Long-wavelength lasing from InAs self-assembled quantum dots on (311) B InP
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Nishi, K
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NEC Corp Ltd, Optoelect & High Frequency Device Res Labs, Tsukuba, Ibaraki 3058501, JapanNEC Corp Ltd, Optoelect & High Frequency Device Res Labs, Tsukuba, Ibaraki 3058501, Japan
Nishi, K
[1
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Yamada, M
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NEC Corp Ltd, Optoelect & High Frequency Device Res Labs, Tsukuba, Ibaraki 3058501, JapanNEC Corp Ltd, Optoelect & High Frequency Device Res Labs, Tsukuba, Ibaraki 3058501, Japan
Yamada, M
[1
]
Anan, T
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NEC Corp Ltd, Optoelect & High Frequency Device Res Labs, Tsukuba, Ibaraki 3058501, JapanNEC Corp Ltd, Optoelect & High Frequency Device Res Labs, Tsukuba, Ibaraki 3058501, Japan
Anan, T
[1
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Gomyo, A
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NEC Corp Ltd, Optoelect & High Frequency Device Res Labs, Tsukuba, Ibaraki 3058501, JapanNEC Corp Ltd, Optoelect & High Frequency Device Res Labs, Tsukuba, Ibaraki 3058501, Japan
Gomyo, A
[1
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Sugou, S
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NEC Corp Ltd, Optoelect & High Frequency Device Res Labs, Tsukuba, Ibaraki 3058501, JapanNEC Corp Ltd, Optoelect & High Frequency Device Res Labs, Tsukuba, Ibaraki 3058501, Japan
Sugou, S
[1
]
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[1] NEC Corp Ltd, Optoelect & High Frequency Device Res Labs, Tsukuba, Ibaraki 3058501, Japan
Nanometer-scale InAs quantum dots were grown on InP by self-assembly using gas-source molecular beam epitaxy. InAs depositions of 0.33 nm in nominal thickness were found to form quantum dots on (311) B InP with a lateral dimension of about 43 nm and a density of 2 x 10(10) cm(-2). A laser structure with seven periods of the quantum dot active layers lased in a wavelength range from 1.1 to 1.4 mu m at 77 K under pulse current injection. The lasing wavelength, changed to a shorter wavelength as the cavity length decreased, indicating gain saturation due to state filling effect in discrete quantum levels, which is typical in quantum dot lasers. This phenomenon can be used to achieve wide-range multiwavelength lasers for optical communication, that can be adjusted merely by changing the effective cavity length. (C) 1998 American Institute of Physics.