ÚTEFČVUT Ústav technické a experimentální fyziky ČVUT v PrazeInstitute of Experimental and Applied Physics, CTU in Prague

Cross Sections of the Production of Mercury and Radon Isotopes in Complete Fusion Reactions with 36,40Ar and 40,48Ca Projectiles

NázevTitle
Cross Sections of the Production of Mercury and Radon Isotopes in Complete Fusion Reactions with 36,40Ar and 40,48Ca ProjectilesCross Sections of the Production of Mercury and Radon Isotopes in Complete Fusion Reactions with 36,40Ar and 40,48Ca Projectiles
Druh výsledkuResult type
Článek v časopiseJournal article
AutořiAuthors
E.V. Chernysheva, A.M. Rodin, V.Y. Vedeneev, A.V. Gulyaev, M. Holík, Ľ. Krupa
Klíčová slovaKeywords
cross section, fusion reaction, heavy ion
DOIDOI
10.3103/S1062873822080044
Časopis / citaceJournal / citation
Bulletin of the Russian Academy of Sciences: Physics 86(8), 883-888 (2022) · ISSN 1934-9432
RokYear
2022
JazykLanguage
eng
ZáznamyRecords
ProjektProject
Institucionální podpora na rozvoj výzkumné org.Institucionální podpora na rozvoj výzkumné org.
CitovánoCited by
1 (INSPIRE-HEP)
2024: 1
Citace ke staženíDownload citation
TXT · BibTeX

AbstraktAbstract

A modified catcher foil technique is used to measure the absolute cross sections of xn-evaporation channels in complete fusion reactions 144Sm(40Ar, xn)184−xHg, 148Sm(36Ar, xn)184−xHg, 144Nd(40Ca, xn)184−xHg, 142Nd(48Ca, xn)190−xHg, and 166Er(40Ar, xn)206−xRn. The effect the spread of the beam’s energy has on the excitation functions as it moves through absorbing foils and the target is addressed by means of deconvolution. The measured excitation functions are compared to ones calculated theoretically using the coupled-channel model.

A modified catcher foil technique is used to measure the absolute cross sections of xn-evaporation channels in complete fusion reactions 144Sm(40Ar, xn)184−xHg, 148Sm(36Ar, xn)184−xHg, 144Nd(40Ca, xn)184−xHg, 142Nd(48Ca, xn)190−xHg, and 166Er(40Ar, xn)206−xRn. The effect the spread of the beam’s energy has on the excitation functions as it moves through absorbing foils and the target is addressed by means of deconvolution. The measured excitation functions are compared to ones calculated theoretically using the coupled-channel model.

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