Radiative recombination center inAs2Se3as studied by optically detected magnetic resonance

1990 ◽  
Vol 42 (18) ◽  
pp. 11845-11856 ◽  
Author(s):  
J. Ristein ◽  
P. C. Taylor ◽  
W. D. Ohlsen ◽  
G. Weiser
1989 ◽  
Vol 163 ◽  
Author(s):  
K. L. Brower

AbstractAn isotropic optically detected magnetic resonance (ODMR) having a Lorentzian lineshape at g - 2.050 ± 0.003 and linewidth (FWHM) of 67.3 mT is observed in GaP doped with 6 - 9 × 1017 S/cm3. The ODMR at g - 2.050 is believed to arise from free electrons (or holes) in the conduction (valence) band. This ODMR is completely quenched due to non-radiative recombination in the vicinity of g - 1.99.


1982 ◽  
Vol 46 (5) ◽  
pp. 473-500 ◽  
Author(s):  
S. Depinna ◽  
B. C. Cavenett ◽  
I. G. Austin ◽  
T. M. Searle ◽  
M. J. Thompson ◽  
...  

1987 ◽  
Vol 104 ◽  
Author(s):  
W. M. Chen ◽  
M. Godlewski ◽  
B. Monemar ◽  
H. P. Gislason

ABSTRACTA range of PGa antisite-related complex defects in LEC GaP:Cu, Li was observed with optically detected magnetic resonance. These isoelectronic defects are formed by a compensation of the PGa double donor by the CUGadouble acceptor on adjacent cation sites. T electronic structure of these defects is discussed, as well as their role in non-radiative recombination.


1987 ◽  
Vol 109 ◽  
Author(s):  
B. C. Hess ◽  
J. Shinar ◽  
Z. Vardeny ◽  
E. Ehrenfreund ◽  
F. Wudl

ABSTRACTFrom detailed optically detected magnetic resonance measurements in polythiophene, we show that the g=2.003 signal is luminescence enhancing, and that the signal comes from a broad photoluminescence band peaking near 1.65 eV. This band is tentatively assigned to Phe radiative recombination of polarons, with lifetimes between 10-8 and 5×10-5sec.


1998 ◽  
Vol 264-268 ◽  
pp. 599-602 ◽  
Author(s):  
Nguyen Tien Son ◽  
Matthias Wagner ◽  
E. Sörman ◽  
W.M. Chen ◽  
Bo Monemar ◽  
...  

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.


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