We study the conditions under which the nucleons inside a deformed nucleus can undergo chaotic motion. To do this we perform self-consistent calculations in semiclassical approximation utilizing a multipole-multipole interaction of the Bohr-Mottelson type for quadrupole and octupole deformations. For the case of harmonic and nonharmonic static potentials, we find that both multipole deformations lead to regular motion of the collective coordinate, the multipole moment of deformation. However, despite this regular collective motion, we observe chaotic single-particle dynamics
AbstractBy computing the Poincaréʼs surfaces of section and Lyapunov exponents, we study the effect ...
The solutions of the semiclassical time–dependent Hartree–Fock-Bogoliubov equations of motion are st...
The phase space of the trajectories of one neutron in a deformed single particle potential is sketch...
We study the conditions under which the nucleons inside a deformed nucleus can undergo chaotic motio...
We study the motion of classical particles confined in a two-dimensional ‘‘nuclear'' billiard whose ...
We study the motion of classical particles confined in a two-dimensional ‘‘nuclear'' billiard whose ...
In order to understand the origin of one-body dissipation in nuclei, we analyze the behavior of a ga...
In order to understand the origin of one-body dissipation in nuclei, we analyze the behavior of a ga...
Abstract. We use two models of nuclear collective dynamics—the geometric collective model and the in...
We analyze on a classical 2D version of the “nuclear billiard” the onset of chaotic behaviour of the...
Here, the problem of the classical chaos effect on dissipation in nuclear many-body systems is addre...
The results for the classical single-particle motion in Woods-Saxon potential with octupole deformat...
The chaotic properties for six particles interacting by a monopole pairing force in a two-j shell mo...
We have presented a complete description of classical dynamics generated by the Hamiltonian of quadr...
The fact that there are more prolate-deformed nuclei than oblate-ones The fact that there are more ...
AbstractBy computing the Poincaréʼs surfaces of section and Lyapunov exponents, we study the effect ...
The solutions of the semiclassical time–dependent Hartree–Fock-Bogoliubov equations of motion are st...
The phase space of the trajectories of one neutron in a deformed single particle potential is sketch...
We study the conditions under which the nucleons inside a deformed nucleus can undergo chaotic motio...
We study the motion of classical particles confined in a two-dimensional ‘‘nuclear'' billiard whose ...
We study the motion of classical particles confined in a two-dimensional ‘‘nuclear'' billiard whose ...
In order to understand the origin of one-body dissipation in nuclei, we analyze the behavior of a ga...
In order to understand the origin of one-body dissipation in nuclei, we analyze the behavior of a ga...
Abstract. We use two models of nuclear collective dynamics—the geometric collective model and the in...
We analyze on a classical 2D version of the “nuclear billiard” the onset of chaotic behaviour of the...
Here, the problem of the classical chaos effect on dissipation in nuclear many-body systems is addre...
The results for the classical single-particle motion in Woods-Saxon potential with octupole deformat...
The chaotic properties for six particles interacting by a monopole pairing force in a two-j shell mo...
We have presented a complete description of classical dynamics generated by the Hamiltonian of quadr...
The fact that there are more prolate-deformed nuclei than oblate-ones The fact that there are more ...
AbstractBy computing the Poincaréʼs surfaces of section and Lyapunov exponents, we study the effect ...
The solutions of the semiclassical time–dependent Hartree–Fock-Bogoliubov equations of motion are st...
The phase space of the trajectories of one neutron in a deformed single particle potential is sketch...