Energy dependence of Bi209 fragmentation in relativistic nuclear collisions
The results of cross-section measurements for the reactions Bi209(C12,X)Au, E=4.8 and 25.2 GeV and Bi209(Ne20,X)Au, E=8.0 GeV are reported. The observed yields of the gold isotopes show a similar dependence on mass number for each reaction, differing slightly in the position of the centroid of the d...
Ausführliche Beschreibung
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1981 |
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Online-Ressource 3 |
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APS Digital Backfile Archive 1893-2003 |
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Übergeordnetes Werk: |
Enthalten in: Physical review / C - Woodbury, NY : Inst., 1970, 23(1981), 3, Seite 1044-1046 |
Übergeordnetes Werk: |
volume:23 ; year:1981 ; number:3 ; pages:1044-1046 ; extent:3 |
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520 | |a The results of cross-section measurements for the reactions Bi209(C12,X)Au, E=4.8 and 25.2 GeV and Bi209(Ne20,X)Au, E=8.0 GeV are reported. The observed yields of the gold isotopes show a similar dependence on mass number for each reaction, differing slightly in the position of the centroid of the distribution. As the projectile energy increases, the inferred excitation energy of the primary residues remains the same or decreases slightly. This observation is in agreement with the predictions of the intranuclear cascade model of relativistic heavy ion collisions.NUCLEAR REACTIONS Bi209(C12,X)Au, E=4.8, 25.2 GeV; Bi209(Ne20,X)Au, E=8.0 GeV; measured Au isotopic distributions, relativistic heavy ions, target fragmentation, Ge(Li) spectroscopy. | ||
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(DE-627)NLEJ249863219 (DE-601)aps:2a6379b999a65fedcc6aafdabd01f16d2a9d95fa DE-627 ger DE-627 rakwb Energy dependence of Bi209 fragmentation in relativistic nuclear collisions 1981 Online-Ressource 3 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The results of cross-section measurements for the reactions Bi209(C12,X)Au, E=4.8 and 25.2 GeV and Bi209(Ne20,X)Au, E=8.0 GeV are reported. The observed yields of the gold isotopes show a similar dependence on mass number for each reaction, differing slightly in the position of the centroid of the distribution. As the projectile energy increases, the inferred excitation energy of the primary residues remains the same or decreases slightly. This observation is in agreement with the predictions of the intranuclear cascade model of relativistic heavy ion collisions.NUCLEAR REACTIONS Bi209(C12,X)Au, E=4.8, 25.2 GeV; Bi209(Ne20,X)Au, E=8.0 GeV; measured Au isotopic distributions, relativistic heavy ions, target fragmentation, Ge(Li) spectroscopy. APS Digital Backfile Archive 1893-2003 Aleklett, K. oth Morrissey, D. J. oth Loveland, W. oth McGaughey, P. L. oth Seaborg, G. T. oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 23(1981), 3, Seite 1044-1046 Online-Ressource (DE-627)NLEJ24823787X (DE-600)1461161-2 1089-490X nnns volume:23 year:1981 number:3 pages:1044-1046 extent:3 https://www.tib.eu/de/suchen/id/aps%3A2a6379b999a65fedcc6aafdabd01f16d2a9d95fa Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 23 1981 3 1044-1046 3 |
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(DE-627)NLEJ249863219 (DE-601)aps:2a6379b999a65fedcc6aafdabd01f16d2a9d95fa DE-627 ger DE-627 rakwb Energy dependence of Bi209 fragmentation in relativistic nuclear collisions 1981 Online-Ressource 3 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The results of cross-section measurements for the reactions Bi209(C12,X)Au, E=4.8 and 25.2 GeV and Bi209(Ne20,X)Au, E=8.0 GeV are reported. The observed yields of the gold isotopes show a similar dependence on mass number for each reaction, differing slightly in the position of the centroid of the distribution. As the projectile energy increases, the inferred excitation energy of the primary residues remains the same or decreases slightly. This observation is in agreement with the predictions of the intranuclear cascade model of relativistic heavy ion collisions.NUCLEAR REACTIONS Bi209(C12,X)Au, E=4.8, 25.2 GeV; Bi209(Ne20,X)Au, E=8.0 GeV; measured Au isotopic distributions, relativistic heavy ions, target fragmentation, Ge(Li) spectroscopy. APS Digital Backfile Archive 1893-2003 Aleklett, K. oth Morrissey, D. J. oth Loveland, W. oth McGaughey, P. L. oth Seaborg, G. T. oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 23(1981), 3, Seite 1044-1046 Online-Ressource (DE-627)NLEJ24823787X (DE-600)1461161-2 1089-490X nnns volume:23 year:1981 number:3 pages:1044-1046 extent:3 https://www.tib.eu/de/suchen/id/aps%3A2a6379b999a65fedcc6aafdabd01f16d2a9d95fa Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 23 1981 3 1044-1046 3 |
