TY - JOUR
T1 - Physical mechanisms of photoluminescence of InGaAs(N) alloy films grown by MOVPE
AU - Sanorpim, Sakuntam
AU - Nakajima, F.
AU - Imura, S.
AU - Katayama, R.
AU - Wu, J.
AU - Onabe, K.
AU - Shiraki, Y.
PY - 2002/12/1
Y1 - 2002/12/1
N2 - Reported here are some results of temperature and excitation power dependences of photoluminescence (PL) from the InGaAs(N) (In = 10.5%, 17.0% and N = 0-2.3%) alloy films grown at 530 °C and 600 °C by metalorganic vapour phase epitaxy (MOVPE). The InGaAs(N) alloy films emitting at room temperature in the wavelength (λ) range of 0.97-1.23 μm have been investigated. The low-temperature PL spectra in this set of samples are dominated by multiple peak emissions associated with both near-band-edge emission of InGaAs(N) (high energy peak, EPH) and strongly localized states (lower energy peaks, EPL) much lower than the InGaAs(N) band-gap. The temperature dependence of integrated PL intensity indicates the presence of non-radiative recombination centers with the localization energy (Eloc = 9.4-25.8 meV), which increased with increasing N concentration. Here we noted that Eloc are in agreement with the energy difference of EPH and EPL peaks. The α values extracted from the relation IPL ∝ Iexα are used to examine the recombination process. In the N-containing layers it is demonstrated that free-excitons, not free-carriers, mainly govern the radiative recombination.
AB - Reported here are some results of temperature and excitation power dependences of photoluminescence (PL) from the InGaAs(N) (In = 10.5%, 17.0% and N = 0-2.3%) alloy films grown at 530 °C and 600 °C by metalorganic vapour phase epitaxy (MOVPE). The InGaAs(N) alloy films emitting at room temperature in the wavelength (λ) range of 0.97-1.23 μm have been investigated. The low-temperature PL spectra in this set of samples are dominated by multiple peak emissions associated with both near-band-edge emission of InGaAs(N) (high energy peak, EPH) and strongly localized states (lower energy peaks, EPL) much lower than the InGaAs(N) band-gap. The temperature dependence of integrated PL intensity indicates the presence of non-radiative recombination centers with the localization energy (Eloc = 9.4-25.8 meV), which increased with increasing N concentration. Here we noted that Eloc are in agreement with the energy difference of EPH and EPL peaks. The α values extracted from the relation IPL ∝ Iexα are used to examine the recombination process. In the N-containing layers it is demonstrated that free-excitons, not free-carriers, mainly govern the radiative recombination.
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U2 - 10.1002/1521-3951(200212)234:3<782::AID-PSSB782>3.0.CO;2-0
DO - 10.1002/1521-3951(200212)234:3<782::AID-PSSB782>3.0.CO;2-0
M3 - Article
AN - SCOPUS:0036929945
SN - 0370-1972
VL - 234
SP - 782
EP - 786
JO - Physica Status Solidi (B): Basic Research
JF - Physica Status Solidi (B): Basic Research
IS - 3
ER -