2,726 research outputs found

    Contactless measurement of electric current using magnetic sensors

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    We review recent advances in magnetic sensors for DC/AC current transducers, especially novel AMR sensors and integrated fluxgates, and we make critical comparison of their properties. Most contactless electric current transducers use magnetic cores to concentrate the flux generated by the measured current and to shield the sensor against external magnetic fields. In order to achieve this, the magnetic core should be massive. We present coreless current transducers which are lightweight, linear and free of hysteresis and remanence. We also show how to suppress their weak point: crosstalk from external currents and magnetic fields

    Design of the new electromagnetic measurement system for RFX-mod upgrade

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    A major modification of the RFX-mod toroidal load assembly has been decided in order to improve passive MHD control and to minimize the braking torque on the plasma, thus extending the operational space in both RFP and Tokamak configurations. With the removal of the vacuum vessel, the support structure will be modified in order to obtain a new vacuum-tight chamber and the first wall tiles will be directly in front of the passive stabilizing shell inside of it, so increasing both the poloidal cross section and the plasma-shell proximity. This implies the design of a new vacuum fit electromagnetic measurement system. The new local probes will be installed in vacuum onto the copper shell, behind the graphite tiles, and shall operate up to a maximum temperature of 180\ub0C to allow for baking cycles for first wall conditioning. Because of the reduced room available, tri-axial pickup probes have been designed, with the additional advantage of allowing the minimization of alignment errors. The paper describes the detailed design of the new probe set, in particular highlighting advantages and effectiveness of different probe solutions. Preliminary tests carried out on local probe prototypes to characterize their electromagnetic behaviour are also reported

    A High-resolution Scintillating Fiber Tracker With Silicon Photomultiplier Array Readout

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    We present prototype modules for a tracking detector consisting of multiple layers of 0.25 mm diameter scintillating fibers that are read out by linear arrays of silicon photomultipliers. The module production process is described and measurements of the key properties for both the fibers and the readout devices are shown. Five modules have been subjected to a 12 GeV/c proton/pion testbeam at CERN. A spatial resolution of 0.05 mm and light yields exceeding 20 detected photons per minimum ionizing particle have been achieved, at a tracking efficiency of more than 98.5%. Possible techniques for further improvement of the spatial resolution are discussed.Comment: 31 pages, 27 figures, pre-print version of an article published in Nuclear Instruments and Methods in Physics Research Section A, Vol. 62

