• Title/Summary/Keyword: Polarization grating

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2-Dimensional scattering by a periodic strip grating on a grounded dielectric slab (접지된 유전체층 위에 위치한 주기적인 스트립격자 구조에 의한 2차원적인 산란)

  • Ko, J.H.;Baek, W.S.;Yun, L.H.;Lee, J.I.;Cho, U.H.;Lee, C.H.;Hong, J.P.;Cho, Y.K.;Son, H.
    • The Journal of Korean Institute of Communications and Information Sciences
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    • v.21 no.10
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    • pp.2710-2723
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    • 1996
  • 2-dimensional scattering problem of electromagnetic waves by a periodic strip grating on a grounded dielectric slab in case of oblique incidence and arbitrary polarization is analyed by the vector Floquet modal expansion method. Solution convergence versus number of Chebyshev polynomial terms representing the unknown strip current density and number of space harmonics is examined, and some numerical results such as variation of power of significant space harmonics(scattered mode) are compared with those obtained by previous method. In particaluar, the relationship between Bragg blazing phonmena and characteristics mode(current) on the srip is discussed in detail.

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The Fast Convergent Solution of E-Polarized Reflection Coefficient by a Perfect Conductor Strip Grating (완전도체 스트립 회절격자에 의한 E-분극 반사계수의 급속한 수염해)

  • Uei-Joong Yoon
    • The Proceeding of the Korean Institute of Electromagnetic Engineering and Science
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    • v.6 no.1
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    • pp.10-16
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    • 1995
  • The E-polarized scattering problems by a perfect conductor strip grating are analyzed by the method of moments. For an E-polarization the induced surface current density is expected to blow up at the strip both edges. Then the induced surface current density on the strip is expanded in a series of multiplication of Ultraspherical ploynomials with zeroth order and functions with appropriate edge boundary condition. The numerical results for current density and reflection cofficient are compared with other functions, it is shown that numerical results better improves the convergence of the moment method soulutions with general incident angles than the existing several other functions. The sharp variation points in the magnitude of geometric-optical reflection coefficient can be moved by varying the incident angle, strip width, and strip spacing.

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40channel Arrayed Waveguide Grating with O.75delta% Refractive Index (0.75Δ% 굴절율차를 가진 40채널 광파장 다중화 및 역다중화 소자 제작 및 특성)

  • Moon, H.M.;Choi, G.S.;Lee, K.H.;Kim, D.H.;Lee, J.H.;Lee, D.H.;Oh, J.K;Kwak, S.C.;Kwon, O.K.;Kang, D.S.;Choi, J.S.;Jong, G;Lee, H.Y.
    • Korean Journal of Optics and Photonics
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    • v.16 no.3
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    • pp.196-200
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    • 2005
  • A 40 channel arrayed-waveguide grating (AWG) filter operating in C-band and L-band wavelength regions has been fabricated using PLC (Planar Lightwave Circuit) processes with 0.75 refractive index difference. Its design was optimized for matching the center wavelength with the ITU-recommended wavelength. The characteristics of the fabricated C-band AWG are as follows; average insertion loss < 2.5 dB, polarization-dependent loss < 0.3 dB, non-adjacent crosstalk >35dB, and the loss uniformity of 0.8 dB. In the L-band AWG, wavelength accuracy is below 0.02nm.

Tunable and switchable multi-wavelength erbium-doped fiber ring laser (파장변환과 스위칭이 가능한 다파장 어븀 첨가 광섬유 링 레이저)

  • Jang, Hyun-Soo;Lee, Kyung-Shik
    • Journal of the Institute of Electronics Engineers of Korea SD
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    • v.42 no.7 s.337
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    • pp.13-20
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    • 2005
  • We propose an erbium-doped fiber ring laser whose multi-wavelength oscillation is tunable and switchable by tuning fiber bragg gratings. By applying axial pressure on the fiber bragg grating, the wavelength spacing of the proposed laser can be tuned continuously. And by adjusting a polarization controller(PC), the proposed laser can be switched among dual-, triple- and four-wavelength lasing operations.

