85
opens the doors to novel design and fabrication of high-speed optical modulators that
can be practical for system integration in on-chip optical interconnections. More work
on device structures and relevant materials growth and device fabrication needs to be
done.
6.2.1 Material Growth Improvements
As many problems emerged
from our measurement results, a number of them came
from the materials: (1) n type doping is ineffective. There is
a need to have higher
doping levels with a high activation rate to engineer the Fermi level. Better doping
control with arsenic and phosphorous needs to be achieved. (2)
High quality thin
buffer layers. Practical applications in optical communications require single optical
mode waveguide and cavity structures. The former needs
thinner buffer layers for
stronger coupling and the latter needs higher quality material with fewer dislocations
to reduce absorption. Moreover, high quality quantum
well material also improves
the I-V characteristics and reduces signal to noise ratio (3) Better control over
selective area growth.
6.2.2 Cavity Modulator
The Asymmetric Fabry-Perot (AFP) modulator cavity allows increased interaction
between light and active material in a smaller form factor. After the Ge/SiGe QW
QCSE electroabsorption, α, is experimentally determined for each sample, a range of
acceptable front and back mirror reflectances, R
f
and R
b
, can be determined from the
AFP design equation [98].
Currently, the DC characteristics of the fabricated device showed clear and high
contrast with low voltage swing. The next step is to improve the monolithic device
fabrication process and material deposition to match the cavity parameters.