Microscopic analysis ofS34(d→,d’)34S*and the relative sign of neutron and proton transition matrix elements for the (0+-22+) transition

1991 ◽  
Vol 44 (2) ◽  
pp. 912-914 ◽  
Author(s):  
Subinit Roy ◽  
S. K. Datta
1984 ◽  
Vol 52 (21) ◽  
pp. 1876-1879 ◽  
Author(s):  
A. Saha ◽  
Kamal K. Seth ◽  
M. Artuso ◽  
B. Harris ◽  
R. Seth ◽  
...  

1982 ◽  
Vol 114 (6) ◽  
pp. 419-422 ◽  
Author(s):  
A. Saha ◽  
Kamal K. Seth ◽  
D. Barlow ◽  
H. Nann ◽  
W.W. Jacobs

1985 ◽  
Vol 31 (2) ◽  
pp. 697-700 ◽  
Author(s):  
R. Alarcon ◽  
J. Rapaport ◽  
R. T. Kouzes ◽  
W. H. Moore ◽  
B. A. Brown

2001 ◽  
Vol 08 (03n04) ◽  
pp. 321-325
Author(s):  
ŞAKIR ERKOÇ ◽  
HATICE KÖKTEN

We have performed self-consistent field (SCF) calculations of the electronic structure of GaAs/Ga 1-x Al x As superlattices with parabolic potential profile within the effective mass theory. We have calculated the optical transition matrix elements involving transitions from the hole states to the electron states, and we have also computed the oscillator strength matrix elements for the transitions among the electron states.


2017 ◽  
Vol 95 (1) ◽  
Author(s):  
B. A. Brown ◽  
A. B. Garnsworthy ◽  
T. Kibédi ◽  
A. E. Stuchbery

1981 ◽  
Vol 103 (4-5) ◽  
pp. 255-258 ◽  
Author(s):  
A.M. Bernstein ◽  
V.R. Brown ◽  
V.A. Madsen

2019 ◽  
Vol 9 (1) ◽  
Author(s):  
Onno R. Diermann ◽  
Martin Holthaus

AbstractWe demonstrate that a periodically driven quantum system can adopt a quasistationary state which is effectively much colder than a thermal reservoir it is coupled to, in the sense that certain Floquet states of the driven-dissipative system can carry much higher population than the ground state of the corresponding undriven system in thermal equilibrium. This is made possible by a rich Fourier spectrum of the system’s Floquet transition matrix elements, the components of which are addressed individually by a suitably peaked reservoir density of states. The effect is expected to be important for driven solid-state systems interacting with a phonon bath predominantly at well-defined frequencies.


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