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完整後設資料紀錄
DC 欄位 | 值 | 語言 |
---|---|---|
dc.contributor.advisor | 郭茂坤 | |
dc.contributor.author | Bae-Renn Chen | en |
dc.contributor.author | 陳柏任 | zh_TW |
dc.date.accessioned | 2021-06-16T16:12:04Z | - |
dc.date.available | 2015-03-15 | |
dc.date.copyright | 2013-03-15 | |
dc.date.issued | 2013 | |
dc.date.submitted | 2013-02-18 | |
dc.identifier.citation | [1] R. M. Stockle, Y. D. Suh, V. Deckert, and R. Zenobi, “Nanoscale chemical analysis by tip-enhanced Raman spectroscopy,” Chem. Phys. Lett. 318, 131-136, 2000.
[2] S. S. Chang, and C. R. C. Wang, “The synthesis and absorption spectra of sev¬eral metal nanoparticle systems,” Chem. 56, 209-222, 1998. [3] H. Xu, E. J. Bjerneld, and M. Kall, “Spectroscopy of single hemoglobin molecule by surface-enhanced Raman scattering,” Phys. Rev. Lett. 22, 4357-4360, 1999. [4] J. J. Mock, M. Barbic, D. R. Smith, D. A. Schultz, and S. Schultz, “Shape effects in plasmon resonance of individual colloidal silver nanoparticles,” J. Chem. Phys. 116, 6755-6759, 2002. [5] E. Dvjardin, L. B. Hsin, C. R. C. Wang, and S. Mann, “DNA-driven self-assembly of gold nanorods,” Chem. Comm. 14, 1264-1265, 2001. [6] Xiong-Rui Su, Wei Zhang, Li Zhou, Xiao-Niu Peng, Qu-Quan Wang, “Plasmon-enhanced Forster energy transfer between semiconductor quantum dots: multipole effects,” OPT. 18 (7), 6516-6521, 2010. [7] Jiunn-Woei Liaw, Chuan-Li Liu, Wei-Min Tu, Chieh-Sheng Sun, and Mao-Kuen Kuo, “Average enhancement factor of molecules-doped coreshell (Ag@SiO2) on fluorescence” OPT. 18.(12), 12788-12797, 2010. [8] Jiunn-Woei Liaw & Chuan-Li Liu & Mao-Kuen Kuo, “Dual-Band Plasmonic Enhancement of Ag-NS@SiO2 on Gain Medium’s Spontaneous Emission” Plasmonics, 6, 673–680, 2011. [9] Manuela Lunz, Valerie A. Gerard, Yurii K. Gun’ko, Vladimir Lesnyak, Nikolai Gaponik, Andrei S. Susha, Andrey L. Rogach, A. Louise Bradley, “Surface Plasmon Enhanced Energy Transfer between Donor and Acceptor CdTe Nanocrystal Quantum Dot Monolayers,” Nano Lett. 11, 3341–3345, 2011 [10] Ki-Se Kim, Jeong-Hee Kim, Hun Kim, Frede ric Laquai, Eric Arifin, Jin-Kyu Lee, Seong I Yoo, Byeong-Hyeok Sohn, “Switching Off FRET in the Hybrid Assemblies of Diblock Copolymer Micelles, Quantum Dots, and Dyes by Plasmonic Nanoparticles,” ACS nano. 6 (6), 5051-5059, 2012. [11] Lei Zhao, Tian Ming, Lei Shao, Huanjun Chen, and Jianfang Wang, “Plasmon-Controlled Forster Resonance Energy Transfer,” J. Phys. Chem. C 116, 8287-8296, 2012. [12] J. J. Mock, D. R. Smith, and S. Schultz, “Local refractive index dependence of plasmon resonance spectra from individual nanoparticles,” Nano. Lett. 3, 485-491, 2003. [13] V.M. Agranovich, and D.L. Mills, Surface Polaritons Electromangeitc at Sur¬faces and Interfaces, North-Holland, New York, 1982. [14] R.H. Ritchie, “Plasma losses by fast electrons in thin films,” Phys. Rev. 106, 874, 1957. [15] V.M. Agranovich, and D.L. Mills, Surface Polaritons Electromangeitc at Sur¬faces and Interfaces, North-Holland, New York, 1982. [16] S. S. Chang, C. W. Shih, C. D. Chen, W. C. Lai, and C. R. Chris Wang, “The shape transition of gold nanorods,” Langmuir 15, 701-709, 1999. [17] Forster T., “Zwischenmolekulare Energiewanderung und Fluoreszenz,” Ann. Physik 437, 55, 1948. [18] Alexander O. Govorov, Jaebem Lee, and Nicolas A. Kotov, “Theory of plasmon-enhanced Forster energy transfer in optically excited semiconductor and metal nanoparticle,” Physics Review B 76, 125308, 2007. [19] Jian Zhang, Yi Fu, and Joseph R. Lakowicz, “Enhanced Forster Resonance Energy Transfer (FRET) on a Single Metal particle,” J. Phys. Chem. C 111, 50-56, 2007. [20] Jian Zhang, Yi Fu, and Joseph R. Lakowicz, “Enhanced Forster Resonance Energy Transfer (FRET) on a Single Metal particle. 