• Title/Summary/Keyword: Polarization imaging

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Direct Imaging of Polarization-induced Charge Distribution and Domain Switching using TEM

  • O, Sang-Ho
    • Proceedings of the Korean Vacuum Society Conference
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    • 2013.08a
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    • pp.99-99
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    • 2013
  • In this talk, I will present two research works in progress, which are: i) mapping of piezoelectric polarization and associated charge density distribution in the heteroepitaxial InGaN/GaN multi-quantum well (MQW) structure of a light emitting diode (LED) by using inline electron holography and ii) in-situ observation of the polarization switching process of an ferroelectric Pb(Zr1-x,Tix)O3 (PZT) thin film capacitor under an applied electric field in transmission electron microscope (TEM). In the first part, I will show that strain as well as total charge density distributions can be mapped quantitatively across all the functional layers constituting a LED, including n-type GaN, InGaN/GaN MQWs, and p-type GaN with sub-nm spatial resolution (~0.8 nm) by using inline electron holography. The experimentally obtained strain maps were verified by comparison with finite element method simulations and confirmed that not only InGaN QWs (2.5 nm in thickness) but also GaN QBs (10 nm in thickness) in the MQW structure are strained complementary to accommodate the lattice misfit strain. Because of this complementary strain of GaN QBs, the strain gradient and also (piezoelectric) polarization gradient across the MQW changes more steeply than expected, resulting in more polarization charge density at the MQW interfaces than the typically expected value from the spontaneous polarization mismatch alone. By quantitative and comparative analysis of the total charge density map with the polarization charge map, we can clarify what extent of the polarization charges are compensated by the electrons supplied from the n-doped GaN QBs. Comparison with the simulated energy band diagrams with various screening parameters show that only 60% of the net polarization charges are compensated by the electrons from the GaN QBs, which results in the internal field of ~2.0 MV cm-1 across each pair of GaN/InGaN of the MQW structure. In the second part of my talk, I will present in-situ observations of the polarization switching process of a planar Ni/PZT/SrRuO3 capacitor using TEM. We observed the preferential, but asymmetric, nucleation and forward growth of switched c-domains at the PZT/electrode interfaces arising from the built-in electric field beneath each interface. The subsequent sideways growth was inhibited by the depolarization field due to the imperfect charge compensation at the counter electrode and preexisting a-domain walls, leading to asymmetric switching. It was found that the preexisting a-domains split into fine a- and c-domains constituting a $90^{\circ}$ stripe domain pattern during the $180^{\circ}$ polarization switching process, revealing that these domains also actively participated in the out-of-plane polarization switching. The real-time observations uncovered the origin of the switching asymmetry and further clarified the importance of charged domain walls and the interfaces with electrodes in the ferroelectric switching processes.

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The research for the enhancement of depth of focus by elliptical polarization illumination(EPI) (타원편광 조명에 의한 초점심도 향상에 관한 연구)

  • 박정보;김기호;이성묵
    • Korean Journal of Optics and Photonics
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    • v.9 no.3
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    • pp.146-150
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    • 1998
  • To enhance the resolution and the depth of focus of the patterns whose size reaches the optical resolution limits, the various imaging methods are being tried. Generally in the linear polarization illumination methods, the contrast gap exists between TE mode TM mode according to the pattern direction. However, through the previous research, the elliptical polarization illumination(EPI) method was proposed to overcome this contrast gap. In this research, we investigated the optimal polarization condition to be able to enhance the depth of focus(DOF) for the optional mask which is containing the opposite direction patterns by applying the various polarization conditions including EPI. The DOF according to each polarization condition was obtained by ED-Tree(Exposure-Defocus Tree) for the given exposure dose and CD error boundaries. As the result, we can ascertain th effect of EPI for the enhancement of DOF in some condition of optical system.

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Hyperpolarization: Sensitivity Boost in Magnetic Resonance Spectroscopy and Imaging

  • Ko, Hyeji;Gong, Gyeonghyeon;Jeong, Gijin;Choi, Ikjang;Seo, Hyeonglim;Lee, Youngbok
    • Journal of the Korean Magnetic Resonance Society
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    • v.19 no.3
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    • pp.124-131
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    • 2015
  • Hyperpolarization methods are the most emerging techniques in the field of magnetic resonance (MR) researches since they make a contribution to overcoming sensitivity limitation of MR spectroscopy and imaging, leading to new fields of researches, real-time in vivo metabolic/molecular imaging and MR analysis of chemical/biological reactions in non-equilibrium conditions. Make use of enormous signal enrichments, it becomes feasible to investigate various chemical and biochemical systems with low ${\gamma}$ nuclei in real-time. This review deals with the theoretical principals of common hyperpolarization methods and their experimental features. In addition, more detailed theories, mechanisms, and applications of dissolution dynamic nuclear polarization (D-DNP) are discussed.

