한국해양대학교

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금속 평행판 도파로를 통한 테라파의 전파 특성

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dc.contributor.author 이의수 -
dc.date.accessioned 2017-02-22T05:54:36Z -
dc.date.available 2017-02-22T05:54:36Z -
dc.date.issued 2009 -
dc.date.submitted 56904-11-24 -
dc.identifier.uri http://kmou.dcollection.net/jsp/common/DcLoOrgPer.jsp?sItemId=000002174709 ko_KR
dc.identifier.uri http://repository.kmou.ac.kr/handle/2014.oak/8784 -
dc.description.abstract We investigated the propagation of single- and multi-mode terahertz (THz) radiation for various gap sizes a parallel-plate waveguide (PPWG) and polarizations of the incoming THz field. Single TEM (TM_(0)) and TE₁ modes within the 4-THz frequency range propagated through a waveguide with a 103μm plate separation. Multi TE and TM modes were observed for a 360-μm separation. High-order modes have a very high group velocity dispersion near the cutoff frequencies, which causes extensive pulse reshaping and broadening in addition to multimode interference in the time and frequency region. The majority dominant mode is TE₁ (97.96%) and TM_(0) (81.61%) modes because the lowest mode has a small absorption and an incident even field pattern. Because each mode has different transmission and coupling coefficients, absorption, and propagation constant, the theoretical calculation for the total TM or TE modes requires a summation of the components. The theoretical calculation and the measured data fit well in the frequency and time domain. The high pass filtering effects using TE₁ mode in which blocks off the signal under the cutoff frequency were also investigated. The well filtered signal from TM multi-mode was also observed. And the experiment at (spoof) surface plasmon polaritons(SPP) with PPWG system was performed. The several rectangular and slit holes on the stainless steel sheet with 50μm thickness were perforated. The resonance signals of SPP known as Bragg reflection were observed. Using the period of rectangular holes and slits, the polarity of the detected resonance signal was explained as the phase differences between the main pulse and resonance pulses. The experiment results show that SPPs propagate the upper and under the metal sheet through holes. The propagation of TM multi-mode terahertz radiation through PPWG with the gap size of 360μm was simulated using the finite-difference time-domain(FDTD) method. The simulation data could explain the difference between the experimental data and the theoretical calculation. Also the experiment of SPP's Bragg reflections by slits was simulated. The simulation shows that how THz wave propagates and reflects in the slits. The results of FDTD simulation fit well with the experimental data and the theoretical calculation. -
dc.description.tableofcontents 제1장 서론 = 1 1. 1 “테라헤르쯔” = 1 1.2 금속 평행판 도파로(Metal Parallel-Plate Waveguide) = 2 1.3 실험 측정 장치도 = 3 제2장 PPWG를 통한 단일·다중 모드 전파 특성 = 6 2. 1 관련 이론 = 6 2.1.1 TM 모드(E_(x), E_(z), H_(y)) = 7 2.1.2 TE 모드(H_(x), H_(z), E_(y)) = 11 2.1.3 Even / Odd Mode = 13 2.2 단일 모드(Single-mode) 전파, TEM(TM_(0))/TE₁ = 14 2.2.1. Reference 측정 = 14 2.2.2. 단일 모드, TEM(TM_(0)) = 14 2.2.3. 단일 모드, TE₁ = 16 2.3 다중 모드(Multi-mode) 전파, TM_(m) / TE_(m) = 17 2.3.1. 다중 모드, TM_(m) = 17 2.3.2. 다중 모드, TE_(m) = 19 2.4 다중 모드 전파 분석 = 20 2.4.1. Spectrocronography = 20 2.4.2. Fitting = 22 제3장 THz Photonics (THz 포토닉스) = 24 3.1 Filter = 24 3.2 표면 플라즈몬 폴라리톤(Surface Plasmon Polaritons) = 25 3.2.1 “Surface Plasmon Polaritons” = 25 3.2.2 SPPs의 수식적 유도 = 27 3.3 PPWG를 이용한 SPPs의 유도 및 전파 특성 연구 = 30 3.3.1 실험 장치도 = 30 3.3.2 측정된 SPPs의 전파 특성 분석 = 31 제4장 FDTD를 이용한 THz 전자기파의 전파 특성 해석(시뮬레이션) = 41 4.1 Finite-Difference Time-Domain(FDTD)란? = 41 4.2 FDTD 시뮬레이션 = 47 4.2.1 Source : 가우시안 펄스 = 49 4.2.2 PML : 흡수 경계 영역 = 50 4.2.3 TM_(m), 다중 모드 (평행판 간격 360㎛) 시뮬레이션 = 52 4.2.4 slit이 존재하는 금속판을 진행하는 테라파 전파 특성 시뮬레이션 = 55 제5장 결론 = 58 참고문헌 = 60 -
dc.language kor -
dc.publisher 한국해양대학교 대학원 -
dc.title 금속 평행판 도파로를 통한 테라파의 전파 특성 -
dc.title.alternative Propagation Properties of Terahertz radiation Through a metal parallel-plate waveguide -
dc.type Thesis -
dc.date.awarded 2009-02 -
dc.contributor.alternativeName LEE -
dc.contributor.alternativeName EUI SU -
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