Dumbbell shapes in the superasymmetric fission of heavy nuclei

We have calculated the fission fragments' mass distributions for several isotopes of heavy and superheavy nuclei from uranium to flerovium within an improved scission point model. For all considered nuclei, in addition to the standard mass-asymmetric fission mode we have found the mass super-asymmetric mode with the mass of heavy fragments equal 190. For the actinide nuclei, the probability of superasymmetric fission is by six orders of magnitude smaller than for standard asymmetric fission. For the superheavy nuclei this probability is only by two orders of magnitude smaller. In all cases, the superasymmetric scission shapes are dumbbells with the heavy fragment close to a sphere. We have estimated the stability of the light fragment concerning the variation of the neck and found out that sequential ternary fission is not favored energetically. The calculations were carried out with nuclear shape described by generalized Cassinian ovals with six deformation parameters, <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mi>α</a:mi></a:math>, <b:math xmlns:b="http://www.w3.org/1998/Math/MathML"><b:msub><b:mi>α</b:mi><b:mn>1</b:mn></b:msub></b:math>, <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"><c:msub><c:mi>α</c:mi><c:mn>2</c:mn></c:msub></c:math>, <d:math xmlns:d="http://www.w3.org/1998/Math/MathML"><d:msub><d:mi>α</d:mi><d:mn>3</d:mn></d:msub></d:math>, <e:math xmlns:e="http://www.w3.org/1998/Math/MathML"><e:msub><e:mi>α</e:mi><e:mn>4</e:mn></e:msub></e:math>, and <f:math xmlns:f="http://www.w3.org/1998/Math/MathML"><f:msub><f:mi>α</f:mi><f:mn>5</f:mn></f:msub></f:math>. The configuration at the moment of the neck rupture was defined by fixing <g:math xmlns:g="http://www.w3.org/1998/Math/MathML"><g:mrow><g:mi>α</g:mi><g:mo>=</g:mo><g:mn>0.98</g:mn></g:mrow></g:math>. This value corresponds to a neck radius <h:math xmlns:h="http://www.w3.org/1998/Math/MathML"><h:mrow><h:msub><h:mi>r</h:mi><h:mi>neck</h:mi></h:msub><h:mo>≈</h:mo><h:mn>1.5</h:mn></h:mrow></h:math> fm. Published by the American Physical Society 2024

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Journal
Physical review. C
Published
2024-12-24
DOI
https://doi.org/10.1103/physrevc.110.064616
Citations
2
Primary Topic
Nuclear physics research studies
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article
Field-Weighted Citation Impact
1.32
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article

Dumbbell shapes in the superasymmetric fission of heavy nuclei

N. Carjan, F. A. Ivanyuk
2 citations
Physical review. C
Nuclear physics research studies
1.32
article

Dumbbell shapes in the superasymmetric fission of heavy nuclei

N. Carjan, F. A. Ivanyuk
article en
2 citations

Abstract

We have calculated the fission fragments' mass distributions for several isotopes of heavy and superheavy nuclei from uranium to flerovium within an improved scission point model. For all considered nuclei, in addition to the standard mass-asymmetric fission mode we have found the mass super-asymmetric mode with the mass of heavy fragments equal 190. For the actinide nuclei, the probability of superasymmetric fission is by six orders of magnitude smaller than for standard asymmetric fission. For the superheavy nuclei this probability is only by two orders of magnitude smaller. In all cases, the superasymmetric scission shapes are dumbbells with the heavy fragment close to a sphere. We have estimated the stability of the light fragment concerning the variation of the neck and found out that sequential ternary fission is not favored energetically. The calculations were carried out with nuclear shape described by generalized Cassinian ovals with six deformation parameters, <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mi>α</a:mi></a:math>, <b:math xmlns:b="http://www.w3.org/1998/Math/MathML"><b:msub><b:mi>α</b:mi><b:mn>1</b:mn></b:msub></b:math>, <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"><c:msub><c:mi>α</c:mi><c:mn>2</c:mn></c:msub></c:math>, <d:math xmlns:d="http://www.w3.org/1998/Math/MathML"><d:msub><d:mi>α</d:mi><d:mn>3</d:mn></d:msub></d:math>, <e:math xmlns:e="http://www.w3.org/1998/Math/MathML"><e:msub><e:mi>α</e:mi><e:mn>4</e:mn></e:msub></e:math>, and <f:math xmlns:f="http://www.w3.org/1998/Math/MathML"><f:msub><f:mi>α</f:mi><f:mn>5</f:mn></f:msub></f:math>. The configuration at the moment of the neck rupture was defined by fixing <g:math xmlns:g="http://www.w3.org/1998/Math/MathML"><g:mrow><g:mi>α</g:mi><g:mo>=</g:mo><g:mn>0.98</g:mn></g:mrow></g:math>. This value corresponds to a neck radius <h:math xmlns:h="http://www.w3.org/1998/Math/MathML"><h:mrow><h:msub><h:mi>r</h:mi><h:mi>neck</h:mi></h:msub><h:mo>≈</h:mo><h:mn>1.5</h:mn></h:mrow></h:math> fm. Published by the American Physical Society 2024

Physical review. CVol. 110(6)
Horia Hulubei National Institute for R and D in Physics and Nuclear Engineering (RO)
Openalex Percentile: Top 10%
Nuclear physics research studies
1.32
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Dumbbell shapes in the superasymmetric fission of heavy nuclei — N. Carjan, F. A. Ivanyuk · Physical review. C (2024) | TGRS Research Map | TGRS