Direct transition energies in strained ten-monolayer Ge/Si superlattices

1990 ◽  
Vol 65 (20) ◽  
pp. 2610-2610 ◽  
Author(s):  
Uwe Schmid ◽  
Niels E. Christensen ◽  
Manuel Cardona
Keyword(s):  
Direct Transition ◽  
Transition Energies

Modifications of direct transition energies in β-FeSi2 epitaxial films grown by molecular beam epitaxy

2009 ◽  
Vol 94 (24) ◽  
pp. 241907 ◽  
Author(s):  
K. Noda ◽  
Y. Terai ◽  
S. Hashimoto ◽  
K. Yoneda ◽  
Y. Fujiwara
Keyword(s):  
Molecular Beam Epitaxy ◽  
Molecular Beam ◽  
Epitaxial Films ◽  
Direct Transition ◽  
Transition Energies

The relativistic coupled-cluster method: transition energies of bismuth and eka-bismuth

1998 ◽  
Vol 94 (1) ◽  
pp. 181-187 ◽  
Author(s):  
EPHRAIM ELIAV ◽  
UZI KALDOR ◽  
YASUYUKI ISHIKAWA
Keyword(s):  
Cluster Method ◽  
Coupled Cluster ◽  
Coupled Cluster Method ◽  
Transition Energies

Measurements of the Rydberg Transition Energies for the n1S0 State and the Ionization Potential for 40Ca Atoms

JETP Letters ◽  
2019 ◽  
Vol 110 (12) ◽  
pp. 761-765
Author(s):  
B. B. Zelener ◽  
S. A. Saakyan ◽  
V. A. Sautenkov ◽  
E. V. Vilshanskaya ◽  
B. V. Zelener ◽  
...  
Keyword(s):  
Ionization Potential ◽  
Transition Energies ◽  
Rydberg Transition

scholarly journals Temperature-Induced Plasmon Excitations for the α–T3 Lattice in Perpendicular Magnetic Field

Nanomaterials ◽  
2021 ◽  
Vol 11 (7) ◽  
pp. 1720
Author(s):  
Antonios Balassis ◽  
Godfrey Gumbs ◽  
Oleksiy Roslyak
Keyword(s):  
Magnetic Field ◽  
Magnetic Fields ◽  
Zeeman Splitting ◽  
Mass Term ◽  
Energy Dispersive Spectrum ◽  
Wave Functions ◽  
Transition Energies ◽  
Gap Opening ◽  
Quantizing Magnetic Field

We have investigated the α–T3 model in the presence of a mass term which opens a gap in the energy dispersive spectrum, as well as under a uniform perpendicular quantizing magnetic field. The gap opening mass term plays the role of Zeeman splitting at low magnetic fields for this pseudospin-1 system, and, as a consequence, we are able to compare physical properties of the the α–T3 model at low and high magnetic fields. Specifically, we explore the magnetoplasmon dispersion relation in these two extreme limits. Central to the calculation of these collective modes is the dielectric function which is determined by the polarizability of the system. This latter function is generated by transition energies between subband states, as well as the overlap of their wave functions.

Direct-Transition Features in Stripping Collisions of Heavy Neutral Atoms and Ions

1972 ◽  
Vol 5 (4) ◽  
pp. 1784-1798 ◽  
Author(s):  
H. H. Fleischmann ◽  
R. C. Dehmel ◽  
S. K. Lee
Keyword(s):  
Neutral Atoms ◽  
Direct Transition
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