A Regularized Analytic Extension on the Upper Half Plane
碩士 === 國立清華大學 === 數學系 === 104 === In electromagnetism, the electric displacement field D represents how an electric field E affects in a given medium. The actual permittivity ε is calculated by =ε_r ε_0=(1+χ)ε_0 , where χ is the electric susceptibility of given material. The electric susceptibility...
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ndltd-TW-104NTHU54790022017-07-30T04:40:50Z http://ndltd.ncl.edu.tw/handle/52150744941839789853 A Regularized Analytic Extension on the Upper Half Plane 上半平面的規範化解析延拓 Luo, Yen Po 羅彥博 碩士 國立清華大學 數學系 104 In electromagnetism, the electric displacement field D represents how an electric field E affects in a given medium. The actual permittivity ε is calculated by =ε_r ε_0=(1+χ)ε_0 , where χ is the electric susceptibility of given material. The electric susceptibility χ satisfies the Kramers-Krönig relation. From the wave equation, electric susceptibility χ , the refractive index n and attenuation coefficient q have the relation χ=〖(n+iq)〗^2. However we can only measure n and q within a finite bandwidth. In this paper, we will find out a subset of the kernel of the Kramer-Krönig relation, and then use a minimization with a regularized extension to recover χ outside the measured bandwidth. We will recover the data of silicon and silver. For silver, we observe the singularity of its data χ_s and apply the KK-relation on χ-χ_(s ). For the singularity of conductors, we put the detail in the section 1.3. Wang, Wei Cheng 王偉成 2016 學位論文 ; thesis 51 en_US |
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碩士 === 國立清華大學 === 數學系 === 104 === In electromagnetism, the electric displacement field D represents how an electric field E affects in a given medium. The actual permittivity ε is calculated by =ε_r ε_0=(1+χ)ε_0 , where χ is the electric susceptibility of given material. The electric susceptibility χ satisfies the Kramers-Krönig relation. From the wave equation, electric susceptibility χ , the refractive index n and attenuation coefficient q have the relation χ=〖(n+iq)〗^2. However we can only measure n and q within a finite bandwidth. In this paper, we will find out a subset of the kernel of the Kramer-Krönig relation, and then use a minimization with a regularized extension to recover χ outside the measured bandwidth. We will recover the data of silicon and silver. For silver, we observe the singularity of its data χ_s and apply the KK-relation on χ-χ_(s ). For the singularity of conductors, we put the detail in the section 1.3.
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author2 |
Wang, Wei Cheng |
author_facet |
Wang, Wei Cheng Luo, Yen Po 羅彥博 |
author |
Luo, Yen Po 羅彥博 |
spellingShingle |
Luo, Yen Po 羅彥博 A Regularized Analytic Extension on the Upper Half Plane |
author_sort |
Luo, Yen Po |
title |
A Regularized Analytic Extension on the Upper Half Plane |
title_short |
A Regularized Analytic Extension on the Upper Half Plane |
title_full |
A Regularized Analytic Extension on the Upper Half Plane |
title_fullStr |
A Regularized Analytic Extension on the Upper Half Plane |
title_full_unstemmed |
A Regularized Analytic Extension on the Upper Half Plane |
title_sort |
regularized analytic extension on the upper half plane |
publishDate |
2016 |
url |
http://ndltd.ncl.edu.tw/handle/52150744941839789853 |
work_keys_str_mv |
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