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10. Appendix

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A4.1 A Prototypical Deep Center in N-Type Zincblende-Type Semiconductors 679<br />

iments have firmly established that the deep centers induced by pressure in<br />

GaAs have the same properties as the DX center found in AlGaAs and, furthermore,<br />

this conversion of shallow donors to DX centers occurred also for<br />

other group IV donors, such as Ge and Sn, and group VI donors like S, Se<br />

and Te. In fact, it has been shown that the effect of a hydrostatic pressure of<br />

0.1 GPa on the DX in GaAs is almost equivalent to adding 1% of Al [Wei89].<br />

It has been known that both pressure and alloying with Al have the similar<br />

effect of lowering the conduction band minima at the X point of the Brillouin<br />

zone in GaAs relative to the zone-center conduction band valley. With<br />

sufficient pressure or Al concentration GaAs can be converted from a direct<br />

band gap semiconductor into an indirect one. At ambient pressure the DX<br />

level associated with donor atoms in GaAs is actually a resonant state above<br />

the conduction band. As a result of the change in the conduction band structure<br />

caused by alloying or by pressure, the DX level emerges from the conduction<br />

band into the band gap and becomes the stable ground state of the<br />

donor. Thus, one can conclude that the DX center is the result of a so-called<br />

“shallow-to-deep transformation” of substitutional donors in GaAs induced by<br />

changes in the conduction band structure. In this transformation the chemical<br />

nature of the impurity plays only a secondary role.<br />

E (eV)<br />

2.5<br />

2.0<br />

1.5<br />

Al Ga As<br />

x 1-x<br />

1.4<br />

0 0.2 0.4 0.6 0.8 1.0<br />

GaAs AlAs Mole Fraction x AlAs<br />

Γ<br />

L<br />

X<br />

E(eV)=0.54x+1.57<br />

Fig. A4.4 The DX center energy<br />

level (open squares) determined by<br />

Chand et al. from temperature-dependent<br />

Hall effect measurement on<br />

Si doped AlGaAs as a function of<br />

the AlAs mole fraction. For comparison<br />

the solid curves labeled as °,<br />

L and X show, respectively, the corresponding<br />

dependence of the direct<br />

band gap energy at the zone center,<br />

the indirect band gap energies between<br />

the conduction valleys at the<br />

L and X points and the zone-center<br />

valence band maximum. Reproduced<br />

from Chand et al. [Chand84].

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