TY - GEN
T1 - Measurement of intensity-dependent carrier lifetime in doping superlattices
AU - Chavez-Pirson, A.
AU - Park, S. H.
AU - Pereira, M.
AU - Peyghambarian, Nasser
AU - Lehman, J. A.
AU - Ruden, P. P.
AU - Hibbs-Brenner, M. K.
PY - 1989
Y1 - 1989
N2 - A structure grown by metalorganic chemical vapor deposition (MOCVD), consisting of ten periods of alternating layers of n- and p-doped GaAs 130-nm thick with a doping concentration of 2 × 1017, was studied. The nonlinear transmission spectrum as a function of intensity as well as the intensity-dependent carrier buildup and decay lifetimes were measured directly using a pump-probe technique. The differential transmission spectrum (ΔT/T) at various pump intensities and the buildup time required to obtain the maximum modulation for a given intensity are shown and discussed. The intensity-dependent decay dynamics was measured by delaying the probe relative to the falling edge of the pump pulse. On a log-log scale the decay of the maximum modulation is linear, indicating a decay time that increases exponentially with decreasing carrier density. Both the buildup and decay dynamics can be effectively modeled with a rate equation whose carrier decay time depends exponentially on carrier density.
AB - A structure grown by metalorganic chemical vapor deposition (MOCVD), consisting of ten periods of alternating layers of n- and p-doped GaAs 130-nm thick with a doping concentration of 2 × 1017, was studied. The nonlinear transmission spectrum as a function of intensity as well as the intensity-dependent carrier buildup and decay lifetimes were measured directly using a pump-probe technique. The differential transmission spectrum (ΔT/T) at various pump intensities and the buildup time required to obtain the maximum modulation for a given intensity are shown and discussed. The intensity-dependent decay dynamics was measured by delaying the probe relative to the falling edge of the pump pulse. On a log-log scale the decay of the maximum modulation is linear, indicating a decay time that increases exponentially with decreasing carrier density. Both the buildup and decay dynamics can be effectively modeled with a rate equation whose carrier decay time depends exponentially on carrier density.
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M3 - Conference contribution
AN - SCOPUS:0024898476
SN - 1557520860
T3 - CONFERENCE ON LASERS AND ELECTRO-0PTICS
SP - 284
EP - 285
BT - CONFERENCE ON LASERS AND ELECTRO-0PTICS
A2 - Anon, null
PB - Publ by IEEE
T2 - Summaries of Papers Presented at the Conference on Lasers and Electro-Optics
Y2 - 24 April 1989 through 28 April 1989
ER -