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Электронный каталог: Ganev, H. G. - Symplectic Symmetry Approach to Multicluster Nuclear Systems: The Case of *1*6O
Ganev, H. G. - Symplectic Symmetry Approach to Multicluster Nuclear Systems: The Case of *1*6O
Статья
Автор: Ganev, H. G.
Nuclear Physics A: Symplectic Symmetry Approach to Multicluster Nuclear Systems: The Case of *1*6O
б.г.
ISBN отсутствует
Автор: Ganev, H. G.
Nuclear Physics A: Symplectic Symmetry Approach to Multicluster Nuclear Systems: The Case of *1*6O
б.г.
ISBN отсутствует
На полку
Статья
Ganev, H.G.
Symplectic Symmetry Approach to Multicluster Nuclear Systems: The Case of *1*6O / H.G.Ganev // Nuclear Physics A. – 2025. – Vol. 1062. – P. 123162. – URL: https://doi.org/10.1016/j.nuclphysa.2025.123162. – Bibliogr.: 84.
Symplectic symmetry approach to clustering (SSAC) in the atomic nucleus is generalized for the more general multicluster nuclear systems. In the limiting case when 𝐴&sub(1) = 𝐴&sub(2) =…= 𝐴&sub(k) = 4 one obtains a microscopic counterpart within the SSAC of the wide class of various multi-𝛼-particle cluster models. As an example, the new microscopic approach is applied to the 4𝛼 cluster nuclear system of &sup(16)O. A good description for the excited states in the lowest 𝐾&sup(*p) = 0&sup(+)&sub(1) , 𝐾&sup(*p) = 0&sup(+)&sub(2) , 𝐾&sup(*p) = 0*sup(−)&sub(1) , 𝐾&sup(*p) = 2&sup(+)&sub(1) , 𝐾&sup(*p) = 3&sup(−)&sub(1) and 𝐾&sup(*p) = 1&sup(−)&sub(1) bands in &sup(16)O with experiment, as well as for the experimentally known 𝐵(𝐸2) low-energy transitions without the use of an effective charge, is obtained.
Спец.(статьи,препринты) = С 341 а - Различные модели ядер$
ОИЯИ = ОИЯИ (JINR)2025
Ganev, H.G.
Symplectic Symmetry Approach to Multicluster Nuclear Systems: The Case of *1*6O / H.G.Ganev // Nuclear Physics A. – 2025. – Vol. 1062. – P. 123162. – URL: https://doi.org/10.1016/j.nuclphysa.2025.123162. – Bibliogr.: 84.
Symplectic symmetry approach to clustering (SSAC) in the atomic nucleus is generalized for the more general multicluster nuclear systems. In the limiting case when 𝐴&sub(1) = 𝐴&sub(2) =…= 𝐴&sub(k) = 4 one obtains a microscopic counterpart within the SSAC of the wide class of various multi-𝛼-particle cluster models. As an example, the new microscopic approach is applied to the 4𝛼 cluster nuclear system of &sup(16)O. A good description for the excited states in the lowest 𝐾&sup(*p) = 0&sup(+)&sub(1) , 𝐾&sup(*p) = 0&sup(+)&sub(2) , 𝐾&sup(*p) = 0*sup(−)&sub(1) , 𝐾&sup(*p) = 2&sup(+)&sub(1) , 𝐾&sup(*p) = 3&sup(−)&sub(1) and 𝐾&sup(*p) = 1&sup(−)&sub(1) bands in &sup(16)O with experiment, as well as for the experimentally known 𝐵(𝐸2) low-energy transitions without the use of an effective charge, is obtained.
Спец.(статьи,препринты) = С 341 а - Различные модели ядер$
ОИЯИ = ОИЯИ (JINR)2025