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(DE-627)NLEJ249863219 (DE-601)aps:2a6379b999a65fedcc6aafdabd01f16d2a9d95fa DE-627 ger DE-627 rakwb Energy dependence of Bi209 fragmentation in relativistic nuclear collisions 1981 Online-Ressource 3 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The results of cross-section measurements for the reactions Bi209(C12,X)Au, E=4.8 and 25.2 GeV and Bi209(Ne20,X)Au, E=8.0 GeV are reported. The observed yields of the gold isotopes show a similar dependence on mass number for each reaction, differing slightly in the position of the centroid of the distribution. As the projectile energy increases, the inferred excitation energy of the primary residues remains the same or decreases slightly. This observation is in agreement with the predictions of the intranuclear cascade model of relativistic heavy ion collisions.NUCLEAR REACTIONS Bi209(C12,X)Au, E=4.8, 25.2 GeV; Bi209(Ne20,X)Au, E=8.0 GeV; measured Au isotopic distributions, relativistic heavy ions, target fragmentation, Ge(Li) spectroscopy. APS Digital Backfile Archive 1893-2003 Aleklett, K. oth Morrissey, D. J. oth Loveland, W. oth McGaughey, P. L. oth Seaborg, G. T. oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 23(1981), 3, Seite 1044-1046 Online-Ressource (DE-627)NLEJ24823787X (DE-600)1461161-2 1089-490X nnns volume:23 year:1981 number:3 pages:1044-1046 extent:3 https://www.tib.eu/de/suchen/id/aps%3A2a6379b999a65fedcc6aafdabd01f16d2a9d95fa Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 23 1981 3 1044-1046 3 |
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(DE-627)NLEJ249863219 (DE-601)aps:2a6379b999a65fedcc6aafdabd01f16d2a9d95fa DE-627 ger DE-627 rakwb Energy dependence of Bi209 fragmentation in relativistic nuclear collisions 1981 Online-Ressource 3 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The results of cross-section measurements for the reactions Bi209(C12,X)Au, E=4.8 and 25.2 GeV and Bi209(Ne20,X)Au, E=8.0 GeV are reported. The observed yields of the gold isotopes show a similar dependence on mass number for each reaction, differing slightly in the position of the centroid of the distribution. As the projectile energy increases, the inferred excitation energy of the primary residues remains the same or decreases slightly. This observation is in agreement with the predictions of the intranuclear cascade model of relativistic heavy ion collisions.NUCLEAR REACTIONS Bi209(C12,X)Au, E=4.8, 25.2 GeV; Bi209(Ne20,X)Au, E=8.0 GeV; measured Au isotopic distributions, relativistic heavy ions, target fragmentation, Ge(Li) spectroscopy. APS Digital Backfile Archive 1893-2003 Aleklett, K. oth Morrissey, D. J. oth Loveland, W. oth McGaughey, P. L. oth Seaborg, G. T. oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 23(1981), 3, Seite 1044-1046 Online-Ressource (DE-627)NLEJ24823787X (DE-600)1461161-2 1089-490X nnns volume:23 year:1981 number:3 pages:1044-1046 extent:3 https://www.tib.eu/de/suchen/id/aps%3A2a6379b999a65fedcc6aafdabd01f16d2a9d95fa Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 23 1981 3 1044-1046 3 |
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(DE-627)NLEJ249863219 (DE-601)aps:2a6379b999a65fedcc6aafdabd01f16d2a9d95fa DE-627 ger DE-627 rakwb Energy dependence of Bi209 fragmentation in relativistic nuclear collisions 1981 Online-Ressource 3 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier The results of cross-section measurements for the reactions Bi209(C12,X)Au, E=4.8 and 25.2 GeV and Bi209(Ne20,X)Au, E=8.0 GeV are reported. The observed yields of the gold isotopes show a similar dependence on mass number for each reaction, differing slightly in the position of the centroid of the distribution. As the projectile energy increases, the inferred excitation energy of the primary residues remains the same or decreases slightly. This observation is in agreement with the predictions of the intranuclear cascade model of relativistic heavy ion collisions.NUCLEAR REACTIONS Bi209(C12,X)Au, E=4.8, 25.2 GeV; Bi209(Ne20,X)Au, E=8.0 GeV; measured Au isotopic distributions, relativistic heavy ions, target fragmentation, Ge(Li) spectroscopy. APS Digital Backfile Archive 1893-2003 Aleklett, K. oth Morrissey, D. J. oth Loveland, W. oth McGaughey, P. L. oth Seaborg, G. T. oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 23(1981), 3, Seite 1044-1046 Online-Ressource (DE-627)NLEJ24823787X (DE-600)1461161-2 1089-490X nnns volume:23 year:1981 number:3 pages:1044-1046 extent:3 https://www.tib.eu/de/suchen/id/aps%3A2a6379b999a65fedcc6aafdabd01f16d2a9d95fa Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 23 1981 3 1044-1046 3 |
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energy dependence of bi209 fragmentation in relativistic nuclear collisions |
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Energy dependence of Bi209 fragmentation in relativistic nuclear collisions |
abstract |
