Exchange interactions of excitons localized at opposite interfaces in type-II GaAs/AlAs superlattices: Optically detected magnetic resonance and level anticrossing

JETP Letters ◽  
1996 ◽  
Vol 64 (10) ◽  
pp. 754-759 ◽  
Author(s):  
P. G. Baranov ◽  
N. G. Romanov ◽  
A. Hofstaetter ◽  
A. Scharmann ◽  
C. Schnorr ◽  
...  
1988 ◽  
Vol 61 (1) ◽  
pp. 129-132 ◽  
Author(s):  
H. W. van Kesteren ◽  
E. C. Cosman ◽  
F. J. A. M. Greidanus ◽  
P. Dawson ◽  
K. J. Moore ◽  
...  

1991 ◽  
Vol 220 ◽  
Author(s):  
T. A. Kennedy ◽  
E. R. Glaser ◽  
J. M. Trombetta ◽  
K. L. Wang ◽  
C. H. Chern ◽  
...  

ABSTRACTSi1−xGex/Si heterostructures with varying layer-thicknesses have been characterized using photoluminescence and magnetic resonance detected on photoluminescence. Three of the four samples studied exhibit sharp photoluminescence bands at different energies. For a 120 Å Si/40 Å Si1−xGex heterostructure, magnetic resonance of an electron in the Si and of a hole in the Sil. xGex layers were observed. These results indicate cross-interface, or Type II, excitonic recombination. Further, anisotropie magnetic resonance spectra indicate the presence of dangling-bonds defects in the heterostructures.


1998 ◽  
Vol 536 ◽  
Author(s):  
H. Porteanu ◽  
A. Glozman ◽  
E. Lifshitz ◽  
A. Eychmüller ◽  
H. Weller

AbstractCdS/HgS/CdS nanoparticles consist of a CdS core, epitaxially covered by one or two monolayers of HgS and additional cladding layers of CdS. The present paper describes our efforts to identify the influence of CdS/HgS/CdS interfaces on the localization of the photogenerated carriers deduced from the magneto-optical properties of the materials. These were investigated by the utilization of optically detected magnetic resonance (ODMR) and double-beam photoluminescence spectroscopy. A photoluminescence (PL) spectrum of the studied material, consists of a dominant exciton located at the HgS layer, and additional non-excitonic band, presumably corresponding to the recombination of trapped carriers at the interface. The latter band can be attenuated using an additional red excitation. The ODMR measurements show the existence of two kinds of electron-hole recombination. These electron-hole pairs maybe trapped either at a twin packing of a CdS/HgS interface, or at an edge dislocation of an epitaxial HgS or a CdS cladding layer.


1985 ◽  
Vol 32 (4) ◽  
pp. 2273-2284 ◽  
Author(s):  
K. M. Lee ◽  
Le Si Dang ◽  
G. D. Watkins ◽  
W. J. Choyke

1997 ◽  
Vol 6 (10) ◽  
pp. 1381-1384 ◽  
Author(s):  
N.T. Son ◽  
E. Sörman ◽  
W.M. Chen ◽  
C. Hallin ◽  
O. Kordina ◽  
...  

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