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NSR database version of May 10, 2024.

Search: Author = A.Cyriac

Found 3 matches.

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2020SA16      Phys.Rev. C 101, 044613 (2020)

K.P.Santhosh, A.Cyriac

Quaternary fission in 244-254Cf isotopes with two α particles as middle fragments

RADIOACTIVITY 244,246,248,250,252,254Cf(SF); calculated driving potential as function of fragment mass number, fragment yields for different combinations of A1 and A2 and two α particles, Q-values in two α-accompanied quaternary fission using the interacting barrier as the sum of Coulomb and nuclear proximity potential, with fragments in collinear configuration, and accounting for deformation and orientation of fragments; deduced highest yields when one fragment is 130Sb for 244Cf, 132Sb for 248Cf, 134Sb for 254Cf, 134I for 246Cf, 132In for 250Cf, and 132Te for 252Cf.

doi: 10.1103/PhysRevC.101.044613
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2019SA47      C.R.Physique 20, 569 (2019)

K.P.Santhosh, A.Cyriac

Studies on the cold binary fragmentation of even-even 230-250U isotopes

NUCLEAR REACTIONS 230,232,234,236,238,240,242,244,246,248,250U(n, F), E cold; framework of the Coulomb and proximity potential model (CPPM).

doi: 10.1016/j.crhy.2018.11.009
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2016SA14      Nucl.Phys. A949, 8 (2016)

K.P.Santhosh, A.Cyriac, S.Krishnan

Isotopic yield in cold binary fission of even-even 244-258Cf isotopes

RADIOACTIVITY 244,246,248,250,252,254,256,258Cf(SF); calculated isotopic yields; deduced change of yield pattern with increasing mass of the mother nucleus. Calculations for 252Cf compared with data taken from γγγ-coin using Gammasphere.

doi: 10.1016/j.nuclphysa.2016.02.036
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