Linear momentum transfer in the reaction of 64–269 MeV He3 with U238
Angular correlations between binary fission fragments have been measured in coincidence with light charged particles for 64, 129, 199, and 269 MeV induced3 reactions on a U238 target. Linear momentum transfer and missing linear momentum have been determined for a broad range of light-charged-particl...
Ausführliche Beschreibung
Gespeichert in:
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| Format: |
E-Artikel |
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| Erschienen: |
1989 |
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| Umfang: |
Online-Ressource 12 |
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| Reproduktion: |
APS Digital Backfile Archive 1893-2003 |
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| Übergeordnetes Werk: |
Enthalten in: Physical review / C - Woodbury, NY : Inst., 1970, 40(1989), 3, Seite 1279-1290 |
| Übergeordnetes Werk: |
volume:40 ; year:1989 ; number:3 ; pages:1279-1290 ; extent:12 |
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| 520 | |a Angular correlations between binary fission fragments have been measured in coincidence with light charged particles for 64, 129, 199, and 269 MeV induced3 reactions on a U238 target. Linear momentum transfer and missing linear momentum have been determined for a broad range of light-charged-particle energies ELCP and emission angles θLCP. Average momentum transfer increases from a fraction of beam momentum for small detection angles to nearly full momentum transfer at backward angles. The missing momentum depends primarily on ‘‘available energy’’ Eav=Ebeam-ELCP, but neither on beam energy Ebeam nor light particle detection angle. Backward proton and deuteron emission is incompatible with statistical evaporation following complete or incomplete fusion. | ||
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(DE-627)NLEJ249799715 (DE-601)aps:96a42313afb94c0b7ddc4bb103530aa1d94394ee DE-627 ger DE-627 rakwb Linear momentum transfer in the reaction of 64–269 MeV He3 with U238 1989 Online-Ressource 12 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Angular correlations between binary fission fragments have been measured in coincidence with light charged particles for 64, 129, 199, and 269 MeV induced3 reactions on a U238 target. Linear momentum transfer and missing linear momentum have been determined for a broad range of light-charged-particle energies ELCP and emission angles θLCP. Average momentum transfer increases from a fraction of beam momentum for small detection angles to nearly full momentum transfer at backward angles. The missing momentum depends primarily on ‘‘available energy’’ Eav=Ebeam-ELCP, but neither on beam energy Ebeam nor light particle detection angle. Backward proton and deuteron emission is incompatible with statistical evaporation following complete or incomplete fusion. APS Digital Backfile Archive 1893-2003 Skulski, W. oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 40(1989), 3, Seite 1279-1290 Online-Ressource (DE-627)NLEJ24823787X (DE-600)1461161-2 1089-490X nnns volume:40 year:1989 number:3 pages:1279-1290 extent:12 https://www.tib.eu/de/suchen/id/aps%3A96a42313afb94c0b7ddc4bb103530aa1d94394ee Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 40 1989 3 1279-1290 12 |
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(DE-627)NLEJ249799715 (DE-601)aps:96a42313afb94c0b7ddc4bb103530aa1d94394ee DE-627 ger DE-627 rakwb Linear momentum transfer in the reaction of 64–269 MeV He3 with U238 1989 Online-Ressource 12 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Angular correlations between binary fission fragments have been measured in coincidence with light charged particles for 64, 129, 199, and 269 MeV induced3 reactions on a U238 target. Linear momentum transfer and missing linear momentum have been determined for a broad range of light-charged-particle energies ELCP and emission angles θLCP. Average momentum transfer increases from a fraction of beam momentum for small detection angles to nearly full momentum transfer at backward angles. The missing momentum depends primarily on ‘‘available energy’’ Eav=Ebeam-ELCP, but neither on beam energy Ebeam nor light particle detection angle. Backward proton and deuteron emission is incompatible with statistical evaporation following complete or incomplete fusion. APS Digital Backfile Archive 1893-2003 Skulski, W. oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 40(1989), 3, Seite 1279-1290 Online-Ressource (DE-627)NLEJ24823787X (DE-600)1461161-2 1089-490X nnns volume:40 year:1989 number:3 pages:1279-1290 extent:12 https://www.tib.eu/de/suchen/id/aps%3A96a42313afb94c0b7ddc4bb103530aa1d94394ee Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 40 1989 3 1279-1290 12 |
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(DE-627)NLEJ249799715 (DE-601)aps:96a42313afb94c0b7ddc4bb103530aa1d94394ee DE-627 ger DE-627 rakwb Linear momentum transfer in the reaction of 64–269 MeV He3 with U238 1989 Online-Ressource 12 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Angular correlations between binary fission fragments have been measured in coincidence with light charged particles for 64, 129, 199, and 269 MeV induced3 reactions on a U238 target. Linear momentum transfer and missing linear momentum have been determined for a broad range of light-charged-particle energies ELCP and emission angles θLCP. Average momentum transfer increases from a fraction of beam momentum for small detection angles to nearly full momentum transfer at backward angles. The missing momentum depends primarily on ‘‘available energy’’ Eav=Ebeam-ELCP, but neither on beam energy Ebeam nor light particle detection angle. Backward proton and deuteron emission is incompatible with statistical evaporation following complete or incomplete fusion. APS Digital Backfile Archive 1893-2003 Skulski, W. oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 40(1989), 3, Seite 1279-1290 Online-Ressource (DE-627)NLEJ24823787X (DE-600)1461161-2 1089-490X nnns volume:40 year:1989 number:3 pages:1279-1290 extent:12 https://www.tib.eu/de/suchen/id/aps%3A96a42313afb94c0b7ddc4bb103530aa1d94394ee Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 40 1989 3 1279-1290 12 |
