TY - JOUR
T1 - Quantum-confined stark effect in an AlGaN/GaN/AlGaN single quantum well structure
AU - Deguchi, Takahiro
AU - Sekiguchi, Kaoru
AU - Nakamura, Atsushi
AU - Sota, Takayuki
AU - Matsuo, Ryuji
AU - Chichibu, Shigefusa
AU - Nakamura, Shuji
PY - 1999/8
Y1 - 1999/8
N2 - Excitonic absorption was observed in a transmittance spectrum of AlGaN/GaN/AlGaN single quantum well structure with a well width of 5 nm at room temperature. The total internal electric field strength in the well was about 0.73 MV/cm, which was estimated from the absorption peak position based on a simple calculation, neglecting excitons. The observation is clearly due to the quantum-confined Stark effect. While excitonic absorption was clearly observed even in such a high internal field, no light emission was detected under a He-Cd laser excitation at temperatures ranging from room temperature to T = 10 K. Light emission accompanied by a blue shift of the emission peak and an increase of emission intensity was observed under higher excitation power density. The obvious conclusion in the present case is that the presence of a high internal electric field in the well is a disadvantage for light emission.
AB - Excitonic absorption was observed in a transmittance spectrum of AlGaN/GaN/AlGaN single quantum well structure with a well width of 5 nm at room temperature. The total internal electric field strength in the well was about 0.73 MV/cm, which was estimated from the absorption peak position based on a simple calculation, neglecting excitons. The observation is clearly due to the quantum-confined Stark effect. While excitonic absorption was clearly observed even in such a high internal field, no light emission was detected under a He-Cd laser excitation at temperatures ranging from room temperature to T = 10 K. Light emission accompanied by a blue shift of the emission peak and an increase of emission intensity was observed under higher excitation power density. The obvious conclusion in the present case is that the presence of a high internal electric field in the well is a disadvantage for light emission.
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U2 - 10.1143/jjap.38.l914
DO - 10.1143/jjap.38.l914
M3 - Article
AN - SCOPUS:0033175440
SN - 0021-4922
VL - 38
SP - L914-L916
JO - Japanese Journal of Applied Physics, Part 2: Letters
JF - Japanese Journal of Applied Physics, Part 2: Letters
IS - 8 B
ER -