跳到主要內容

臺灣博碩士論文加值系統

(216.73.217.86) 您好!臺灣時間:2026/11/01 10:27
字體大小: 字級放大   字級縮小   預設字形  
回查詢結果 :::

詳目顯示

: 
twitterline
研究生:徐子晴
研究生(外文):Tzu-Ching Shu
論文名稱:奈米銀陣列的表面增強拉曼特性研究:分子濃度與表面電漿共振的影響
論文名稱(外文):The Research of Silver Nanoparticle Array for Surface-Enhanced Raman Spectroscopy : The Effect of Molecular Concentration and Surface Plasmon Resonance
指導教授:曾賢德
指導教授(外文):Shien-Der Tzeng
口試委員:江海邦、賴建智
口試委員(外文):Hai-Pang Chiang、Chien-Chih Lai
口試日期:2018-07-23
學位類別:碩士
校院名稱:國立東華大學
系所名稱:物理學系
學門:自然科學學門
學類:物理學類
論文種類:學術論文
論文出版年:2018
畢業學年度:106
語文別:中文
論文頁數:80
中文關鍵詞:銀奈米粒子、表面增強拉曼散射、表面電漿共振
外文關鍵詞:Silver Nanoparticle、Surface-Enhanced Raman Spectroscopy、Surface Plasmon Resonance
相關次數:
  • 被引用被引用:0
  • 點閱點閱:407
  • 評分評分:
  • 下載下載:11
  • 收藏至我的研究室書目清單書目收藏:0
表面增強拉曼散射(Surface Enhanced Raman Scattering , SERS)主要的增強機制有化學增強機制和電場增強機制。兩個金屬的奈米粒子之間的距離很接近時會產生耦合的作用,粒子中間間隙的地方會有電場增強,稱為熱點。本實驗使用化學還原合成法製備銀奈米粒子溶液,再將銀奈米粒子表面修飾8-mercapto-octanoic acid (MOA)分子,最後使用離心法將修飾過的銀奈米粒子排列成固定間距的陣列。分別使用浸泡或滴乾的方法,讓待測分子Rhodamine 6G (R6G)在樣品上吸附,待測分子會進入銀奈米粒子陣列中的間隙,使分子SERS訊號增強。檢測不同濃度的R6G分子在銀奈米陣列上的SERS訊號強度,發現強度並非隨著濃度提升而持續增強。當R6G密度低於1⤫10^3 (分子個數/ μm^2)時,SERS強度和濃度會呈正相關,推測是位於熱點的R6G分子數量隨密度增加。當R6G密度在高於1⤫10^3 (分子個數/ μm^2)時,SERS強度反而隨密度上升而些微下降。推測是由於表面吸附的R6G分子密度高而造成分子重疊,讓其SERS訊號降低。上述實驗我們以兩種不同波長的拉曼激發光源做量測,量測出來的SERS強度會整體改變,但趨勢變化相似。先前的模擬結果發現,不同激發光波長會影響銀奈米粒子間電場增強的程度。因此SERS訊號隨密度的變化或許可以由熱點的電場增強程度與範圍來解釋。
The main enhancement mechanism of Surface Enhanced Raman Scattering (SERS) is chemical strengthening mechanism and electric field enhancement mechanism. When two metal nanoparticles get very close, they will couple each other. There will be an electric field enhancement between two particles, called a hot spot. In this experiment, the silver nanoparticle solution were prepared by chemical reduction method. After that, the silver nanoparticles were surface-modified with 8-mercapto-octanoic acid (MOA) molecules. Finally, the modified silver nanoparticles were arranged into a fixed-pitch array by centrifugation. Using the method of immersion and titration, the Rhodamine (R6G) molecule is adsorbed on the sample. The R6G molecule enters the gap between the nanoparticles and enhances the SERS signal. The SERS signal intensity of different density of R6G molecules on the silver nanoparticles array was measured. We found that the SERS signal intensity did not increase continuously with the increase of R6G concentration. When the R6G density is lower than 1⤫10^3 (molecule/ μm^2), the SERS signal intensity and concentration will be positive correlation. We assumed that the number of R6G molecules distributed near the hot spots increase as the concentration increase. When the concentration of R6G is higher than 1⤫10^3 (molecule/ μm^2). Instead, the SERS signal slightly decrease with the increase of R6G density. We suppose that high R6G molecule density lead to R6G molecules overlapping. As a result, the SERS signal will be decreased. In the above experiments, we use the Raman excitation light of two different wavelengths as the light source. The measured SERS signal intensity will change overall. However, it will not affect variation trend of the R6G density and the SERS signal intensity. Previous simulation have shown that Raman excitation light of different wavelengths affect the degree of electric field enhancement between silver nanoparticles. Therefore, the variation of the SERS signal with density may be explained by the degree and extent of electric field enhancement of the hot spot.
