Jh. Irby et Wd. Hunt, CALCULATION OF DELTA-N(2) AND KAPPA FOR AN ACOUSTICALLY INDUCED DISTRIBUTED-BRAGG-REFLECTOR (ADBR), IEEE journal of quantum electronics, 34(2), 1998, pp. 213-224
The preliminary feasibility analysis and theoretical design of an acou
stically induced distributed Bragg reflector (ADBR) suitable for possi
ble integration with a III-V semiconductor laser is presented, The pro
posed ADBR structure consists of a simple unapodized interdigitated tr
ansducer (IDT) patterned by e-beam lithography atop a III-V compound s
emiconductor optical waveguide structure, It is proposed that a gigahe
rtz-range surface acoustic wave (SAW) could present a tunable distribu
ted Bragg reflector (DBR) index grating to a colinearly propagating gu
ided optical wave, Both the change in the impermeability tensor, Delta
n(2), and the resulting distributed feedback (DFB) coupling coefficie
nt, kappa, in the ADBR section are calculated due to only the classic
photoelastic effect by employing a Laguerre polynomial SAW analysis te
chnique, The SAW fields are normalized using the normal mode IDT equiv
alent circuit model and a power balance technique to provide realistic
kappa values in order to assess the feasibility of this device while
driven at its center frequency, The analysis of the ADBR kappa is limi
ted to the coupling between counterpropagating TE optical modes and is
calculated using general overlap integral expression, For an example
lambda(o), = 1.55 mu m In1-xGaxAsyP1-y-InP multiple-quantum-well (MQW)
laser structure coated with a 0.1-mu m ZnO piezoelectric layer, the m
aximum ADBR re was calculated to be 4.9 cm(-1) when using a series-ind
uctor-tuned submicron electrode IDT-SAW reflector configuration driven
by a RF source operating at approximately 2.9 GHz. It is shown that e
xceeding the maximum strain on the substrate or the occurrence of diel
ectric breakdown can put an upper limit on the realizable value of kap
pa. The potential optical tunability of an ADBR section is estimated f
or the case when an unapodized IDT is used for SAW generation, Finally
, various fabrication and design techniques are listed which may enhan
ce the ADBR kappa value, along with a list of other physical effects w
hich may need to be considered in future analyses.