U. Pietsch et al., DETERMINATION OF THE ANHARMONICITY CONSTANT OF GAAS BY MEANS OF THE BIJVOET RELATION OF THE WEAK (666) REFLECTION, Acta crystallographica. Section B, Structural science, 49, 1993, pp. 822-825
As a result of the influence of anomalous dispersion the weak (hhh) an
d (hhhBAR) reflections of the zinc blende structure differ from each o
ther. At large scattering vectors this difference, described by the Bi
jvoet relation B, depends solely on the size of the anharmonic force c
onstant beta. It can be determined by measuring B near the K-absorptio
n edge of any constituent. This experiment was performed for the (666)
and (666BAR) reflections of GaAs between lambda = 0.90 and 0.97 angst
rom using synchrotron radiation. Outside the extended X-ray absorption
fine-structure spectroscopy region the integrated intensities decreas
e in a different manner with increasing lambda for both reflections me
asured at 'umweganregung' free azimuthal positions. Under the assumpti
on Of beta(Ga) = -beta(As) and using the measured wavelength dependenc
e of B, the anharmonicity constant is evaluated to beta = - 1.75 (0.15
) x 10(-17) J angstrom-3 which is nearly the same as that for germaniu
m.