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Розрахунок властивостей ядер для iзотопiв 56–62Fe у модельному просторі осциляторних функцій з використанням NuShellX@MSU кода

Розрахунок властивостей ядер для iзотопiв 56–62Fe у модельному просторі осциляторних функцій з використанням NuShellX@MSU кода

The nuclear shell model has been applied to calculate the yrast energy levels, quadrupole transition probability (BE2), deformation parameter B2, rotational energy (hw), and inertia moment (20/h2) for the ground state band. The NuShellX@MSU code has been used to determine the nuclear properties of 5...

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Bibliographic Details
Main Author: Obeed, F.H.
Format: Article
Language:English
Published: Publishing house "Academperiodika" 2021
Subjects:
iрастовi рiвнi енергiї
ймовiрнiсть квадрупольного переходу
NuShellX@MSU код
параметр деформацiї
частота обертання
момент iнерцiї
yrast energy levels
quadrupole transition probability
NuShellX@MSU code
deformation parameter
rotational frequency
inertia moment
Determination of Nuclear Properties for 56-62Fe Isotopes in the Model Space (Ho) Using NuShellx Code
Online Access:https://ujp.bitp.kiev.ua/index.php/ujp/article/view/2020027
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Summary:The nuclear shell model has been applied to calculate the yrast energy levels, quadrupole transition probability (BE2), deformation parameter B2, rotational energy (hw), and inertia moment (20/h2) for the ground state band. The NuShellX@MSU code has been used to determine the nuclear properties of 56−62Fe isotopes, by using the harmonic oscillator (HO) model space for P (1f7/2), N (2p3/2), N (1f5/2), and N (2p1/2) orbits and (HO) interaction. The results are in good agreement with the available experimental data on the above nuclear properties and all nuclei under study. In addition, the back bending phenomenon has been explained by the calculations, and it has been very clear in 58,60,62Fe nuclei. It has also been confirmed and determined the most spins and parities of energy levels. In these calculations, new values have been theoretically determined for the most nuclear properties which were previously experimentally unknown.

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