A Study of Diffraction Efficiency Depended on $Ag^+$ of Amorphous Chalcogenide Thin Films (Amorphous chalcogenide 박막의 $Ag^+$ 의존적 회절효율 특성에 관한 연 구)

  • Jeong, Won-Kook;Nam, Ki-Hyun;Chung, Hong-Bay
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2010.06a
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    • pp.134-134
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    • 2010
  • We have investigated the holographic grating formation on Ag-doped amorphous chalcogenide AsGeSeS thin films with Ag thickness. Holographic gratings have been formed using Diode Pumped Solid State laser (DPSS, 532.0nm) under [P:P] polarized the intensity polarization holography. The diffraction efficiency was obtained by +1st order intensity.

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Polarimetric fiber pressure sensor based on polarization-maintaining fiber and fiber grating (편광유지 광섬유와 광섬유 격자를 기반으로 하는 편광 간섭형 광섬유 압력 센서)

  • Choi, Sungwook;Lee, Yong Wook
    • Proceedings of the KIEE Conference
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    • 2015.07a
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    • pp.1265-1266
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    • 2015
  • 본 논문에서는 PMF와 FBG로 구성된 PDL 기반 사냑 간섭계를 이용하여 편광 간섭형 광섬유 압력 센서를 구현하였다. 여러 종류의 PMF들에서 압력 민감도를 비교하기 위해, 서로 다른 세 종류의 보우-타이형 PMF를 센서부로 사용하였다. 구현된 광섬유 압력 센서를 이용하여 0~0.3 MPa의 범위에서 압력 측정을 수행하였으며, 최대 압력 민감도는 근사적으로 -15.07 nm/MPa로 측정되었고, 센서의 선형성을 나타내는 $R^2$값은 ~0.992로 측정되었다. 제안된 센서는 FBG를 이용하여 외부 온도 변화의 보상이 가능하면서도, 이전의 편광유지 광자결정 광섬유 기반 압력 센서에 비해 압력 민감도를 4배까지 증가시킬 수 있었다.

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Surface Relief Holograms on azo-polymer film

  • Yatagai, Toyohiko;Harada, Kenji
    • 한국정보디스플레이학회:학술대회논문집
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    • 2002.08a
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    • pp.293-296
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    • 2002
  • Surface relief holograms are fabricated by means of irradiation of laser interference patterns. The diffraction efficiency and the surface relief depth depend on the writing energy and the polarization of the writing laser beam. This structure is very stable at temperatures under glass transition temperature $T_g$ and can be erased by heating above $T_g$. We proposed a new technique to control the surface relief structure. The electric charge was deposited on the surface relief grating in a corona-depositing poling setup in an oven. The first-order diffraction efficiency measured before and after corona discharge increased from about 0.24 % to about 28 %. This diffraction efficiency increase is mainly caused by the increase of the relief depth caused by the electric charge. The relief depth is increased from 20 nm to 350 nm by corona charging. .

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Splitting of Surface Plasmon Resonance Peaks Under TE- and TM-polarized Illumination

