The giant dipole resonance and isospin in^8^9Y(p, γ)^9^0Zr
The 90^o cross section for the reaction ^8^9Y(p,γ"o)^9^0Zr has been measured for proton energies between 2.6 and 19.0 MeV using Van de Graaff protons and a Nal counter. Some angular distributions were also measured. There is no evidence of a well-defined component of the dipole resonance with T...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1969 |
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| Reproduktion: |
Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 |
|---|---|
| Übergeordnetes Werk: |
in: Nuclear Physics, Section A - Amsterdam : Elsevier, 135(1969), 1, Seite 193-206 |
| Übergeordnetes Werk: |
volume:135 ; year:1969 ; number:1 ; pages:193-206 |
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| 520 | |a The 90^o cross section for the reaction ^8^9Y(p,γ"o)^9^0Zr has been measured for proton energies between 2.6 and 19.0 MeV using Van de Graaff protons and a Nal counter. Some angular distributions were also measured. There is no evidence of a well-defined component of the dipole resonance with T = T"3 + 1 = 6.At low energies, the excitation function is in agreement with a statistical calculation of the Hausser-Feshbach type. At higher energies, there is a ''direct'' component showing strong electric quadrupole interference. | ||
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(DE-627)NLEJ181202700 (DE-599)GBVNLZ181202700 DE-627 ger DE-627 rakwb eng The giant dipole resonance and isospin in^8^9Y(p, γ)^9^0Zr 1969 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The 90^o cross section for the reaction ^8^9Y(p,γ"o)^9^0Zr has been measured for proton energies between 2.6 and 19.0 MeV using Van de Graaff protons and a Nal counter. Some angular distributions were also measured. There is no evidence of a well-defined component of the dipole resonance with T = T"3 + 1 = 6.At low energies, the excitation function is in agreement with a statistical calculation of the Hausser-Feshbach type. At higher energies, there is a ''direct'' component showing strong electric quadrupole interference. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Mason, W.M. oth Kernel, G. oth Black, J.L. oth Tanner, N.W. oth in Nuclear Physics, Section A Amsterdam : Elsevier 135(1969), 1, Seite 193-206 (DE-627)NLEJ177217928 (DE-600)1466542-6 0375-9474 nnns volume:135 year:1969 number:1 pages:193-206 http://linkinghub.elsevier.com/retrieve/pii/0375-9474(69)90158-4 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 135 1969 1 193-206 |
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(DE-627)NLEJ181202700 (DE-599)GBVNLZ181202700 DE-627 ger DE-627 rakwb eng The giant dipole resonance and isospin in^8^9Y(p, γ)^9^0Zr 1969 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The 90^o cross section for the reaction ^8^9Y(p,γ"o)^9^0Zr has been measured for proton energies between 2.6 and 19.0 MeV using Van de Graaff protons and a Nal counter. Some angular distributions were also measured. There is no evidence of a well-defined component of the dipole resonance with T = T"3 + 1 = 6.At low energies, the excitation function is in agreement with a statistical calculation of the Hausser-Feshbach type. At higher energies, there is a ''direct'' component showing strong electric quadrupole interference. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Mason, W.M. oth Kernel, G. oth Black, J.L. oth Tanner, N.W. oth in Nuclear Physics, Section A Amsterdam : Elsevier 135(1969), 1, Seite 193-206 (DE-627)NLEJ177217928 (DE-600)1466542-6 0375-9474 nnns volume:135 year:1969 number:1 pages:193-206 http://linkinghub.elsevier.com/retrieve/pii/0375-9474(69)90158-4 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 135 1969 1 193-206 |
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(DE-627)NLEJ181202700 (DE-599)GBVNLZ181202700 DE-627 ger DE-627 rakwb eng The giant dipole resonance and isospin in^8^9Y(p, γ)^9^0Zr 1969 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The 90^o cross section for the reaction ^8^9Y(p,γ"o)^9^0Zr has been measured for proton energies between 2.6 and 19.0 MeV using Van de Graaff protons and a Nal counter. Some angular distributions were also measured. There is no evidence of a well-defined component of the dipole resonance with T = T"3 + 1 = 6.At low energies, the excitation function is in agreement with a statistical calculation of the Hausser-Feshbach type. At higher energies, there is a ''direct'' component showing strong electric quadrupole interference. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Mason, W.M. oth Kernel, G. oth Black, J.L. oth Tanner, N.W. oth in Nuclear Physics, Section A Amsterdam : Elsevier 135(1969), 1, Seite 193-206 (DE-627)NLEJ177217928 (DE-600)1466542-6 0375-9474 nnns volume:135 year:1969 number:1 pages:193-206 http://linkinghub.elsevier.com/retrieve/pii/0375-9474(69)90158-4 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 135 1969 1 193-206 |