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(DE-627)NLEJ249799715 (DE-601)aps:96a42313afb94c0b7ddc4bb103530aa1d94394ee DE-627 ger DE-627 rakwb Linear momentum transfer in the reaction of 64–269 MeV He3 with U238 1989 Online-Ressource 12 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Angular correlations between binary fission fragments have been measured in coincidence with light charged particles for 64, 129, 199, and 269 MeV induced3 reactions on a U238 target. Linear momentum transfer and missing linear momentum have been determined for a broad range of light-charged-particle energies ELCP and emission angles θLCP. Average momentum transfer increases from a fraction of beam momentum for small detection angles to nearly full momentum transfer at backward angles. The missing momentum depends primarily on ‘‘available energy’’ Eav=Ebeam-ELCP, but neither on beam energy Ebeam nor light particle detection angle. Backward proton and deuteron emission is incompatible with statistical evaporation following complete or incomplete fusion. APS Digital Backfile Archive 1893-2003 Skulski, W. oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 40(1989), 3, Seite 1279-1290 Online-Ressource (DE-627)NLEJ24823787X (DE-600)1461161-2 1089-490X nnns volume:40 year:1989 number:3 pages:1279-1290 extent:12 https://www.tib.eu/de/suchen/id/aps%3A96a42313afb94c0b7ddc4bb103530aa1d94394ee Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 40 1989 3 1279-1290 12 |
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(DE-627)NLEJ249799715 (DE-601)aps:96a42313afb94c0b7ddc4bb103530aa1d94394ee DE-627 ger DE-627 rakwb Linear momentum transfer in the reaction of 64–269 MeV He3 with U238 1989 Online-Ressource 12 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Angular correlations between binary fission fragments have been measured in coincidence with light charged particles for 64, 129, 199, and 269 MeV induced3 reactions on a U238 target. Linear momentum transfer and missing linear momentum have been determined for a broad range of light-charged-particle energies ELCP and emission angles θLCP. Average momentum transfer increases from a fraction of beam momentum for small detection angles to nearly full momentum transfer at backward angles. The missing momentum depends primarily on ‘‘available energy’’ Eav=Ebeam-ELCP, but neither on beam energy Ebeam nor light particle detection angle. Backward proton and deuteron emission is incompatible with statistical evaporation following complete or incomplete fusion. APS Digital Backfile Archive 1893-2003 Skulski, W. oth Enthalten in Physical review / C Woodbury, NY : Inst., 1970 40(1989), 3, Seite 1279-1290 Online-Ressource (DE-627)NLEJ24823787X (DE-600)1461161-2 1089-490X nnns volume:40 year:1989 number:3 pages:1279-1290 extent:12 https://www.tib.eu/de/suchen/id/aps%3A96a42313afb94c0b7ddc4bb103530aa1d94394ee Verlag Deutschlandweit zugänglich GBV_USEFLAG_U ZDB-1-APS GBV_NL_ARTICLE AR 40 1989 3 1279-1290 12 |
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Linear momentum transfer in the reaction of 64–269 MeV He3 with U238 |
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Angular correlations between binary fission fragments have been measured in coincidence with light charged particles for 64, 129, 199, and 269 MeV induced3 reactions on a U238 target. Linear momentum transfer and missing linear momentum have been determined for a broad range of light-charged-particle energies ELCP and emission angles θLCP. Average momentum transfer increases from a fraction of beam momentum for small detection angles to nearly full momentum transfer at backward angles. The missing momentum depends primarily on ‘‘available energy’’ Eav=Ebeam-ELCP, but neither on beam energy Ebeam nor light particle detection angle. Backward proton and deuteron emission is incompatible with statistical evaporation following complete or incomplete fusion. |
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Angular correlations between binary fission fragments have been measured in coincidence with light charged particles for 64, 129, 199, and 269 MeV induced3 reactions on a U238 target. Linear momentum transfer and missing linear momentum have been determined for a broad range of light-charged-particle energies ELCP and emission angles θLCP. Average momentum transfer increases from a fraction of beam momentum for small detection angles to nearly full momentum transfer at backward angles. The missing momentum depends primarily on ‘‘available energy’’ Eav=Ebeam-ELCP, but neither on beam energy Ebeam nor light particle detection angle. Backward proton and deuteron emission is incompatible with statistical evaporation following complete or incomplete fusion. |
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Angular correlations between binary fission fragments have been measured in coincidence with light charged particles for 64, 129, 199, and 269 MeV induced3 reactions on a U238 target. Linear momentum transfer and missing linear momentum have been determined for a broad range of light-charged-particle energies ELCP and emission angles θLCP. Average momentum transfer increases from a fraction of beam momentum for small detection angles to nearly full momentum transfer at backward angles. The missing momentum depends primarily on ‘‘available energy’’ Eav=Ebeam-ELCP, but neither on beam energy Ebeam nor light particle detection angle. Backward proton and deuteron emission is incompatible with statistical evaporation following complete or incomplete fusion. |
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