Formulation and Calculation of spontaneous Emission Rate and Coupling Factor in Microcavity Structures
碩士 === 國立交通大學 === 電子物理學系 === 82 === In this thesis, we study spontaneous emission in slab and cylindrical dielectric waveguides and the coupling factor in micro-cavity, including surface emitting lasers, micro -disk and micro-ring lasers, b...
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ndltd-TW-082NCTU04290132016-07-18T04:09:35Z http://ndltd.ncl.edu.tw/handle/80814928955596356805 Formulation and Calculation of spontaneous Emission Rate and Coupling Factor in Microcavity Structures 微共振腔結構中自發放射速率及耦合係數之理論與計算 Jang Wang 王蕙貞 碩士 國立交通大學 電子物理學系 82 In this thesis, we study spontaneous emission in slab and cylindrical dielectric waveguides and the coupling factor in micro-cavity, including surface emitting lasers, micro -disk and micro-ring lasers, by numerical simulations. Strong dependence of spontaneous emission rate on the dipole orientation was found. In planar waveguides, the emission for vertical dipoles was essentially inhibited, while the emission for horizontal dipoles falls into the lowest TE mode when thickness of the waveguide is a fraction of optical wavelength. Total spontaneous emission rates are obtained by adding the contribution from waveguide modes and radiation modes. Spontaneous emission factor β, defined as the fraction of total spontaneous emission into the waveguide or laser mode, was also found to depend strongly on the dimension of the structures. For proton-implanted GaAs surface emitting lasers incorporating AlGaAs/AlAs distributed Bragg reflectors, β is 1.85E-3. For micro-ring,β is as large as 0.925. As for micro- disk lasers,the disk diameter is 1 ∼5μm,when β is 0.1∼0.25 . Dr.Kuochou Tai 戴國仇 1994 學位論文 ; thesis 89 zh-TW |
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碩士 === 國立交通大學 === 電子物理學系 === 82 === In this thesis, we study spontaneous emission in slab and
cylindrical dielectric waveguides and the coupling factor in
micro-cavity, including surface emitting lasers, micro -disk
and micro-ring lasers, by numerical simulations. Strong
dependence of spontaneous emission rate on the dipole
orientation was found. In planar waveguides, the emission for
vertical dipoles was essentially inhibited, while the emission
for horizontal dipoles falls into the lowest TE mode when
thickness of the waveguide is a fraction of optical wavelength.
Total spontaneous emission rates are obtained by adding the
contribution from waveguide modes and radiation modes.
Spontaneous emission factor β, defined as the fraction of
total spontaneous emission into the waveguide or laser mode,
was also found to depend strongly on the dimension of the
structures. For proton-implanted GaAs surface emitting lasers
incorporating AlGaAs/AlAs distributed Bragg reflectors, β is
1.85E-3. For micro-ring,β is as large as 0.925. As for micro-
disk lasers,the disk diameter is 1 ∼5μm,when β is 0.1∼0.25 .
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author2 |
Dr.Kuochou Tai |
author_facet |
Dr.Kuochou Tai Jang Wang 王蕙貞 |
author |
Jang Wang 王蕙貞 |
spellingShingle |
Jang Wang 王蕙貞 Formulation and Calculation of spontaneous Emission Rate and Coupling Factor in Microcavity Structures |
author_sort |
Jang Wang |
title |
Formulation and Calculation of spontaneous Emission Rate and Coupling Factor in Microcavity Structures |
title_short |
Formulation and Calculation of spontaneous Emission Rate and Coupling Factor in Microcavity Structures |
title_full |
Formulation and Calculation of spontaneous Emission Rate and Coupling Factor in Microcavity Structures |
title_fullStr |
Formulation and Calculation of spontaneous Emission Rate and Coupling Factor in Microcavity Structures |
title_full_unstemmed |
Formulation and Calculation of spontaneous Emission Rate and Coupling Factor in Microcavity Structures |
title_sort |
formulation and calculation of spontaneous emission rate and coupling factor in microcavity structures |
publishDate |
1994 |
url |
http://ndltd.ncl.edu.tw/handle/80814928955596356805 |
work_keys_str_mv |
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