  • Yoon, Su-Jin;Hwang, Jeongwoo;Lee, Myeong-Ju;Kang, Sang-Woo;Kim, Jong-Su;Ku, Zahyun;Urbas, Augustine;Lee, Sang Jun
    • Proceedings of the Korean Vacuum Society Conference
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    • 2014.02a
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    • pp.296-296
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    • 2014
  • We investigate experimentally and theoretically the splitting of surface plasmon (SP) resonance peaks under TE- and TM-polarized illumination. The SP structure at infrared wavelength is fabricated with a 2-dimensional square periodic array of circular holes penetrating through Au (gold) film. In brief, the processing steps to fabricate the SP structure are as follows. (i) A standard optical lithography was performed to produce to a periodic array of photoresist (PR) circular cylinders. (ii) After the PR pattern, e-beam evaporation was used to deposit a 50-nm thick layer of Au. (iii) A lift-off processing with acetone to remove the PR layer, leading to final structure (pitch, $p=2.2{\mu}m$; aperture size, $d=1.1{\mu}m$) as shown in Fig. 1(a). The transmission is measured using a Nicolet Fourier-transform infrared spectroscopy (FTIR) at the incident angle from $0^{\circ}$ to $36^{\circ}$ with a step of $4^{\circ}$ both in TE and TM polarization. Measured first and second order SP resonances at interface between Au and GaAs exhibit the splitting into two branches under TM-polarized light as shown in Fig. 1(b). However, as the incidence angle under TE polarization is increased, the $1^{st}$ order SP resonance peak blue-shifts slightly while the splitting of $2^{nd}$ order SP resonance peak tends to be larger (not shown here). For the purpose of understanding our experimental results qualitatively, SP resonance peak wavelengths can be calculated from momentum matching condition (black circle depicted in Fig. 2(b)), $k_{sp}=k_{\parallel}{\pm}iG_x{\pm}jG_y$, where $k_{sp}$ is the SP wavevector, $k_{\parallel}$ is the in-plane component of incident light wavevector, i and j are SP coupling order, and G is the grating momentum wavevector. Moreover, for better understanding we performed 3D full field electromagnetic simulations of SP structure using a finite integration technique (CST Microwave Studio). Fig. 1(b) shows an excellent agreement between the experimental, calculated and CST-simulated splitting of SP resonance peaks with various incidence angles under TM-polarized illumination (TE results are not shown here). The simulated z-component electric field (Ez) distribution at incident angle, $4^{\circ}$ and $16^{\circ}$ under TM polarization and at the corresponding SP resonance wavelength is shown in Fig. 1(c). The analysis and comparison of theoretical results with experiment indicates a good agreement of the splitting behavior of the surface plasmon resonance modes at oblique incidence both in TE and TM polarization.

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Non-uniform Leaky Wave Structure Composed of Finite Conducting Strip Array on a Grounded Dielectric Layer (접지된 유전체층 위에 위치한 유한한 도체스트립 배열구조로 구성된 비균일 누설파구조)

  • Lee, Jong-Ig;Lee, Cheol-Hoon;Cho, Young-Ki
    • Journal of the Korean Institute of Telematics and Electronics D
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    • v.36D no.8
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    • pp.45-53
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    • 1999
  • Electromagnetic scattering by finite number of conducting strips loaded on a grounded dielectric is considered for the TM polarization case from the viewpoints of transmitting(receiving) leaky wave antenna and grating coupler. An integro-differential equation whose unknowns are the induced currents over the strips is derived and solved by use of the method of moments. In order to construct the non-uniform leaky wave structures with specific source(current) distributions over the strips, distances between two adjacent strips and strip width are simultaneously varied along the structure. From some results for the current distributions over the strips and surface wave powers, it is observed that the maximum coupling efficiencies of the appropriately constructed non-uniform leaky wave structures from the viewpoints of both a receiving leaky wave antenna and a grating coupler amount upto 95%, which are about 15% improvements compared with those(80%) of the uniform structures.

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Guided-mode Resonances in Periodic Surface Structures Induced on Si Thin Film by a Laser (레이저에 의해 생성된 Si 박막의 주기적 표면 구조에서의 도파모드 공진 연구)

  • Ji Hyuk Lee;Yoon Joo Lee;Hyun Hong;Eun Sol Cho;Ji Young Park;Ju Hyeon Kim;Min Jin Kang;Eui Sun Hwang;Byoung-Ho Cheong
    • Korean Journal of Optics and Photonics
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    • v.34 no.6
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    • pp.241-247
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    • 2023
  • We examine the spectral characteristics of laser-induced periodic surface structures (LIPSSs) formed on an amorphous silicon film irradiated by a 355-nm nanosecond laser. A Gaussian beam with a diameter of 196 ㎛ is used to perform a two-dimensional raster scan. The laser's pulse number is varied from 190 to 280, and its intensity is adjusted within 100-130 mJ/cm2. LIPSSs with a periodicity of approximately 330 nm form on the surface of the Si film, aligned perpendicular to the laser's polarization. Transmission spectra of the samples show dips around 700 nm for transverse electric polarization and around 500 nm for transverse magnetic polarization. The features are investigated with a one-dimensional-grating model using a rigorous coupled-wave analysis. Simulations confirm that the observed dips are due to the resonant modes, depending on the polarization.