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基於光纖端面之導模共振探頭的浸入式感測器 = = Dip-Type Se...

游致傑

基於光纖端面之導模共振探頭的浸入式感測器 = = Dip-Type Sensor Based on a Guided-Mode Resonance Probe at the Facet of an Optical Fiber /

Record Type:	Language materials, printed : Monograph/item
Title/Author:	基於光纖端面之導模共振探頭的浸入式感測器 =/ 游致傑.
Reminder of title:	Dip-Type Sensor Based on a Guided-Mode Resonance Probe at the Facet of an Optical Fiber /
remainder title:	Dip-Type Sensor Based on a Guided-Mode Resonance Probe at the Facet of an Optical Fiber.
Author:	游致傑
Published:	雲林縣 :國立虎尾科技大學 , : 民113.07.,
Description:	[7], 40面 :圖, 表 ; : 30公分.;
Notes:	指導教授: 廖重賓, 郭文凱.
Subject:	nanoimprinting. -
Online resource:	電子資源

基於光纖端面之導模共振探頭的浸入式感測器 = = Dip-Type Sensor Based on a Guided-Mode Resonance Probe at the Facet of an Optical Fiber /
游致傑

基於光纖端面之導模共振探頭的浸入式感測器 =Dip-Type Sensor Based on a Guided-Mode Resonance Probe at the Facet of an Optical Fiber /Dip-Type Sensor Based on a Guided-Mode Resonance Probe at the Facet of an Optical Fiber.游致傑. - 初版. - 雲林縣 :國立虎尾科技大學 ,民113.07. - [7], 40面 :圖, 表 ;30公分.

指導教授: 廖重賓, 郭文凱.

碩士論文--國立虎尾科技大學光電工程系光電與材料科技碩士班.

含參考書目.

透過在光纖端面整合 GMR 探頭實現了浸入式導模共振 (GMR) 感測器。導模共振元件的結構是波導和光柵的結合。光柵可以將入射光耦合到波導中並在內部傳播以產生洩漏模式。這種傳播的漏模波可以在共振條件下對零級傳輸波產生相消干涉，其高度依賴於GMR光柵表面液體的折射率(RI)，這可以用作RI感測器來感測由雙分子反應引起的RI 變化。 GMR 探頭採用奈米壓印紫外線固化樹脂製成，並使用低成本矽管安裝在單模光纖的端面。光纖傳輸光並將發散光束入射到 GMR 探頭感測器上。 GMR探頭的輸出光束處出現TM偏振共振條紋暗帶，且GMR感測器表面折射率變化所造成的條紋偏移可以透過低成本的CMOS影像感測器偵測到。實驗結果表明，可以達到1.18×10-5 RIU/像素的檢測極限，使原先整體測量系統體積整體縮小。.

(平裝)Subjects--Topical Terms:

1086329
nanoimprinting.

基於光纖端面之導模共振探頭的浸入式感測器 = = Dip-Type Sensor Based on a Guided-Mode Resonance Probe at the Facet of an Optical Fiber /
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245 1 0 $a 基於光纖端面之導模共振探頭的浸入式感測器 = $b Dip-Type Sensor Based on a Guided-Mode Resonance Probe at the Facet of an Optical Fiber / $c 游致傑.
246 1 1 $a Dip-Type Sensor Based on a Guided-Mode Resonance Probe at the Facet of an Optical Fiber.
250 $a 初版.
260 # $a 雲林縣 : $b 國立虎尾科技大學 , $c 民113.07.
300 $a [7], 40面 : $b 圖, 表 ; $c 30公分.
500 $a 指導教授: 廖重賓, 郭文凱.
500 $a 學年度: 112.
502 $a 碩士論文--國立虎尾科技大學光電工程系光電與材料科技碩士班.
504 $a 含參考書目.
520 3 $a 透過在光纖端面整合 GMR 探頭實現了浸入式導模共振 (GMR) 感測器。導模共振元件的結構是波導和光柵的結合。光柵可以將入射光耦合到波導中並在內部傳播以產生洩漏模式。這種傳播的漏模波可以在共振條件下對零級傳輸波產生相消干涉，其高度依賴於GMR光柵表面液體的折射率(RI)，這可以用作RI感測器來感測由雙分子反應引起的RI 變化。 GMR 探頭採用奈米壓印紫外線固化樹脂製成，並使用低成本矽管安裝在單模光纖的端面。光纖傳輸光並將發散光束入射到 GMR 探頭感測器上。 GMR探頭的輸出光束處出現TM偏振共振條紋暗帶，且GMR感測器表面折射率變化所造成的條紋偏移可以透過低成本的CMOS影像感測器偵測到。實驗結果表明，可以達到1.18×10-5 RIU/像素的檢測極限，使原先整體測量系統體積整體縮小。.
520 3 $a An immersed guided mode resonance (GMR) sensor was realized by integrating a GMR probe on the fiber end face. The structure of the guided mode resonant element is a combination of waveguide and grating. Gratings can couple incident light into the waveguide and propagate internally to create leakage modes. This propagating leaky mode wave can produce destructive interference to the zero-order transmitted wave under resonant conditions, which is highly dependent on the refractive index (RI) of the liquid on the surface of the GMR grating, which can be used as an RI sensor to sense the signal produced by the dual Changes in RI caused by molecular reactions. The GMR probe is made from nano-imprinted UV-curable resin and mounted on the end face of a single-mode optical fiber using low-cost silicon tubing. The optical fiber transmits the light and impinges the divergent beam onto the GMR probe sensor. The TM polarization resonance fringe dark band appears at the output beam of the GMR probe, and the fringe shift caused by the change in the refractive index of the GMR sensor surface can be detected through a low-cost CMOS image sensor. Experimental results show that the detection limit of 1.18×10-5 RIU/pixel can be reached..
563 $a (平裝)
650 # 4 $a nanoimprinting. $3 1086329
650 # 4 $a Guided-mode resonance. $3 1449875
650 # 4 $a fiber sensor. $3 1449874
650 # 4 $a 導模共振. $3 1015634
650 # 4 $a 光纖感測器. $3 1126992
650 # 4 $a 奈米壓印. $3 997511
856 7 # $u https://handle.ncl.edu.tw/11296/736q76 $z 電子資源 $2 http