• 센서학회지
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• 제13권5호
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• pp.342-349
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• 2004

SK (SPR Kinds) index, which can categorize the complicated measurement methods of surface plasmon resonance by simple method, has been proposed and verified. SK index is composed of three digits, where each digit presents the type of immobilized ligand, the type of illumination and the kinds of varying parameter, sequentially. The measurement method of (33#) series among SK indices shows the possibility of the multi-sensing capability, by which the response of 2-dimensional array of immobilized ligands can be detected simultaneously. The proposed possibility of multi-sensing capability has been verified by the modeling that is based on Fresnel reflection model.

• 한국농업기계학회:학술대회논문집
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• 한국농업기계학회 2003년도 동계 학술대회 논문집
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• pp.200-208
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• 2003

미생물수를 측정하는 가장 정확하고 보편적인 방법은 배양법이다. 그러나 배양법은 많은 시간과 노력이 소요되기 때문에 현장에서 실시간에 준하는 측정법으로 사용하기에는 원천적으로 한계를 가지고 있다. 이러한 한계를 극복하기 위해서는 실시간(real-time) 또는 준실시간(near real-time)으로 미생물을 검출할 수 있는 기술이 요구된다. 표면플라즈몬공명(surface plasmon resonance: SPR)은 생물분자 또는 미생물을 실시간 또는 준실시간으로 검출할 수 있는 센서로서 특이성(specificity)과 정확도(accuracy) 측면에서 일찍이 큰 관심을 받아왔다. 1902년, Wood(1902)는 반사 회절격자를 사용하여 연속광원의 스펙트럼을 관찰한 결과, 회절광 스펙트럼에서 어두운 좁은 밴드를 발견하였으며, Fano(1941)는 이 현상이 surface plasma waves와 관련이 있음을 이론적으로 밝혔다. (중략)

• 전기학회논문지
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• 제58권4호
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• pp.795-800
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• 2009

Surface plasmon resonance (SPR) has been widely used for biological and chemical sensing applications. The present study investigates numerically the optical characteristics for the single Au film and bimetallic Ag/Au film SPR configurations by using the multiple beam interference matrix (MBIM) method. We use the prism coupling method, especially Kretschmann configuration for excitation of surface plasmon wave (SPW). The estimated results of reflectance, phase shift and magnetic field intensity enhancement factor are provided for finding out the optimum configuration with high sensitivity for SPR measurement. As a result, the optimum thicknesses are found to be 52 nm for a single Au film and 5 nm to 36 nm for bimetallic Ag-Au film. From the comparison of full width half maximum (FWHM) values for reflectance, phase shift, and enhancement of magnetic field intensity, it is concluded that the highest sensitivity can be obtained when using the phase shift for SPR sensor.

• 센서학회지
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• 제15권5호
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• pp.347-351
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• 2006

A novel surface plasmon resonance sensor, which can measure 2-dimensional array of immobilized ligands without using imaging devices such as CCD, has been proposed. Regular surface plasmon resonance can be directly used due to the insertion of additional layers with different thickness, on which each ligands are immobilized. Surface plasmon resonance signals are separated depending on the thickness of additional layers. The possibility of multi-sensing capability of the proposed surface plasmon resonance sensor has been verified by the modeling that is based on Fresnel reflection model.

• 전기학회논문지
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• 제59권5호
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• pp.922-926
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• 2010

We have investigated the grating coupled surface plasmon resonance (GC-SPR) sensors using ZnO nano-grating structures to enhance the sensitivity of an SPR sensor. The GC-SPR sensors were analyzed using the finite-difference time-domain method. The optimum resonance angles of 49 degrees are obtained in the 150 nm wide grating structure with a period of 300 nm for the ZnO thickness of 30 nm. Then, the ZnO nano-grating patterns were fabricated by using laser interference lithography. The measured resonance angle of nano-grating patterns was around 49 degrees. Here, an enhanced evanescent field is obtained due to the surface plasmon on the edge of the bandgap when the ZnO grating structures are used to excite the surface palsmon.

• 한국정밀공학회:학술대회논문집
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• 한국정밀공학회 2009년도 춘계학술대회 논문집
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• pp.863-864
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• 2009

• 센서학회지
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• 제14권6호
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• pp.402-408
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• 2005

This paper describes the optimal design of a multi-layered surface plasmon resonance sensors to meet various specifications and improve some physical parameters. Dip 3 dB bandwidth and depth were chosen as design parameters and the objective function was the norm of the difference between design parameters and target values. The design variables are thicknesses of each layer and to obtain the design parameters, the optical admittance method was employed. The (1+1) evolution strategy was employed as an optimization tool. By applying the proposed optimization procedure to a 3-layered sensor, the optimized design variables considerably improved the 3 dB bandwidth by 4.8 nm and the dip depth by 1.1 dB.

• 전기학회논문지
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• 제61권3호
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• pp.433-436
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• 2012

We propose a novel micro surface plasmon resonance (SPR) sensor system based on polymer materials. The proposed SPR system consists of the incident medium with polymer waveguide and the gold thin film for sensing area. Using a polymer optical waveguide instead of a prism in SPR sensing system offers miniaturization, low cost, and potable sensing capability. The whole device performance was analyzed using the finite-difference time domain method. The optimum gold thickness in the attenuated total reflection mirror of polymer waveguide is around 50 nm and the resonance angle to generate surface plasmon wave is 68 degrees.

• 통합자연과학논문집
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• 제2권2호
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• pp.59-64
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• 2009

금속 나노 입자의 표면편재 플라즈몬 공명 주파수에 영향을 미치는 금속의 유전율은 조사된 빛의 파장 값에 의존하는 함수로 표현된다. 본 연구에서는 유전율의 실수부와 허수부 값을 체계적으로 변화시킬 수 있는 가상의 금속 나노 막대를 대상으로, 이산 쌍극자 근사(Discrete dipole approximation)를 사용하여, 광학적 성질을 계산하였다. 계산 결과, 유전율 함수의 실수부가 선형적으로 감소하는 경우에는 금속의 크기가 커짐에 따라 최대 소광이 나타나는 피크가 긴 파장영역으로 이동했고, 반대로 실수부가 선형적으로 증가하는 경우에는 최대 소광이 나타나는 피크가 짧은 파장영역으로 이동함을 알 수 있었다. 허수부 값을 증가시켰을 경우에는, 실수부에 관계없이 그 값이 증가함에 따라 피크의 세기가 감쇠하는 경향을 보였다.

• 대한전기학회논문지:전기물성ㆍ응용부문C
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• 제55권10호
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• pp.492-498
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• 2006

A novel surface plasmon resonance(SPR) multisensing method, which does not require imaging apparatus such as CCD, has been proposed and implemented experimentally. The proposed method is based on the multichannel SPR and the separation of signals by use of additional layers whose thickness is controlled. SPR signals are influenced by the thickness of sensing layer as well as the optical condition of sensing surface. As the SPR signals from different ligands are usually positioned closely, the reflected light from sensing surface does not provide us with the clear differences of resonance signal depending on the kinds of ligands. It was found from our experiments that SPR signals from each ligand that is located on the additional layer with different thickness can be separated clearly enough to identify various signals from different ligands. Proposed method with theoretical design and simulation has been verified experimentally by using $SiO_2$ thin film layer as additional layer.