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2022DA17      Phys.Rev. C 106, 064603 (2022)

P.S.Damodara Gupta, N.Sowmya, H.C.Manjunatha, L.Seenappa, T.Ganesh

Quasifission barrier of heavy ion fusion reactions leading to the formation of the superheavy nucleus ³⁰²120

NUCLEAR REACTIONS ²⁵¹Cf(⁵⁶Ti, 3n)³⁰⁴120, E^*=36 MeV; ²⁵¹Cf(⁵⁷Ti, 4n)³⁰⁴120, E^*=47 MeV; ²⁵¹Cf(⁵⁸Ti, 5n)³⁰⁴120, E^*=60 MeV; ²⁴⁹Bk(⁵⁸V, 3n)³⁰⁴120, E^*=37 MeV; ²⁴⁹Bk(⁵⁹V, 4n)³⁰⁴120, E^*=47 MeV; ²⁴⁹Bk(⁶⁰V, 5n)³⁰⁴120, E^*=59 MeV; ²⁴⁸Cm(⁵⁹Cr, 3n)³⁰⁴120, E ^*=36 MeV; ²⁴⁸Cm(⁶⁰Cr, 4n)³⁰⁴120, E^*=46 MeV; ²⁴⁸Cm(⁶¹Cr, 5n)³⁰⁴120, E^*=57 MeV; ²⁴⁸Cf(⁴⁵Sc, 3n)²⁹⁰119, E^*=39 MeV; ²⁴⁷Bk(⁵⁰Ti, 3n)²⁹⁴119, E^*=36 MeV; ²⁴²Cm(⁵¹V, 3n)²⁹⁰119, E^*=38 MeV; ²⁴²Am(⁵⁴Cr, 3n)²⁹³119, E^*=37 MeV; calculated evaporation residue σ. ²³⁷Th(⁶⁵Zn, X), ²¹⁸Po(⁸⁴Kr, X), E not given; calculated nucleus-nucleus interaction potential from the fusion which leads to ³⁰²120 production. ²⁵²Cf(⁵⁰Ti, X), E(cm)=223 MeV; ²⁴⁹Bk(⁵³V, X), E(cm)=229 MeV; ²⁴⁸Cm(⁵⁴Cr, X), E(cm)=236 MeV; ²⁴⁴Pu(⁵⁸Fe, X), E(cm)=249 MeV; ²³⁹Pa(⁶³Cu, X), E(cm)=260 MeV; ²³²Th(⁷⁰Zn, X), E(cm)=281 MeV; ²²²Rn(⁸⁰Se, X), E(cm)=309 MeV; ²²⁸Ra(⁷⁴Ge, X), E(cm)=240 MeV; ²³⁸U(⁶⁴Ni, X), E(cm)=267 MeV; calculated quasifission barrier, evaporation residue σ, entrance channel parameters. Investigated the influence of the projectile-target orientation and angular momentum on quasifission barriers. Dinuclear system (DNS) model. Comparison to other theoretical estimations.

doi: 10.1103/PhysRevC.106.064603
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