The results of cross-section measurements for the reactions Bi209(C12,X)Au, E=4.8 and 25.2 GeV and Bi209(Ne20,X)Au, E=8.0 GeV are reported. The observed yields of the gold isotopes show a similar dependence on mass number for each reaction, differing slightly in the position of the centroid of the distribution. As the projectile energy increases, the inferred excitation energy of the primary residues remains the same or decreases slightly. This observation is in agreement with the predictions of the intranuclear cascade model of relativistic heavy ion collisions.NUCLEAR REACTIONS Bi209(C12,X)Au, E=4.8, 25.2 GeV; Bi209(Ne20,X)Au, E=8.0 GeV; measured Au isotopic distributions, relativistic heavy ions, target fragmentation, Ge(Li) spectroscopy. |
abstractGer |
The results of cross-section measurements for the reactions Bi209(C12,X)Au, E=4.8 and 25.2 GeV and Bi209(Ne20,X)Au, E=8.0 GeV are reported. The observed yields of the gold isotopes show a similar dependence on mass number for each reaction, differing slightly in the position of the centroid of the distribution. As the projectile energy increases, the inferred excitation energy of the primary residues remains the same or decreases slightly. This observation is in agreement with the predictions of the intranuclear cascade model of relativistic heavy ion collisions.NUCLEAR REACTIONS Bi209(C12,X)Au, E=4.8, 25.2 GeV; Bi209(Ne20,X)Au, E=8.0 GeV; measured Au isotopic distributions, relativistic heavy ions, target fragmentation, Ge(Li) spectroscopy. |
abstract_unstemmed |
The results of cross-section measurements for the reactions Bi209(C12,X)Au, E=4.8 and 25.2 GeV and Bi209(Ne20,X)Au, E=8.0 GeV are reported. The observed yields of the gold isotopes show a similar dependence on mass number for each reaction, differing slightly in the position of the centroid of the distribution. As the projectile energy increases, the inferred excitation energy of the primary residues remains the same or decreases slightly. This observation is in agreement with the predictions of the intranuclear cascade model of relativistic heavy ion collisions.NUCLEAR REACTIONS Bi209(C12,X)Au, E=4.8, 25.2 GeV; Bi209(Ne20,X)Au, E=8.0 GeV; measured Au isotopic distributions, relativistic heavy ions, target fragmentation, Ge(Li) spectroscopy. |
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Energy dependence of Bi209 fragmentation in relativistic nuclear collisions |
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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">NLEJ249863219</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20231114103013.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">231114s1981 xx |||||o 00| ||und c</controlfield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)NLEJ249863219</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-601)aps:2a6379b999a65fedcc6aafdabd01f16d2a9d95fa</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">Energy dependence of Bi209 fragmentation in relativistic nuclear collisions</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1981</subfield></datafield><datafield tag="300" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield></datafield><datafield tag="300" ind1=" " ind2=" "><subfield code="a">3</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 results of cross-section measurements for the reactions Bi209(C12,X)Au, E=4.8 and 25.2 GeV and Bi209(Ne20,X)Au, E=8.0 GeV are reported. The observed yields of the gold isotopes show a similar dependence on mass number for each reaction, differing slightly in the position of the centroid of the distribution. As the projectile energy increases, the inferred excitation energy of the primary residues remains the same or decreases slightly. This observation is in agreement with the predictions of the intranuclear cascade model of relativistic heavy ion collisions.NUCLEAR REACTIONS Bi209(C12,X)Au, E=4.8, 25.2 GeV; Bi209(Ne20,X)Au, E=8.0 GeV; measured Au isotopic distributions, relativistic heavy ions, target fragmentation, Ge(Li) spectroscopy.</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">Aleklett, K.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Morrissey, D. J.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Loveland, W.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">McGaughey, P. L.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Seaborg, G. T.</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">23(1981), 3, Seite 1044-1046</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:23</subfield><subfield code="g">year:1981</subfield><subfield code="g">number:3</subfield><subfield code="g">pages:1044-1046</subfield><subfield code="g">extent:3</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://www.tib.eu/de/suchen/id/aps%3A2a6379b999a65fedcc6aafdabd01f16d2a9d95fa</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">23</subfield><subfield code="j">1981</subfield><subfield code="e">3</subfield><subfield code="h">1044-1046</subfield><subfield code="g">3</subfield></datafield></record></collection>
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