研究生: |
邱政傑 Cheng-Chieh Chiu |
---|---|
論文名稱: |
沉積氮化鈦島狀結構應用於 表面拉曼散射基材 Dense Titanium Nitride Islands Coating for Surface-Enhanced Raman Scattering Substrates |
指導教授: |
周賢鎧
Shyankay Jou |
口試委員: |
郭鴻飛
Hungfei Kuo 蔡豐羽 none |
學位類別: |
碩士 Master |
系所名稱: |
工程學院 - 材料科學與工程系 Department of Materials Science and Engineering |
論文出版年: | 2014 |
畢業學年度: | 102 |
語文別: | 中文 |
論文頁數: | 156 |
中文關鍵詞: | 表面拉曼散射 、拉曼光譜 、氮化鈦 、密集島狀結構 |
外文關鍵詞: | surface-enhanced Raman scattering, Raman spectroscopy, titanium nitride, dense arrays of islands |
相關次數: | 點閱:259 下載:8 |
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本論文研究密集堆積氮化鈦(TiN)不連續薄膜結構應用於表面拉曼散射基材,利用脈衝射頻磁控濺鍍方式製備氮化鈦島狀結構於石英玻璃基材上,探討氮化鈦島狀結構對消光光譜之消光波長及拉曼散射光譜影響。
我們利用脈衝射頻磁控濺鍍通入工作氣體氬氣(Ar)與氮氣(N2)比例為30 : 3.5,工作壓力為3.99 Pa (3×10–2 torr),基板溫度為200 oC及基板旋轉速率8 #/min下,沈積密集氮化鈦島狀結構於石英玻璃基材(10 × 10 × 0.5 mm3),並藉由改變總鍍膜時間(Ttotal)、脈衝頻率(Pulse Frequency)、工作比例(Duty ratio)等條件,控制氮化鈦島狀結構得到有極佳拉曼散射增強基材。當使用脈衝射頻功率80W、脈衝頻率為1000 Hz、工作比例60%、總鍍膜時間15 min,得到最佳的氮化鈦島狀結構之拉曼散射基材。此氮化鈦島狀結構之拉曼散射基材顆粒大小為13.4 ± 1.0 nm、相鄰間距為 1.5 ± 0.3 nm,消光光光譜最大消光波長位置為497 nm。另外將此氮化鈦島狀結構之拉曼散射基材固定受測分子R6G (濃度10-5 M),受雷射光波長532 nm照射的拉曼散射訊號,與固定受測分子R6G (濃度10-3 M)於石英玻璃基材受雷射光波長532 nm激發的拉曼散射訊號作為基準,透過公式計算出拉曼散射光譜訊號增幅比值(Enhancement Factor, EF)大於104。
最後為了解TiN島狀結構之SERS基材的拉曼散射光譜增強訊號均勻度,故利用20× 20× 0.5 mm3石英玻璃試片選取16個不同位置做拉曼光譜分析,以拉曼光譜訊號為779 cm-1做討論,其平均拉曼散射光譜訊號增強比值為43912,標準差為6972。
This thesis studied surface-enhanced Raman scattering (SERS) substrates consisting dense arrays of titanium nitride (TiN) islands. We prepared TiN coatings on a quartz glass of 10 × 10 × 0.5 mm3 by RF magnetron sputter deposition and investigated their of extinction spectra and Raman scattering spectra.
We deposited dense TiN islands using pulse RF magnetron sputter on 200 oC quartz substrate under flowing of Ar and N2 (gas ratio of 30:3.5), working pressure of 3.99 Pa (3×10–2 torr) and substrate rotation speed of 8 #/min. Controlling total sputtering time (Ttotal), pulse frequency and duty ratio could lead to nanostructure TiN islands with enhanced Raman scattering character. The experiments proved that using RF power of 80 W, pulse frequency of 1000 Hz, duty ratio of 60 % and total sputtering time of 15 min resulted in the TiN islands with better Raman scattering performance. The average sizes of the TiN islands were 13.4 ± 1.0 nm and the spacing between TiN islands was around 1.5 ± 0.3 nm. The TiN islands thin film had an extinction peak at around 497 nm, which related to surface plasmon resonance. By comparing Raman scattering intensity of the TiN islands substrate absorbed with 10-5 M rhodamine 6G (R6G) solution and that of 10-3 M R6G-absorbed reference substrate using 532 nm laser, an enhancement factor (EF) greater than 104 was obtained.
In order to understand the uniformity of the TiN islands, Raman scattering spectrum was recorded from 16 different positions on a 20 × 20 × 0.5 mm3 Raman substrate. Raman scattering signal of 779 cm-1 peaks had an average EF of 43912 and standard deviation of 6972.
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