In separate confined heterostructure (SCH) lasers, injected electrons
and holes thermalize into a quantum well after diffusion through the o
uter cladding layers. The carriers move towards equilibrium by emittin
g optical phonons. In narrow quantum wells, as compared to the 1-2 ps
required in bulk semi-conductors, this phonon emission process can be
considerably slowed down due to the 2-D density of states and the natu
re of the electron-optical phonon interaction. This process has been s
tudied theoretically using a Monte Carlo program which allows us to se
e the carrier distribution as a function of time. Typical times for ca
rrier relaxation are 10-15 ps for a 50 angstrom GaAs well with Al0.30G
a0.70As barriers and approximately 5 ps for a 200 angstrom well. These
calculations have been complemented by time-resolved photoluminescenc
e measurements on SCH structures where the relaxation time from a 3D d
istribution into In0.20Ga0.80As/GaAs wells is measured at T = 200 K. C
arrier relaxation times of 50, 41, 22, and 17 ps are obtained for well
s of sizes 30, 40, 50, and 100 angstrom, respectively. The results sho
w clearly that the use of narrow quantum wells in low threshold lasers
will pose a serious limitation to the efficiency and small-signal mod
ulation bandwidth of these devices.