Stereo 3 mm Millimeter Wave Imaging for Distance Estimation to Concealed Objects (스테레오 3mm 밀리미터파 영상을 이용한 은닉물체의 거리추정에 관한 연구)

  • Yeom, Seokwon
    • Journal of the Institute of Convergence Signal Processing
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    • v.18 no.1
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    • pp.21-24
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    • 2017
  • Passive millimeter wave (MMW) imaging penetrates clothing to detect concealed objects. The distances extraction to the concealed objects is critical for the security and defense. In this paper, we address a passive stereo 3 mm MMW imaging system to extract the longitudinal distance to the concealed object. The concealed object area is segmented and extracted by the k-means clustering algorithm with splitting initialization. The distance to the concealed object is estimated by the corresponding centers of the segmented objects. In the experimental two pairs (each pair for horizontal and vertical polarization) of stereo MMW images are obtained to estimate distances to concealed objects.

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FIRST NEAR-INFRARED CIRCULAR POLARIZATION SURVEY

  • Kwon, Jungmi;Tamura, Motohide;Hough, James H.
    • The Bulletin of The Korean Astronomical Society
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    • v.41 no.2
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    • pp.57.2-57.2
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    • 2016
  • Polarimetry is an important tool for studying the physical processes in the interstellar medium, including star-forming regions. Polarimetry of young stellar objects and their circumstellar structures provides invaluable information about distributions of matter and configurations of magnetic fields in their environments. However, only a few near-infrared circular polarization (CP) observations were reported so far (before our survey). A systematic near-infrared CP survey has been firstly conducted in various star-forming regions, covering high-mass, intermediate-mass, and low-mass young stellar objects. All the observations were made using the SIRPOL imaging polarimeter on the Infrared Survey Facility (IRSF) 1.4 m telescope at the South African Astronomical Observatory (SAAO). In this presentation, we present the first CP survey results. The polarization patterns, extents, and maximum degrees of circular and linear polarizations are used to determine the prevalence and origin of CP in the star-forming regions. Our results are explained with a combination of circumstellar scattering and dichroic extinction mechanism generating the high degrees of CP in star-forming regions. The universality of the large and extended CPs in star-formaing regions can also be linked with the origin of homochirality of life.

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Statistical Characteristics of Polarization - Sensitive Optical Coherence Tomography for Tissue Imaging

  • Oh, Jung-Taek;Kim, Beop-Min;Kim, Seung-Woo
    • Journal of the Optical Society of Korea
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    • v.7 no.4
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    • pp.211-215
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    • 2003
  • Statistical characteristics of the backscattered light from turbid tissues obtained by polarizationsensitive optical coherence tomography are investigated. The amplitude of the backscattered light is found to faithfully follow the Rayleigh distribution predicted by the scattering theory of electromagnetic waves in random media. The probability density function of the phase difference between the two orthogonal polarization components of the backscattered light is explicitly derived and then verified in comparison with the experimental data measured from in-vitro tissues of porcine ligament.

Observation of the domain using secondary electron microscopy with polarization analysis(SEMPA)

  • Lee, Sang-Seon;Park, Yong-Seong;Kim, Won-Dong;Hwang, Chan-Yong
    • Proceedings of the Korean Vacuum Society Conference
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    • 2010.02a
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    • pp.396-396
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    • 2010
  • 최근에 자구벽 이동을 이용한 race track memory, 혹은 나노자성체의 자구 동역학 등에 대한 관심이 집중되고 있다. 용량은 하드디스크의 크기를 가지며 속도는 SRAM, 집적도는 DRAM에 필적하는 새로운 메모리의 실현은 지금까지 이용되는 대부분의 메모리를 대체할 가능성이 있다. 이러한 메모리의 개발에 가장 기본이 되는 측정기술은 나노크기의 자성 구조체에서 자구 혹은 자구벽 이동을 측정하는 기술로써 현재 국내에서 자성 나노구조의 자화방향과 더불어 topography를 동시에 측정할 수 있는 장치는 본 SEMPA가 유일하다. SEMPA는 기존에 사용되어지던 SEM(전자 현미경) 에서 알 수 있는 나노 구조의 형상이외에 전자의 스핀방향을 검출함으로써 형상과 스핀의 결함된 imaging 을 할 수 있다. 일반적으로 기존의 SEM의 경우 고 에너지빔의 전자빔을 주사시키고 이때 발생되는 이차 전자의 수를 2차원상의 영역에 따라 달라지는 비로 mapping 을 하게 된다. 이때 전자의 수뿐만 아니라 이들의 스핀편향(spin polarization) 을 측정할 수 있다면 형상뿐만 아니라 표면에서의 스핀상태를 동시에 측정 할 수 있게 된다. 본 발표에서는 이 방법을 이용하여 나노구조체의 자구측정 결과를 제시하고자 한다.

