photoexcitation spectrum
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2009 ◽  
Vol 113 (12) ◽  
pp. 2715-2723 ◽  
Author(s):  
Jang Sook Kwon ◽  
Chang Min Choi ◽  
Hwan Jin Kim ◽  
Nam Joon Kim ◽  
Joonkyung Jang ◽  
...  

2009 ◽  
Vol 96 (3) ◽  
pp. 602a
Author(s):  
Mino Yang ◽  
Jang Sook Kwon ◽  
Chang Min Choi ◽  
Whan Jin Kim ◽  
Nam Joon Kim ◽  
...  

JETP Letters ◽  
1998 ◽  
Vol 67 (10) ◽  
pp. 808-813
Author(s):  
R. I. Rokitskii ◽  
D. Yu. Parashchuk ◽  
T. A. Kulakov ◽  
V. M. Kobryanskii

1990 ◽  
Vol 140 (2) ◽  
pp. 307-316 ◽  
Author(s):  
James R. Chow ◽  
Robert A. Beaudet ◽  
Werner Schulz ◽  
Klaus Weyer ◽  
Herbert Walther

1989 ◽  
Vol 148 ◽  
Author(s):  
H.J. Von Bardeleben ◽  
J.C. Bourgoin ◽  
P. Basmaji ◽  
P. Gibart

ABSTRACTThe electron paramagnetic resonance study of the DX center in Sn doped direct gap Ga0.69Al0.31 As shows the existence of a shallow effective mass like excited configuration of this defect. The photoexcitation spectrum for this transformation has a threshold at 0.8 eV; the photoionization of the DX center is not a transition to the lowest r conduction band as previously assumed. After photoexcitation additional paramagnetic defects are observed.


1977 ◽  
Vol 46 (1) ◽  
pp. 125-128 ◽  
Author(s):  
Paras N. Prasad ◽  
A.I. Attia ◽  
A.H. Francis

1972 ◽  
Vol 50 (18) ◽  
pp. 2186-2193 ◽  
Author(s):  
B. Pajot ◽  
F. Merlet ◽  
G. Taravella

The Zeeman effect in the photoexcitation spectrum of phosphorus in silicon has been studied up to 64 kG in the Faraday configuration with the field parallel to the three principal axes of the crystal. In this work, we have observed a slight decrease of the transverse effective mass with the field and we found a fair agreement between theory and experiment for the 2p± and 3p± levels. Better agreement is obtained, however, if the variation of the effective Bohr radii with the magnetic field is taken into account. For the 2p0 and 3p0 levels, the variation of the effective Bohr radius [Formula: see text] alone cannot be observed experimentally in the Faraday configuration, but our results indicate a much more important decrease than for the p± levels and a variational calculation is necessary in this case. The shift of the 2p0 and 3p0 lines obeys roughly the n2(n2 − 1) relation, which should not be observed in the case of strong interactions with upper levels.


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