第一章 緒論 1
第二章 研究原理 9
第三章 研究方法 21
第四章 研究結果與討論 45
第五章 結論 73
文獻參考 75
[1] C. V. Raman, “A new radiation,” Indian J. Phys. 2, 387–398(1928)
[2] C. V. Raman and K. S. Krishnan, “A New Type of Secondary Radiation,” Nature, 121,501-502 (1928)
[3] R. L. McCreery, “Raman Spectroscopy for Chemical Analysis,” Chemical Analysis, 157, Wuley Inter-Science.
[4] M.Fleischmann, P.J.Hendra, A.J.McQuillan, “Raman spectra of pyridine adsorbed at a silver electrode,” Chem. Phys. Lett., 26, 2, 163 (1974)
[5] D. L.Jeanmaire, Richard P.Van Duyne, “ Surface raman spectroelectrochemistry: Part I. Heterocyclic, aromatic, and aliphatic amines adsorbed on the anodized silver electrode,” Journal of Electroanalytical Chemistry and Interfacial Electrochemistry, 84, 1-120 (1977)
[6] M. Grant Albrecht, J. Alan Creighton, “Anomalously intense Raman spectra of pyridine at a silver electrode,” J. Am. Chem. Soc., 99, 15, 5215–5217 (1977)
[7] A. Otto, “On the significance of Shalaev’s ‘hot spots’ in ensemble and single-molecule SERS by adsorbates on metallic films at the percolation threshold,” J. Raman Spectrosc., 37, 937–947 (2006)
[8] D. J. Bergman, D. Stroud. “Physical Properties of Macroscopically Inhomogeneous Media,” Solid-State Physics, 46, 147-269. (1992)
[9] D. P. Tsai, J. Kovacs, Zhouhang Wang, Martin Moskovits, Vladimir M. Shalaev, J. S. Suh, R. Botet, “Photon scanning tunneling microscopy images of optical excitations of fractal metal colloid clusters,” Phys. Rev. Lett., 72, (1994)
[10] Vladimir M.Shalaev, “Electromagnetic properties of small-particle composites,” Physics Reports, 272, 2–3, 61-137 (1996)
[11] S. Grésillon, L. Aigouy, A. C. Boccara, J. C. Rivoal, X. Quelin, C. Desmarest, P. Gadenne, V. A. Shubin, A. K. Sarychev, V. M. Shalaev, “Experimental Observation of Localized Optical Excitations in Random Metal-Dielectric Films,” Phys. Rev. Lett., 82, 4520 (1999)
[12] Mark I. Stockman, Sergey V. Faleev, David J. Bergman, “Localization versus Delocalization of Surface Plasmons in Nanosystems: Can One State Have Both Characteristics?,” Phys. Rev. Lett., 87, 167, 401 (2001)
[13] V. M. Shalaev, “Optical Properties of Nanostructured Random Media,” Topics in Applied Physics, 82, Springer.
[14] D. J. Bergman, M. I. Stockman, “Surface Plasmon Amplification by Stimulated Emission of Radiation: Quantum Generation of Coherent Surface Plasmons in Nanosystems,” Phys. Rev. Lett., 90, 027, 402 (2003)
[15] F. Brouers, S. Blacher, A. N. Lagarkov, A. K. Sarychev, P. Gadenne, V. M. Shalaev, “Theory of giant Raman scattering from semicontinuous metal films,” Phys. Rev. B, 55, 132, 34 (1997)
[16] Nie S, Emory SR, “Probing Single Molecules and Single Nanoparticles by Surface-Enhanced Raman Scattering,” Science. 275, 1102 (1997)
[17] K. Bosnick, M. Maillard, L. Brus, “Single Molecule Raman Spectroscopy at the Junctions of Large Ag Nanocrystals,” J. Phys. Chem. B, 107, 37, 9964–9972 (2003)
[18] Hongxing Xu, Mikael Käll Prof, “Polarization‐Dependent Surface‐Enhanced Raman Spectroscopy of Isolated Silver Nanoaggregates,” Chemphyschem, 4, 1001 (2003)
