Ryf. Yip et al., BAND ALIGNMENT ENGINEERING FOR HIGH-SPEED, LOW DRIVE FIELD QUANTUM-CONFINED STARK-EFFECT DEVICES, Journal of applied physics, 83(3), 1998, pp. 1758-1769
An analysis and discussion of the device physics for the quantum-confi
ned Stark effect based on barrier height and band alignment considerat
ions is presented. It identifies two important design principles for b
and structure engineering of the multi-quantum well stack: (1) Due to
the counterbalance relationship between field-induced redshift and fie
ld-induced polarization of the quantum well eigenstates, design strate
gies must look to attain an optimal balance or compromise between a mi
nimum drive field and maximum absorption coefficient change. This can
be achieved with an appropriate choice of the valence band discontinui
ty. (2) In III-V semiconductors, the strong asymmetry in the field res
ponse of the conduction and valence band eigenstates is due directly t
o the asymmetry of the conduction and valence band effective masses. A
s a result, optimum device performance is obtained by using a heterost
ructure with a disproportionately large conduction band offset to comp
ensate the effective mass asymmetry and balance the field-induced wave
function leakage in the conduction band to that in the valence band.
The relative wave function leakage between conduction and valence band
s is compared by examining tunneling currents through the quantum well
barriers as a function of the electric field and barrier height. For
conduction and valence band effective masses of, respectively, 0.055 a
nd 0.5 times the free electron mass, the optimal band alignment requir
es a conduction band discontinuity 3-9 times greater than the valence
band discontinuity. Applying these design principles for high speed, l
ow drive voltage optical modulators shows that the overall performance
of these devices may be improved by using a combination of balanced b
and alignments and low valence hand barriers. The low valence band bar
riers reduce the drive field required to operate the devices, which ha
s direct effects upon the drive voltage, device capacitance, attenuati
on coefficient, and optical coupling and propagation losses. The analy
sis and discussion is supported by experimental modulation depth and d
rive field data obtained from strained-layer multiple quantum well InA
sP/InP and strain-compensated InAsP/InGaP optical modulators fabricate
d with layers grown on InP(001) by metalorganic vapor phase epitaxy. (
C) 1998 American Institute of Physics. [S0021-8979(98)07203-X].