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Integral Imaging System Enabling Enhanced Depth of Field Incorporating a Birefringent Liquid Crystal Lens Array (복굴절 특성을 갖는 액정 렌즈어레이를 이용한 깊이감이 향상된 집적영상 시스템)

  • Park, Chan-Kyu;Hwang, Yong-Seok;Lee, Sang-Shin
    • Korean Journal of Optics and Photonics
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    • v.19 no.6
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    • pp.394-399
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    • 2008
  • An integral imaging system enabling enhanced depth of field by incorporating a pair of liquid-crystal (LC) lens arrays was proposed and demonstrated. The lens arrays exhibit two different refractive indexes depending on the light polarization. The proposed LC lens array I and II were implemented by depositing a ZLI-4119 LC and an E-7 LC, respectively, on top of a lens-array substrate in glass. When the two LC lens arrays were aligned appropriately, a birefringence was obtained for a specific light polarization in such a way that the incoming light sees different refractive indexes for them. As a result, the focal length associated with the imaging system utilizing the LC lens arrays was adaptively varied, thereby enhancing the depth of field for the image reconstruction. We have theoretically analyzed the proposed integral imaging system with the $LightTools^{(R)}$ to confirm that the focal length could be adjusted with the help of the birefringent lens array. Finally the proposed imaging system successfully reconstructed the objects. The birefringent lens array employing the ZLI-4119 LC produced a real image with the focal length of 680 mm, while the other using the E-7 LC yielded a virtual image with the focal length of -29 mm.

Polarization-sensitive Optical Coherence Tomography Imaging of Pleural Reaction Caused by Talc in an ex vivo Rabbit Model (생체 외 토끼 모델에서의 탈크에 의해 유발되는 흉막 반응의 편광 민감 광 결맞음 단층촬영 이미징)

  • Park, Jung-Eun;Xin, Zhou;Oak, Chulho;Kim, Sungwon;Lee, Haeyoung;Park, Eun-Kee;Jung, Minjung;Kwon, Daa Young;Tang, Shuo;Ahn, Yeh-Chan
    • Korean Journal of Optics and Photonics
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    • v.31 no.1
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    • pp.1-6
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    • 2020
  • The chest wall, an organ directly affected by environmental particles through respiration, consists of ribs, a pleural layer and intercostal muscles. To diagnose early and treat disease in this body part, it is important to visualize the details of the chest wall, but the structure of the pleural layer cannot be seen by chest computed tomography or ultrasound. On the other hand, optical coherence tomography (OCT), with a high spatial resolution, is suited to observe pleural-layer response to talc, one of the fine materials. However, intensity-based OCT is weak in providing information to distinguish the detailed structure of the chest wall, and cannot distinguish the reaction of the pleural layer from the change in the muscle by the talc. Polarization-sensitive OCT (PS-OCT) takes advantage of the fact that specific tissues like muscle, which have optical birefringence, change the backscattered light's polarization state. Moreover, the birefringence of muscle associated with the arrangement of myofilaments indicates the muscle's condition, by measuring retardation change. The PS-OCT image is interpreted from three major perspectives for talc-exposure chest-wall imaging: a thickened pleural layer, a separation between pleural layer and muscle, and a phase-retardation measurement around lesions. In this paper, a rabbit chest wall after talc pleurodesis is investigated by PS-OCT. The PS-OCT images visualize the pleural layer and muscle, respectively, and this system shows different birefringence of normal and damaged lesions. Also, an analyisis based on phase-retardation slope supports results from the PS-OCT image and histology.

The Large Magellanic Cloud Polarization Source Catalog : Evaluation of the polarimetric results

  • Kim, Jaeyeong;Jeong, Woong-Seob;Pak, Soojong;Sim, Chae Kyung;Park, Won-Kee;Pavel, Michael D.
    • The Bulletin of The Korean Astronomical Society
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    • v.38 no.2
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    • pp.53.1-53.1
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    • 2013
  • We compiled a near-infrared photometric and polarimetric catalog of $5{\times}9$ fields (${\sim}39^{\prime}{\times}69^{\prime}$) in the eastern side of the Large Magellanic Cloud (LMC). This catalog contains 9067 sources brighter than 16 mag in the J, H, and Ks bands, the polarization degree and position angle of each source. The photometric and polarimetric data were simultaneously obtained in J, H, and Ks bands using SIRPOL, an imaging polarimeter of the InfraRed Survey Facility (IRSF), in 2008 December and 2011 December. In this poster, we present a comparison between our results and those of Nakajima et al. (2007, PASJ, 59, 519) on the same sources in the 30 Doradus region in the LMC. We also discuss possible uncertainties in our polarimetric results when the Source Extractor is used to measure aperture photometry.

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