The spontaneous emission factor in the rate equation of the injection laser is derived with help of the classical electromagnetic theory. The spontaneous emission is treated as the radiations from dipoles located in the active region. The value of the spontaneous emission factor given theoretically is in good agreement with the measured results. The magnitude of the spontaneous emission factor is inversely proportional to the volume of the active region and the spectral width of the spontaneous emission, and is proportional to the energy confinement factor and the fourth power of the wavelength. The possibility of the suppression of the relaxation oscillation by reducing the volume of the active region is predicted theoretically.
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Yasuharu SUEMATSU, Kazuhito FURUYA, "Theoretical Spontaneous Emission Factor of Injection Lasers" in IEICE TRANSACTIONS on transactions,
vol. E60-E, no. 9, pp. 467-472, September 1977, doi: .
Abstract: The spontaneous emission factor in the rate equation of the injection laser is derived with help of the classical electromagnetic theory. The spontaneous emission is treated as the radiations from dipoles located in the active region. The value of the spontaneous emission factor given theoretically is in good agreement with the measured results. The magnitude of the spontaneous emission factor is inversely proportional to the volume of the active region and the spectral width of the spontaneous emission, and is proportional to the energy confinement factor and the fourth power of the wavelength. The possibility of the suppression of the relaxation oscillation by reducing the volume of the active region is predicted theoretically.
URL: https://global.ieice.org/en_transactions/transactions/10.1587/e60-e_9_467/_p
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@ARTICLE{e60-e_9_467,
author={Yasuharu SUEMATSU, Kazuhito FURUYA, },
journal={IEICE TRANSACTIONS on transactions},
title={Theoretical Spontaneous Emission Factor of Injection Lasers},
year={1977},
volume={E60-E},
number={9},
pages={467-472},
abstract={The spontaneous emission factor in the rate equation of the injection laser is derived with help of the classical electromagnetic theory. The spontaneous emission is treated as the radiations from dipoles located in the active region. The value of the spontaneous emission factor given theoretically is in good agreement with the measured results. The magnitude of the spontaneous emission factor is inversely proportional to the volume of the active region and the spectral width of the spontaneous emission, and is proportional to the energy confinement factor and the fourth power of the wavelength. The possibility of the suppression of the relaxation oscillation by reducing the volume of the active region is predicted theoretically.},
keywords={},
doi={},
ISSN={},
month={September},}
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TY - JOUR
TI - Theoretical Spontaneous Emission Factor of Injection Lasers
T2 - IEICE TRANSACTIONS on transactions
SP - 467
EP - 472
AU - Yasuharu SUEMATSU
AU - Kazuhito FURUYA
PY - 1977
DO -
JO - IEICE TRANSACTIONS on transactions
SN -
VL - E60-E
IS - 9
JA - IEICE TRANSACTIONS on transactions
Y1 - September 1977
AB - The spontaneous emission factor in the rate equation of the injection laser is derived with help of the classical electromagnetic theory. The spontaneous emission is treated as the radiations from dipoles located in the active region. The value of the spontaneous emission factor given theoretically is in good agreement with the measured results. The magnitude of the spontaneous emission factor is inversely proportional to the volume of the active region and the spectral width of the spontaneous emission, and is proportional to the energy confinement factor and the fourth power of the wavelength. The possibility of the suppression of the relaxation oscillation by reducing the volume of the active region is predicted theoretically.
ER -