2019
DOI: 10.1007/s10967-019-06497-7
|View full text |Cite
|
Sign up to set email alerts
|

Hot fusion of fission fragments for the synthesis of doubly magic nucleus $${}_{126}^{310} X^{184}$$ 126 310 X 184

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2

Citation Types

0
2
0

Year Published

2020
2020
2024
2024

Publication Types

Select...
7

Relationship

1
6

Authors

Journals

citations
Cited by 11 publications
(2 citation statements)
references
References 22 publications
0
2
0
Order By: Relevance
“…The shell correction δU for a given nucleus is taken from [9]. The bulk α and asymmetry a a constants are obtained by equating the ground state mass excess of AME2016 [10] or of FRDM(2012) [3] by with V A Z U LDM , ( )+δ [11].…”
Section: Methodsmentioning
confidence: 99%
“…The shell correction δU for a given nucleus is taken from [9]. The bulk α and asymmetry a a constants are obtained by equating the ground state mass excess of AME2016 [10] or of FRDM(2012) [3] by with V A Z U LDM , ( )+δ [11].…”
Section: Methodsmentioning
confidence: 99%
“…where n = 0, 1, 2, 3.., referring to ground state (n = 0) and excited states (n = 1, 2, 3...) solutions, i =1 and 2 refers to the heavy and light binary fragment, respectively. The term V LDM is liquid drop energy [10] with its bulk and asymmetry constants adjusted by [11] and references therein, dU is the shell correction [12], V P is the nuclear proximity potential [13], V C (T) = e 2 Z 1 Z 2 /R(T) is the Coulomb potential and the centrifugal potentials is V = + ( )…”
Section: Methodsmentioning
confidence: 99%