2. Dependence on Donor-Acceptor Separation Distance, Particle Size, and Distance from Metal Surface,” J. Phys. Chem. C 111, 11784-11792, 2007 [21] H. Y. Xie , H. Y. Chung, P. T. Leung, and D. P. Tsai, “Plasmonic enhancement of Forster energy transfer between two molecules in the vicinity of a metallic nanoparticle: Nonlocal optical effects,” Physics Review B 80, 155448, 2009. [22] Tacakol Pakizeh and Mikael Kӓll, “Unidirectional Ultracompact Optical Nanoantennas,” Nano Lett., 9 (6) 2343-2349, 2009. [23] 孫聖傑,“三維奈米粒子於電磁場解析解研究”,國立臺灣大學應用力學研究所碩士論文, 2008 [24] 江崇煜,“金屬奈米殼之電漿子模態分析”,國立臺灣大學應用力學研究所碩士論文, 2011 [25] P. Nordlander and C. Oubre, “Plasmon Hybridization in Nanoparticle Dimers,” J. Biomed. Nano Lett., 4 (5), 899-903, 2004. [26] Jiunn-Woei Liaw, Jeng-Hong Chen, Chi-San Chen, and Mao-Kuen Kuo, “Purcell effect of nanoshell dimer on single molecule’s fluorescence,” Opt., 17 (16), 135329, 2009. [27] Jiunn-Woei Liaw, Chi-SanChen, Jeng-HongChen, “Enhancement or quenching effect of metallic nanodimer on spontaneous emission,” J. Quant. Spectrosc. Radiat. Transfer. 111, 454-465, 2010. [28] V. Faessler, C. Hrelescu, A.A. Lutich, L. Osinkina, S. Mayilo, F. Jackel, J. Feldmann, “Accelerating fluorescence resonance energy transfer with plasmonic nanoresonator,” Chem. Phys. Lett. 508, 67-70, 2011. [29] J. H. Weaver, and H. P. R. Frederikse, Optical Properties of Selected Elements, McGraw Hill, New York, 1972. [30] M. Liu, T. W. Lee, and S. K. Gray, “Optical properties of rodlike and bipyramidal gold nanoparticle from three-dimensional computations,” Phy. Rev. B 76, 235428, 2007. [31] C. F. Bohren, and D. R. Huffman, Absorption and Scattering of Light by Small Particles, Wiley, New York, 1983. [32] J. H. Weaver, and H. P. R. Frederikse, Optical Properties of Selected Elements, McGraw Hill, New York, 1972. [33] P. B. Johnson, and R. W. Christy, “Optical constants of the noble metals,” Phys. Rev. B 6, 4370-4379, 1972. [34] J. A. Stratton, Electromagnetic Theory, McGraw Hill, New York, 1941. [35] C. T. Tai, “Dyadic Green Functions in Electromagnetic Theory,” IEEE, New York, 1994 [36] C. Hafner, “Beitrage zur berechnung der ausbreitung electromagneitscher wellen in zylindrischen struckturen mit hilfe des point-matching ver fahrens,” Ph.D. disser¬tation, Swiss Polytechnical Institute of Technology, Zurich, Switzerland, 1980. [37] I. N. Vekua, New Methods for Solving Elliptic Equations, North-Holland, New York, 1993. [38] F. M. Kahnert, “Numerical methods in electromagnetic scattering theory,” J. Quant. Spectrosc. Radiat. Transfer. 79, 775-824, 2003. [39] N. Kuster, and R. Ballisti, “MMP method simulation of antenna with scattering object in the closer-near field,” IEEE. Trans. Magn. 26. 