Add to ORKG887-891The 152-156Sm isotopes are classified as deformed nuclei. The phenomenological model is presented to describe the complete low-energy structure of 152-156Sm isotopes by taking into account the Coriolis mixing between states. The parameters fitted to the model are calculated. The energy spectra of positive-parity states which are found to be in good agreement with the experimental data are presented. It is found that the non-adiabaticity of rotational energy bands occurred at high spin due to the Coriolis effect. Few new states are predicted. </span
In this study, the quadrupole moments of the 166−180Hf, 180−186W and 152−168Sm isotopic chains have ...
Accounting for Coriolis mixing of experimentally known rotational bands non-adiabatic effects in ene...
The nuclear structures of even-even isotopes Nd (A=148,150,152) are studied by using the first Inte...
The 152–156Sm isotopes are classified as deformed nuclei. The phenomenological model is presented to...
Low-lying excited states and structure of even-even, deformed, rare earth 152,154,156Sm and 156,158,...
(〖E(8〗_1^+))/(〖E(2〗_1^+)),(〖E(6〗_1^+))/(〖E(2〗_1^+)) , ( 〖E(4〗_1^+))/(〖E(2〗_1^+)) and the ratios of I...
Interacting boson model (IBM-1) was used in the present work to study some of nuclear structures for...
The nucleus {sup 152}Sm is characterized by a variety of low-energy collective modes, conventionally...
Interacting boson model (IBM-1) was used in the present work to study some of nuclear structures for...
Recent high resolution (p; t) experiments have established the existence of a large number of low-ly...
A systematic investigation of low-lying levels of nuclides in the mass 150 region has been undertake...
A systematic investigation of low-lying levels of nuclides in the mass 150 region has been undertake...
The low-spin excitations of the nucleus 146Sm which is just two neutrons and two protons away from t...
In this work, non - adiabatic effects manifested in the magnetic properties of lowlying states of e...
Due to the character of the original source materials and the nature of batch digitization, quality ...
In this study, the quadrupole moments of the 166−180Hf, 180−186W and 152−168Sm isotopic chains have ...
Accounting for Coriolis mixing of experimentally known rotational bands non-adiabatic effects in ene...
The nuclear structures of even-even isotopes Nd (A=148,150,152) are studied by using the first Inte...
The 152–156Sm isotopes are classified as deformed nuclei. The phenomenological model is presented to...
Low-lying excited states and structure of even-even, deformed, rare earth 152,154,156Sm and 156,158,...
(〖E(8〗_1^+))/(〖E(2〗_1^+)),(〖E(6〗_1^+))/(〖E(2〗_1^+)) , ( 〖E(4〗_1^+))/(〖E(2〗_1^+)) and the ratios of I...
Interacting boson model (IBM-1) was used in the present work to study some of nuclear structures for...
The nucleus {sup 152}Sm is characterized by a variety of low-energy collective modes, conventionally...
Interacting boson model (IBM-1) was used in the present work to study some of nuclear structures for...
Recent high resolution (p; t) experiments have established the existence of a large number of low-ly...
A systematic investigation of low-lying levels of nuclides in the mass 150 region has been undertake...
A systematic investigation of low-lying levels of nuclides in the mass 150 region has been undertake...
The low-spin excitations of the nucleus 146Sm which is just two neutrons and two protons away from t...
In this work, non - adiabatic effects manifested in the magnetic properties of lowlying states of e...
Due to the character of the original source materials and the nature of batch digitization, quality ...
In this study, the quadrupole moments of the 166−180Hf, 180−186W and 152−168Sm isotopic chains have ...
Accounting for Coriolis mixing of experimentally known rotational bands non-adiabatic effects in ene...
The nuclear structures of even-even isotopes Nd (A=148,150,152) are studied by using the first Inte...