states of F17. Compared with experimental results. |
abstractGer |
The giant dipole resonance of F17 was studied by radiative proton capture. An observed integrated strength of 10 MeV mb, presumably mostly T=12, is centered at 22 MeV with a width of ~ 5 MeV. Calculations were performed for odd-parity 2p-1h, 1p excitations in a basis of good isospin. These calculations predict correctly the observed strength distribution. Some general rules for the T components of the E1 collective state are consistent with the microscopic calculation. The f72→d52 strength was located near 18 MeV, in agreement with other experimental evidence.NUCLEAR REACTIONS F17, O16(p, γ), Ep=15.75-31.66 MeV. Measured dσdΩ(90°). Measured angular distributions deduced ET=12 of GDR. Calculated 1p and 2p-1h states of F17. Compared with experimental results. |
abstract_unstemmed |
The giant dipole resonance of F17 was studied by radiative proton capture. An observed integrated strength of 10 MeV mb, presumably mostly T=12, is centered at 22 MeV with a width of ~ 5 MeV. Calculations were performed for odd-parity 2p-1h, 1p excitations in a basis of good isospin. These calculations predict correctly the observed strength distribution. Some general rules for the T components of the E1 collective state are consistent with the microscopic calculation. The f72→d52 strength was located near 18 MeV, in agreement with other experimental evidence.NUCLEAR REACTIONS F17, O16(p, γ), Ep=15.75-31.66 MeV. Measured dσdΩ(90°). Measured angular distributions deduced ET=12 of GDR. Calculated 1p and 2p-1h states of F17. Compared with experimental results. |
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E1 transitions in F17. II. The region of the giant resonances |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000naa a22002652 4500</leader><controlfield tag="001">NLEJ24990215X</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20231114103118.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">231114s1975 xx |||||o 00| ||und c</controlfield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)NLEJ24990215X</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-601)aps:9c05f74a758a7bb95bd8f4951f001f7281c7d100</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="245" ind1="1" ind2="0"><subfield code="a">E1 transitions in F17. II. The region of the giant resonances</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1975</subfield></datafield><datafield tag="300" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield></datafield><datafield tag="300" ind1=" " ind2=" "><subfield code="a">7</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">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">The giant dipole resonance of F17 was studied by radiative proton capture. An observed integrated strength of 10 MeV mb, presumably mostly T=12, is centered at 22 MeV with a width of ~ 5 MeV. Calculations were performed for odd-parity 2p-1h, 1p excitations in a basis of good isospin. These calculations predict correctly the observed strength distribution. Some general rules for the T components of the E1 collective state are consistent with the microscopic calculation. The f72→d52 strength was located near 18 MeV, in agreement with other experimental evidence.NUCLEAR REACTIONS F17, O16(p, γ), Ep=15.75-31.66 MeV. Measured dσdΩ(90°). Measured angular distributions deduced ET=12 of GDR. Calculated 1p and 2p-1h states of F17. Compared with experimental results.</subfield></datafield><datafield tag="533" ind1=" " ind2=" "><subfield code="f">APS Digital Backfile Archive 1893-2003</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Harakeh, M. N.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Paul, P.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Physical review / C</subfield><subfield code="d">Woodbury, NY : Inst., 1970</subfield><subfield code="g">11(1975), 3, Seite 1008-1014</subfield><subfield code="h">Online-Ressource</subfield><subfield code="w">(DE-627)NLEJ24823787X</subfield><subfield code="w">(DE-600)1461161-2</subfield><subfield code="x">1089-490X</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:11</subfield><subfield code="g">year:1975</subfield><subfield code="g">number:3</subfield><subfield code="g">pages:1008-1014</subfield><subfield code="g">extent:7</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://www.tib.eu/de/suchen/id/aps%3A9c05f74a758a7bb95bd8f4951f001f7281c7d100</subfield><subfield code="x">Verlag</subfield><subfield code="z">Deutschlandweit zugänglich</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_U</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">ZDB-1-APS</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">11</subfield><subfield code="j">1975</subfield><subfield code="e">3</subfield><subfield code="h">1008-1014</subfield><subfield code="g">7</subfield></datafield></record></collection>
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