658-661, 1990. [40] C. Hafner, and N. Kuster, “Computation of electromagnetic fields by multiple multipole method (generalized multipole technique),” Radio. Sci. 26, 291-297, 1991. [41] C. Hafner, The Generalized Multipole Technique for Computational Electromaga-netics, Artech. House, Boston, 1991. [42] H. William, A. T. Saul, T. V. William, and F. P. Brian, Numerical Recipes C++: the Art of Scientific Computing, Cambridge University Press, New York, 2002. [43] 劉傳立,“含螢光分子之多層奈米粒子的平均螢光增益”,國立臺灣大學應用力學研究所碩士論文, 2010 [44] 蔡孝彥,“金奈米桿及偏心球殼結構之光學特性研究”,國立臺灣大學應用力學研究所碩士論文, 2011 [45] 黃駿惠,“奈米桿表面電漿電漿子共振模態分析”,國立臺灣大學應用力學研究所碩士論文, 2012 [46] S. J. Oldenburg, G. D. Hale, J. B. Jackson, and N. J. Halas, “Light scattering from dipole and quadrupole nanoshell antennas,” Appl. Phys. Lett. 75, 1063-1064, 1999. [47] Elefterios Lidorikis, “Modeling of enhanced absorption and Raman scattering caused by plasmonic nanoparticle near fields”, J. Quant. Spectrosc. Radiat. Transfer. 113, 2573-2584, 2012. [48] Anatoliy I. Dragan, Eric S. Bishop, Jose R., Casas-Finet Robert J., Strouse James McGivney, Mark A. Schenerman,Chris D. Geddes, “Distance Dependence of Metal-Enhanced Fluorescence”, J. Quant. Spectrosc. Radiat. Transfer. 113, 2573-2584, 2012. [49] 陳建宏,“研究單分子與金屬奈米粒子耦合結構下之螢光增益現象,” 國立臺灣大學應用力學研究所碩士論文, 2008. [50] 陳啟三,“金屬奈米結構對營光增益之研究,” 國立臺灣大學應用力學研究所碩士論文, 2009. [51] 李承諭,“金奈米桿結構之光學特性分析,” 國立臺灣大學應用力學研究所碩士論文, 2010. [52] J. W. Liaw, M. K. Kuo, and C.N. Liao, “Plasmon resonances of spherical and ellipsoidal nanoparticles,” J. of Electromagn. Waves and Appl. 19 (13), 1787-1794, 2005. [53] J. W. Liaw, S. W. Tsai, K. L. Chen, and F. Y. Hsu, “Single-photon and two-photon cellular imagings of gold nanorods and dye,” J. Nanosci. Nanotech. 10 (1), 467-473, 2010. [54] J. W. Liaw, C. S. Chen, and J. H. Chen, “Enhancement or quenching effect of metallic nanodimer on spontaneous emission,” J. Quant. Spectrosc. Radiat. Transfer. 111, 454-465, 2010. [55] Manuela Lunz, “Surface Plasmon Enhanced Energy Transfer between Donor and Acceptor CdTe Nanocrystal Quantum Dot Monolayers,” Nano. Lett. 11, 3341-3345, 2011. [56] Ki-Se Kim, “Switching Off FRET in the Hybrid Assemblies of Diblock Copolymer Micelles, Quantum Dots, and Dyes by Plasmonic Nanoparticles,” ACS Nano. 6 (6), 5051-5059, 2012. | |
dc.identifier.uri | http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/62840 | - |
dc.description.abstract | 本研究探討銀奈米殼、銀奈米桿等結構的電漿子共振模態所產生的各種光學特性。分析銀奈米結構之電漿子共振模態對於兩個螢光分子的螢光共振能量轉移(fluorescence resonance energy transfer, FRET)之能量轉移效率的影響,以及對螢光分子的螢光增強效益的影響。根據Maxwell電磁理論,我們分別以Mie理論以及並矢格林函數等解析解,分析單顆球型銀奈米殼受到不同頻率的平面波或電偶極波源作用下內外域的電磁場分佈,探討各個電漿子共振模態的近、遠場特性及對螢光共振能量轉移的影響。並且使用多重多極展開法計算複雜結構,討論銀奈米桿或雙顆銀奈米殼的電漿子共振特性,對分子的螢光增益及螢光共振能量轉移的影響。
計算結果顯示銀奈米殼或銀奈米桿結構透過特定的入射方向及電場極化方向可以激發於特定區域內的螢光分子,一旦螢光分子受到激發,其能量的轉移會與電漿子共振模態和量子效應有關。特別是對於銀奈米桿,在固定細長比的情況下,銀奈米桿的兩端愈尖者,愈能提供較強的能量轉移效率。 在雙顆銀奈米殼的研究中發現,相較於單顆銀奈米殼,雙顆銀奈米殼的耦合效應對於位於間隙中的螢光分子具有更大的螢光增強效應,且其第一個模態有著明顯的紅位移。 | zh_TW |
dc.description.abstract | In this thesis, we studied the interactions among fluorescent molecules, silver nanoshell (SNSs), and silver nanorods (SNRs). Analysis the surface plasmon resonance modes of silver nanostructures for fluorescence resonance energy transfer(FRET) of energy transfer rate of two fluorescent molecule, and enhancement factor of the fluorescent molecule.Based on Maxwell's equations, we obtained the the analytical solutions internal and external electromagnetic field in the metal ball nanoparticles by plane wave incident or electric dipole source analytic solution to explore various modes of electromagnetic fields near the nature of the far-fielduse of dyadic Green's function , Mie theory, and. the multiple-multipole (MMP) method was used to solve these problems, We studied the surface plasmon resonances (SPRs) of these nanoparticles irradiated by different incident plane waves with different polarizations.
