L&#220; Yi-jun, GAO Yu-lin, ZHENG Jian-sheng, CAI Zhi-gang, SANG Hai-yu, ZENG Xue-ran. Luminescence Decay of Partially Ordered (Al<sub>x</sub>Ga<sub>1-x</sub>)<sub>0.51</sub>In<sub>0.49</sub>P(<i>x</i>=0.29) Alloy[J]. Chinese Journal of Luminescence, 2002,23(2): 129-132
L&#220; Yi-jun, GAO Yu-lin, ZHENG Jian-sheng, CAI Zhi-gang, SANG Hai-yu, ZENG Xue-ran. Luminescence Decay of Partially Ordered (Al<sub>x</sub>Ga<sub>1-x</sub>)<sub>0.51</sub>In<sub>0.49</sub>P(<i>x</i>=0.29) Alloy[J]. Chinese Journal of Luminescence, 2002,23(2): 129-132DOI:
time-resolved photoluminescence(TRPL) was applied to study the optical properties of partially ordered quaternary (Al
x
Ga
1-x
)
0.51
In
0.49
P(
x
=0.29) alloy grown by MOVPE
the process of the transfer of carriers and the blue-shift of PL peak in (Al
x
Ga
1-x
)
0.51
In
0.49
P(
x
=0.29) alloy are directly observed.Both excitation-wavelength dependence of lifetime and excitation-intensity dependence of lifetime show wide distribution of carriers along bands.In TRPL spectra measured at 77K
the PL peak almost keeps unchanged
while at 300K
the PL peak has a small blue-shift with the delay of time
which is completely opposite to the character of donor-acceptor pair (DAP). The blue-shift phenomenon apparently suggests the occurrence of transfer of carriers and is coincident with the report of the Z-shape character of the PL temperature-dependent spectra
in which an anomalous blue-shift of PL peak energy occurs between 55K and 84K. This phenomenon further indicates the existence of sub-bands which is derived from the superlattice effect of ordered structure
which is a so-called orientational superlattice structure and which is considered to be a composite of the low-band-gap ordered domains in a high-band-gap disordered matrix. Thus
this phenomenon verifies our conjecture about band-folding effect of conduction band from L band to Γ band
i.e.
the carriers transfer from Γ band to L band during the decay time. The transfer of carriers between Γ and L band reveals the origin of the anomalous blue-shift in the PL temperature-dependent spectra as well. The single exponential component fitting equation suggests the same category carriers of Γ band and L band. The transfer of carriers at 300K is more apparent than that at 77K. This is because that the blue-shift effect of PL peak energy occurs during 55~84K
the luminescence is dominated by L band at 300K and it is easier for the carriers to get energy to transfer under higher temperature.