The Role of EL2 for the Mobility-Lifetime Product of Photoexcited Electrons in GaAs
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		    The role of EL2 for the mobility-lifetime product of photoexcited electrons in GaAs G. C. Valley Hughes Research Laboratories Malibu, Ca 90265 - USA H.J. von Bardeleben Groupe de Physique des Solides de I' Ecole Normale Sup~rieure Centre national de la Recherche Scientifique Tour 23, 2 place Jussieu 75251 Paris Cedex 05, France. H. Rajbenbach Laboratoire Central de Recherches Thomson-CSF Domaine de Corbeville 91404 Orsay Cedex, France
 
 abstract The mobility
 
 lifetime
 
 products for
 
 photo-electrons
 
 in semi-insulating
 
 GaAs,
 
 which
 
 fit
 
 successfully the results of photorefractive studies undertaken in the presence of electric fields
 
 are
 
 three
 
 orders
 
 of
 
 magnitude
 
 smaller
 
 than
 
 those
 
 inferred
 
 from
 
 transport
 
 measurements or from the photorefractive effect with no applied electrical field. Consideration of enhanced recombination via EL2 effective-mass states linked to the Lconduction band minimum allows us to fit the dependence of the photorefractive beam coupling gain coefficient on the grating period for both AC fields and moving gratings. A cascade-capture process, which is three orders of magnitude faster than recombination by multiphonon emission from the products for field influence
 
 of
 
 the
 
 strengths EL2
 
 r
 
 band to EL2, leads to greatly reduced mobility-lifetime
 
 greater than 1 kV/cm. Our results establish
 
 defect properties
 
 on the
 
 recombination
 
 processes
 
 the dominant essential
 
 for
 
 modelling and optimizing the photorefractive effect in semi-insulating GaAs.
 
 Undoped semi-insulating GaAs is an important electronic material and since 1984 has been shown to have very promising properties for beam coupling, phase conjugation and optical data
 
 processing
 
 [1-7].
 
 EL2
 
 is the dominant native defect in this material with a 16 concentration of typically 2.10 cm -3. It dominates the extrinsic absorption spectrum by the photoionisation from the valence band and to the conduction band. Without an external applied field, in GaAs
 
 however, coupling coefficients in photorefractive experiment are rather small
 
 because of its small electro-optic coefficient. To increase the coupling coefficient
 
 many researchers have applied external DC and AC fields to enhance charge transport and Mat. Res. Soc. Symp. Proc. Vol. 163. @1990 Materials Research Society
 
 838
 
 obtain large internal space-charge field grating [3,4,6,7]. This has led to larger coupling coefficients, but the results are in disagreement with theoretical predictions based on photorefractive theories and intrinsic properties of semi-insulating GaAs [7-9]. Here we explicitly demonstrate this discrepancy between theoretical prediction and experimental result in measurements made on undoped GaAs in which the defect responsible for the photorefractive effects in EL2. The results can be consistently interpreted in terms of enhanced recombination in the presence of large electric fields.
 
 Nd:YA6 laser X,= 1.06pro
 
 I 
 
 IS.
 
 C,aAs
 
 's
 
 Fig.l: Photorefractive two-beam coupling experiment (ref.15). The optical beams photoinduce a phase volume grating in GaAs a		
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