[19] A. Otto ,Indian J. Phys. Part B, 77B: 63.(2003)
[20] K. Kneipp, M. Moskovits, H. Kneipp, “Surface-Enhanced Raman Scattering: Physics and Applications,” Springer.
[21] P. G. Etchegoin, E. C. Le Ru, “A perspective on single molecule SERS: current status and future challenges,” Phys. Chem. Chem. Phys., 10, 6079-6089 (2008)
[22] E. C. Le Ru, E. Blackie, M. Meyer, P. G. Etchegoin, “Surface Enhanced Raman Scattering Enhancement Factors: A Comprehensive Study,” J. Phys. Chem. C, 111, 13794-13803 (2007)
[23] B.N.J.Persson, “Surface resistivity: theory and applications,” Surface Science, 269–270, 103-112 (1992)
[24] Yujin Wang, Hailong Chen, Mengtao Sun, Zehan Yao, Baogang Quan, Zhe Liu, Yuxiang Weng, Jimin Zhao, Changzhi Gu, Junjie Li, “Ultrafast carrier transfer evidencing graphene electromagnetically enhanced ultrasensitive SERS in graphene/Ag-nanoparticles hybrid,” Carbon, 122, 98-105 (2017)
[25] Chonghui Li, Chao Zhang, Shicai Xu, Yanyan Huo, Shouzhen Jiang,Cheng Yang, Zhen Li, Xiaofei Zhaoa, Suzhen Zhang, Baoyuan Man, “Experimental and theoretical investigation for a hierarchical SERSactivated platform with 3D dense hot spots,” Sensors and Actuators B, 263, 408–416 (2018)
[26] Jun Wang, Liqing Huang, Lipeng Zhai, Lin Yuan, Lihua Zhao, Weiwei Zhang, Dongzhi Shan, Aiwen Hao, Xuehong Feng, Jian Zhu, “Hot spots engineering in hierarchical silver nanocap array for surface-enhanced Raman scattering,” Applied Surface Science, 261, 605– 609 (2012)
[27] Joel I. Gersten, “The effect of surface roughness on surface enhanced Raman scattering,” J. Chem. Phys., 72, 5779 (1980)
[28] Joel I. Gersten, “Rayleigh, Mie, and Raman scattering by molecules adsorbed on rough surfaces,” J. Chem. Phys., 72, 5780 (1980)
[29] M. Kerker, “Resonances in electromagnetic scattering by objects with negative absorption,” Appl. Opt., 18, 1180 (1979)
[30] M. Kerker, O. Siiman, D. S. Wang, “Effect of aggregates on extinction and surface-enhanced Raman scattering spectra of colloidal silver,” J. Phys. Chem., 88, 3168 (1984)
[31] K. Kneipp, H. Kneipp, I. Itzkan, R. R. Dasari, M. S. Feld, “Surface-enhanced Raman scattering and biophysics,” J. Phys., 14, R597–R624 (2002)
[32] J. B. Jackson, N. J. Halas, “Silver Nanoshells:  Variations in Morphologies and Optical Properties,” J. Phys. Chem. B, 105, 2743 (2001)
[33] A. Otto, I. Mrozek, H Grabhorn, W. Akemann, “Surface-enhanced Raman scattering,” J. Phys., 4, 1143 (1992)
[34] A.Campion, P. Kambhampati, “Surface-enhanced Raman scattering,” Chem. Soc. Rev., 27 241 (1998)
[35] J. D. Jiang, E. Burstein, H. Kobayashi, “Resonant Raman Scattering by Crystal-Violet Molecules Adsorbed on a Smooth Gold Surface: Evidence for a Charge-Transfer Excitation,” Phys. Rev. Lett., 57, 1793 (1986)
[36] Juan F. Arenas, Juan Soto, Isabel López Tocón, David J. Fernández, Juan C. Otero, and Juan I. Marcos, “The role of charge-transfer states of the metal-adsorbate complex in surface-enhanced Raman scattering,” J. Chem. Phys., 112 7669 (2000)
[37] V. P. Drachev, S. V. Perminov, S. G. Rautian, V. P. Safonov, “Nonlinear Optical Effects and Selective Photomodification of Colloidal Silver Aggregates,” Optical Properties of Nanostructured Random Media,113–147 (2002)