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(DE-627)NLEJ181202700 (DE-599)GBVNLZ181202700 DE-627 ger DE-627 rakwb eng The giant dipole resonance and isospin in^8^9Y(p, γ)^9^0Zr 1969 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The 90^o cross section for the reaction ^8^9Y(p,γ"o)^9^0Zr has been measured for proton energies between 2.6 and 19.0 MeV using Van de Graaff protons and a Nal counter. Some angular distributions were also measured. There is no evidence of a well-defined component of the dipole resonance with T = T"3 + 1 = 6.At low energies, the excitation function is in agreement with a statistical calculation of the Hausser-Feshbach type. At higher energies, there is a ''direct'' component showing strong electric quadrupole interference. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Mason, W.M. oth Kernel, G. oth Black, J.L. oth Tanner, N.W. oth in Nuclear Physics, Section A Amsterdam : Elsevier 135(1969), 1, Seite 193-206 (DE-627)NLEJ177217928 (DE-600)1466542-6 0375-9474 nnns volume:135 year:1969 number:1 pages:193-206 http://linkinghub.elsevier.com/retrieve/pii/0375-9474(69)90158-4 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 135 1969 1 193-206 |
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(DE-627)NLEJ181202700 (DE-599)GBVNLZ181202700 DE-627 ger DE-627 rakwb eng The giant dipole resonance and isospin in^8^9Y(p, γ)^9^0Zr 1969 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier The 90^o cross section for the reaction ^8^9Y(p,γ"o)^9^0Zr has been measured for proton energies between 2.6 and 19.0 MeV using Van de Graaff protons and a Nal counter. Some angular distributions were also measured. There is no evidence of a well-defined component of the dipole resonance with T = T"3 + 1 = 6.At low energies, the excitation function is in agreement with a statistical calculation of the Hausser-Feshbach type. At higher energies, there is a ''direct'' component showing strong electric quadrupole interference. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Mason, W.M. oth Kernel, G. oth Black, J.L. oth Tanner, N.W. oth in Nuclear Physics, Section A Amsterdam : Elsevier 135(1969), 1, Seite 193-206 (DE-627)NLEJ177217928 (DE-600)1466542-6 0375-9474 nnns volume:135 year:1969 number:1 pages:193-206 http://linkinghub.elsevier.com/retrieve/pii/0375-9474(69)90158-4 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 135 1969 1 193-206 |
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The giant dipole resonance and isospin in^8^9Y(p, γ)^9^0Zr |
| abstract |
The 90^o cross section for the reaction ^8^9Y(p,γ"o)^9^0Zr has been measured for proton energies between 2.6 and 19.0 MeV using Van de Graaff protons and a Nal counter. Some angular distributions were also measured. There is no evidence of a well-defined component of the dipole resonance with T = T"3 + 1 = 6.At low energies, the excitation function is in agreement with a statistical calculation of the Hausser-Feshbach type. At higher energies, there is a ''direct'' component showing strong electric quadrupole interference. |
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The 90^o cross section for the reaction ^8^9Y(p,γ"o)^9^0Zr has been measured for proton energies between 2.6 and 19.0 MeV using Van de Graaff protons and a Nal counter. Some angular distributions were also measured. There is no evidence of a well-defined component of the dipole resonance with T = T"3 + 1 = 6.At low energies, the excitation function is in agreement with a statistical calculation of the Hausser-Feshbach type. At higher energies, there is a ''direct'' component showing strong electric quadrupole interference. |
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The 90^o cross section for the reaction ^8^9Y(p,γ"o)^9^0Zr has been measured for proton energies between 2.6 and 19.0 MeV using Van de Graaff protons and a Nal counter. Some angular distributions were also measured. There is no evidence of a well-defined component of the dipole resonance with T = T"3 + 1 = 6.At low energies, the excitation function is in agreement with a statistical calculation of the Hausser-Feshbach type. At higher energies, there is a ''direct'' component showing strong electric quadrupole interference. |
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