beta transition
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Author(s):  
Chenoa D. Tremblay ◽  
Christopher H. Jordan ◽  
Maria Cunningham ◽  
Paul A. Jones ◽  
Natasha Hurley-Walker

AbstractWe detail tentative detections of low-frequency carbon radio recombination lines from within the Orion molecular cloud complex observed at 99–129 MHz. These tentative detections include one alpha transition and one beta transition over three locations and are located within the diffuse regions of dust observed in the infrared at 100 μm, the Hα emission detected in the optical, and the synchrotron radiation observed in the radio. With these observations, we are able to study the radiation mechanism transition from collisionally pumped to radiatively pumped within the H ii regions within the Orion molecular cloud complex.


Optik ◽  
2016 ◽  
Vol 127 (10) ◽  
pp. 4470-4472 ◽  
Author(s):  
H. Yurtseven ◽  
O. Tari

2016 ◽  
Author(s):  
Hamit Yurtseven ◽  
Özlem Tari ◽  
Ayşegül Gümüş
Keyword(s):  

2010 ◽  
Vol 19 (07) ◽  
pp. 1383-1409 ◽  
Author(s):  
S. KERROUCHI ◽  
N. H. ALLAL ◽  
M. FELLAH ◽  
M. DOUICI

Particle-number fluctuations effects on the beta transition probabilities are studied in the neutron–proton pairing framework. The Hamiltonian of the system has been considered in its most general form and has been diagonalized by means of the linearization method. However, since the generalized Bogoliubov–Valatin transformation obtained in this way leads to a quasi-particle Hamiltonian which is still nondiagonal, a rediagonalization has been performed. The corresponding wave functions have been projected on both the good neutron and proton numbers using a recently proposed method. Expressions of the beta transition probabilities which strictly conserve the particle-number have then been established. As a first step, the model has been numerically tested within the framework of the schematic one-level model. As a second step, nuclei such as N = Z has been studied using the single-particle energies and eigenstates of the Woods–Saxon deformed mean field. It has thus been shown the necessity of: (i) including the isovector pairing correlations, (ii) performing a rediagonalization of the Hamiltonian, (iii) performing a particle-number projection, (iv) carefully choice the pairing-strength values, when calculating the transition probabilities.


Pramana ◽  
2007 ◽  
Vol 69 (3) ◽  
pp. 369-375 ◽  
Author(s):  
D. I. Salamov ◽  
S. Unlu ◽  
N. Cakmak
Keyword(s):  

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