[38] Otto A, “Surface-enhanced Raman scattering: ‘classical’ and ‘chemical’ origins Light Scattering in Solids IV. Electronic Scattering, Spin Effects, SERS and Morphic Effects edMCardona and G Guntherodt,” Berlin: Springer, 289 (1984)
[39] M. Kerker, D.-S. Wang, and H. Chew, “Surface enhanced Raman scattering (SERS) by molecules adsorbed at spherical particles,” Appl. Opt., 19, 4159 (1980)
[40] 吳民耀、劉威志,表面電漿子理論與模擬,物理雙月刊。廿八卷二期,486頁,2006年。
[41] 邱國斌、蔡定平,金屬表面電漿簡介,物理雙月刊。廿八卷二期,472頁,2006年。
[42] 郭清癸、黃俊傑、牟中原,金屬奈米粒子的製造,物理雙月刊。23卷6期,2001年。
[43] Jan W. Slot, Hans J. Geuze, “A new method of preparing gold probes for multiple-labeling cytochemistry,” European Journal of Cell Biology, 38, 87-93 (1985)
[44] 楊素卿,利用離心法製作奈米金顆粒薄膜探討其形成與顆粒間交互作用的關係。國立東華大學碩士論文,2010年。
[45] A. J. Bain, P. Chandna, G. Butcher, J. Bryant, “Picosecond polarized fluorescence studies of anisotropic fluid media. II.Experimental studies of molecular order and motion in jet aligned rhodamine 6G and resorufin solutions,” J. Phys. Chem., 112, 23 (2000)
[46] 羅聖全,科學基礎研究之重要利器 - 掃描式電子顯微鏡,科學研習月刊。第52卷第5期,2013年。
[47] P. Hildebrandt, M. Stockburger, “Surface-Enhanced Resonance Raman Spectroscopy of Rhodamine 6G Adsorbed on Colloidal Silver,” J. Phys. Chem., 88, 5935-5944 (1984)
連結至畢業學校之論文網頁點我開啟連結
註: 此連結為研究生畢業學校所提供,不一定有電子全文可供下載,若連結有誤,請點選上方之〝勘誤回報〞功能,我們會盡快修正,謝謝!
QRCODE
 
 
 
 
 
                                                                                                                                                                                                                                                                                                                                                                                                               
第一頁 上一頁 下一頁 最後一頁 top
無相關期刊