The γ -strength functions and level densities in the quasicontinuum of 147 , 149 Sm isotopes have been extracted from particle- γ coincidences using the Oslo method. The nuclei of interest were populated via (p,d) reactions on pure 148 , 150 Sm targets and the reaction products were recorded by the Hyperion array. An upbend in the low-energy region of the γ SF has been observed. The systematic analysis of the γ SF for a range of Sm isotopes highlights the interplay between scissors mode and the upbend. Shell-model calculations show reasonable agreement with the experimental γ SFs and confirm the correspondence between the upbend and scissors mode
International audienceParticle-γ coincidence experiments were performed at the Oslo Cyclotron Labora...
The level densities and γ-ray strength functions of 105 ,106,111,112Cd have been extracted from part...
The γ -ray strength function and level density in the quasi-continuum of 151,153Sm have been measure...
The nuclear level densities (NLDs) and the γ-ray strength functions (γSFs) of 153,155Sm have been ex...
We present experimental γ-ray strength functions up to Eγ ∼ Sn measured at the Oslo Cyclotron Labora...
We present experimental γ-ray strength functions up to Eγ ∼ Sn measured at the Oslo Cyclotron Lab...
The nuclear γ-ray strength function is one of the indispensable inputs needed for reaction-rate calc...
The γ-ray strength functions and nuclear level densities in the quasi-continuum of 180,181Ta are ext...
The experimental γ-ray strength functions (γSFs) of 142,144–151Nd have been studied for γ-ray energi...
Particle- γ coincidence experiments were performed at the Oslo Cyclotron Laboratory with the 181 Ta...
The γ -ray strength functions and nuclear level densities in the quasi-continuum of 180,181Ta are ex...
The γ decay of highly excited nuclear levels can be described within the statistical model of nucleu...
The nuclei 163,164 Dy were analyzed at the Oslo Cyclotron laboratory (OCL) by use of the so-called O...
Nuclei in the 135I region have been identified as being a possible bottleneck for the i process. Her...
The γ-ray strength function and level density of 111, 112, 113Sn are being studied at the Oslo Cyclo...
International audienceParticle-γ coincidence experiments were performed at the Oslo Cyclotron Labora...
The level densities and γ-ray strength functions of 105 ,106,111,112Cd have been extracted from part...
The γ -ray strength function and level density in the quasi-continuum of 151,153Sm have been measure...
The nuclear level densities (NLDs) and the γ-ray strength functions (γSFs) of 153,155Sm have been ex...
We present experimental γ-ray strength functions up to Eγ ∼ Sn measured at the Oslo Cyclotron Labora...
We present experimental γ-ray strength functions up to Eγ ∼ Sn measured at the Oslo Cyclotron Lab...
The nuclear γ-ray strength function is one of the indispensable inputs needed for reaction-rate calc...
The γ-ray strength functions and nuclear level densities in the quasi-continuum of 180,181Ta are ext...
The experimental γ-ray strength functions (γSFs) of 142,144–151Nd have been studied for γ-ray energi...
Particle- γ coincidence experiments were performed at the Oslo Cyclotron Laboratory with the 181 Ta...
The γ -ray strength functions and nuclear level densities in the quasi-continuum of 180,181Ta are ex...
The γ decay of highly excited nuclear levels can be described within the statistical model of nucleu...
The nuclei 163,164 Dy were analyzed at the Oslo Cyclotron laboratory (OCL) by use of the so-called O...
Nuclei in the 135I region have been identified as being a possible bottleneck for the i process. Her...
The γ-ray strength function and level density of 111, 112, 113Sn are being studied at the Oslo Cyclo...
International audienceParticle-γ coincidence experiments were performed at the Oslo Cyclotron Labora...
The level densities and γ-ray strength functions of 105 ,106,111,112Cd have been extracted from part...
The γ -ray strength function and level density in the quasi-continuum of 151,153Sm have been measure...