The calculation results show that silver nanoshell structure can be excited through a specific incidence direction and the electric polarization of fluorescent molecules within a specific area, and once the fluorescent molecules are excited, the energy transfer with the resonant modes of the scattering body and quantum effects are closely related. The silver rods scatter, the longer longitudinal axis c, said silver nanorods more sharp, can provide a stronger radiation and non-radiation efficiency and energy transfer rate. In research of the silver nanoshells enhancement factor found that the efficiency of silver nanoshell dimer more strong than single,and first mode has obvious red shift. | en |
dc.description.provenance | Made available in DSpace on 2021-06-16T16:12:04Z (GMT). No. of bitstreams: 1 ntu-102-R99543042-1.pdf: 3633513 bytes, checksum: 8dcf77fcbffe74403666e04f100afcf6 (MD5) Previous issue date: 2013 | en |
dc.description.tableofcontents | 第一章 緒論............................................1
1.1 前言..............................................1 1.2 文獻回顧...........................................2 1.3 本文內容...........................................4 第二章 電磁理論.........................................6 2.1 Maxwell方程式與邊界條件.............................6 2.2 Helmholtz方程式與向量波函數.........................8 2.3平面波於奈米殼之散射.................................13 2.4電磁場基底函數.....................................16 2.5 散射截面積、吸收截面積、消光截面積、激發效率 ...........19 2.6 輻射功率、非輻射功率、量子效率、能量轉移效率、電場增益 ...21 第三章 解析解與多重中心展開法 ...........................23 3.1電偶極與球型奈米結構解析解...........................23 3.1.1電偶極波源..............................23 3.1.2電偶極波源之並矢格林函數..................24 3.2多重中心展開法....................................28 3.2.1 多重中心展開法的基本觀念.................28 3.2.2 奈米粒子的電磁場問題....................29 3.2.3 奇異值拆解法求解電磁場之未知係數..........33 第四章 數值結果與討論.................................39 4.1 銀奈米結構之電漿子共振模態輔助能量轉移................39 4.1.1單顆銀奈米殼(nanoshell).........................39 4.1.1.1 平面波激發.................................40 4.1.1.2 電偶極激發.................................40 4.1.1.3 能量轉移效率...............................41 4.1.2銀奈米桿.......................................48 4.1.2.1 平面波激發................................48 4.1.2.2 電偶極激發................................50 4.1.2.3 能量轉移效率..............................52 4.2 雙顆銀奈米殼(nanoshell dimer)的螢光增益...........76 4.2.1 平面波激發....................................76 4.2.2 電偶極激發....................................77 4.2.3 螢光增益效率 ..................................77 第五章 結論與未來展望.................................82 5.1 結論...........................................82 5.2 未來展望........................................84 附錄A平面波於核-殼球奈米結構之散射......................85 附錄B電偶極於核-殼球奈米結構外之散射.....................88 參考文獻............................................90 | |
dc.language.iso | zh-TW | |
dc.title | 銀奈米結構之電漿子共振模態對螢光共振能量轉移的影響 | zh_TW |
dc.title | Plasmonic Resonance Modes of Silver Nanostructures on Fluorescence Resonance Energy Transfer | en |
dc.type | Thesis | |
dc.date.schoolyear | 101-1 | |
dc.description.degree | 碩士 | |
dc.contributor.coadvisor | 廖駿偉 | |
dc.contributor.oralexamcommittee | 葉超雄,鄧崇任 | |
dc.subject.keyword | 銀奈米桿,銀奈米殼,FRET,表面電漿子共振,並矢格林函數,多重多極展開法,螢光分子,吸收截面積,散射截面積,激發效率,輻射功率,量子效率,能量轉移效率,電場增益, | zh_TW |
dc.subject.keyword | silver nanorods,silver nanoshell,Forster resonance energy transfer,surface plasmon resonance (SPR),dyadic Green’s functions,multiple-multipole (MMP),fluorescent molecule,absorption cross section,scattering cross section,excitation rate,quantum yield,energy transfer rate,enhancement factor, | en |
dc.relation.page | 95 | |
dc.rights.note | 有償授權 | |
dc.date.accepted | 2013-02-18 | |
dc.contributor.author-college | 工學院 | zh_TW |
dc.contributor.author-dept | 應用力學研究所 | zh_TW |
顯示於系所單位: | 應用力學研究所 |
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