    고해상도 CMOS 이미지 μ„Όμ„œλ₯Ό μœ„ν•œ λ‚˜λ…Έκ΄‘ν•™μ†Œμž

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    ν•™μœ„λ…Όλ¬Έ(박사) -- μ„œμšΈλŒ€ν•™κ΅λŒ€ν•™μ› : κ³΅κ³ΌλŒ€ν•™ 전기·정보곡학뢀, 2021.8. μ΄λ³‘ν˜Έ.Image sensor is a device that converts electromagnetic waves scattered by the objects or environment into electric signals. Recently, in the mobile device and autonomous vehicle industries, multiple image sensors having different purposes are required for a single device. In particular, image sensors with more than 100 million pixels are being developed in response to the development of a display to a high resolution of 8K or more. However, due to the limited space of the mobile device, the size of pixels constituting the sensor must be reduced for a high-resolution image sensor, which causes factors that reduce image quality, such as a decrease in light efficiency, a decrease in quantum efficiency, and color interference. Metasurface is a device that modulates electromagnetic waves through an array of antennas smaller than wavelength. It has been proposed as a device that replaces the color filter, lens, and photodiode constituting the optical system of the image sensor. However, the performance of the metasurface corresponding to the miniaturized pixel size was limited by the operating principle that requires several array of nano-antennas. In this dissertation, I present a metasurface optical device that can improve the image quality of an existing image sensor composed of micropixels. First, an absorption type color filter that suppresses reflection is discussed. The reflection that inevitably occurs in the conventional metasurface color filter elements causes a flare phenomenon in the captured image. In this dissertation, I design a color filter that transmits only a specific band and absorbs the rest of the absorption resonant band of a hyperbolic metamaterial antenna using a particle swarm optimization method. In particular, I present a Bayer pattern color filter with a pixel size of 255 nm. Second, I introduce a color distribution meta-surface to increase the light efficiency of the image sensor. Since the photodiode converts light having energy above the band gap into an electric signal, an absorption type color filter is used for color classification in image sensor. This means that the total light efficiency of the image sensor is limited to 33% by the blue, green, and red filters constituting one pixel. Accordingly, a freeform metasurface device is designed that exceeds the conventional optical efficiency limit by distributing light incident on the sub-pixel in different directions according to color. Finally, an optical confinement device capable of increasing signal-to-noise ratio (SNR) in low-illuminance at near-infrared is presented. Through the funnel-shaped plasmonic aperture, the light is focused on a volume much smaller than the wavelength. The focused electric and magnetic fields interact with the spatially distributed semiconductors, which achieve a Purcell effect enhanced by the presence of the metasurface. This dissertation is expected to overcome the conventional nanophotonic devices for image sensors and become a cornerstone of the development of micropixel or nanopixel image sensors. Furthermore, it is expected to contribute to building a new image sensor platform that will replace the optical system constituting the image sensor with metasurface.이미지 μ„Όμ„œλŠ” ν™˜κ²½μ— μ˜ν•΄ μ‚°λž€λ˜λŠ” μ „μžκΈ°νŒŒλ₯Ό μ „κΈ°μ‹ ν˜Έλ‘œ λ°”κΎΈλŠ” μ†Œμžλ‘œ, 졜근 λͺ¨λ°”일 기기와 자율 μ£Όν–‰ μžλ™μ°¨ μ‚°μ—…μ—μ„œ 단일 λ””λ°”μ΄μŠ€μ— λ‹€λ₯Έ λͺ©μ μ„ 가진 이미지 μ„Όμ„œλ“€μ΄ μš”κ΅¬λ˜κ³  μžˆλ‹€. 특히, λ””μŠ€ν”Œλ ˆμ΄κ°€ 8K μ΄μƒμ˜ κ³ ν•΄μƒλ„λ‘œ λ°œμ „ν•¨μ— λŒ€μ‘ν•˜μ—¬ 1μ–΅ν™”μ†Œ μ΄μƒμ˜ 이미지 μ„Όμ„œκ°€ 개발되고 μžˆλ‹€. κ·ΈλŸ¬λ‚˜, λͺ¨λ°”일 기기의 μ œν•œλœ 곡간에 μ˜ν•΄ 고해상도 이미지 μ„Όμ„œλ₯Ό μœ„ν•΄μ„œλŠ” μ„Όμ„œλ₯Ό κ΅¬μ„±ν•˜λŠ” ν”½μ…€μ˜ 크기λ₯Ό 쀄여야 ν•˜λ©°, μ΄λŠ” κ΄‘ 효율 κ°μ†Œ, μ–‘μž 효율 κ°μ†Œ, 색 κ°„μ„­ λ“±μ˜ ν™”μ§ˆμ„ κ°μ†Œμ‹œν‚€λŠ” μš”μ†Œλ“€μ„ μ•ΌκΈ°ν•œλ‹€. λ©”νƒ€ν‘œλ©΄μ€ 파μž₯보닀 μž‘μ€ μ•ˆν…Œλ‚˜λ“€μ˜ 배열을 톡해 μ „μžκΈ°νŒŒλ₯Ό λ³€μ‘°ν•΄μ£ΌλŠ” μ†Œμžλ‘œ, 이미지 μ„Όμ„œμ˜ κ΄‘ν•™ μ‹œμŠ€ν…œμ„ κ΅¬μ„±ν•˜λŠ” 색 ν•„ν„°, 렌즈, 포토 λ‹€μ΄μ˜€λ“œλ₯Ό λŒ€μ²΄ν•˜λŠ” μ†Œμžλ‘œ μ œμ•ˆλ˜μ—ˆλ‹€. ν•˜μ§€λ§Œ, μ†Œν˜•ν™” 된 ν”½μ…€ 크기에 λŒ€μ‘ν•˜λŠ” λ©”νƒ€ν‘œλ©΄μ€ λ‚˜λ…Έ μ•ˆν…Œλ‚˜μ˜ λ™μž‘μ›λ¦¬μ™€ λ°°μ—΄μ˜ ν•œκ³„μ— μ˜ν•΄ μ„±λŠ₯이 μ œν•œλ˜μ—ˆλ‹€. λ³Έ λ…Όλ¬Έμ—μ„œλŠ” μ΄ˆμ†Œν˜• ν”½μ…€λ‘œ κ΅¬μ„±λœ κΈ°μ‘΄ 이미지 μ„Όμ„œμ— λŒ€ν•œ ν™”μ§ˆμ„ 높일 수 μžˆλŠ” λ©”νƒ€ν‘œλ©΄ κ΄‘ν•™μ†Œμžλ₯Ό μ œμ‹œν•œλ‹€. 첫째둜, λ°˜μ‚¬λ₯Ό μ–΅μ œν•˜λŠ” ν‘μˆ˜ν˜• 색 필터에 λŒ€ν•΄μ„œ λ…Όμ˜ν•œλ‹€. κΈ°μ‘΄ λ©”νƒ€ν‘œλ©΄ 색 ν•„ν„° μ†Œμžμ—μ„œ ν•„μ—°μ μœΌλ‘œ λ°œμƒν•˜λŠ” λ‚΄λΆ€ λ°˜μ‚¬λŠ” 찍은 μ΄λ―Έμ§€μ—μ„œ ν”Œλ ˆμ–΄ ν˜„μƒμ„ μœ λ°œν•œλ‹€. λ³Έ λ…Όλ¬Έμ—μ„œλŠ” 쌍곑 λ©”νƒ€λ¬Όμ§ˆ μ•ˆν…Œλ‚˜μ˜ 흑수 곡진 λŒ€μ—­μ„ μž…μž 무리 μ΅œμ ν™” 방식을 μ΄μš©ν•΄ νŠΉμ • λŒ€μ—­ λ§Œμ„ νˆ¬κ³Όν•˜κ³  λ‚˜λ¨Έμ§€λŠ” ν‘μˆ˜ν•˜λŠ” 색 ν•„ν„°λ₯Ό μ„€κ³„ν•œλ‹€. 특히, 255 nm 크기 ν”½μ…€μ˜ 베이어 νŒ¨ν„΄ 색 ν•„ν„°λ₯Ό μ œμ‹œν•œλ‹€. λ‘˜μ§Έλ‘œ, 이미지 μ„Όμ„œμ˜ κ΄‘ νš¨μœ¨μ„ 높이기 μœ„ν•œ 색 λΆ„λ°° λ©”νƒ€ν‘œλ©΄μ„ μ œμ‹œν•œλ‹€. 이미지 μ„Όμ„œμ˜ 포토 λ‹€μ΄μ˜€λ“œλŠ” λ°΄λ“œ κ°­ μ΄μƒμ˜ μ—λ„ˆμ§€λ₯Ό κ°€μ§€λŠ” 빛에 λŒ€ν•΄ μ „κΈ°μ‹ ν˜Έλ‘œ λ³€ν™˜ν•˜λ―€λ‘œ, 색 ꡬ뢄을 μœ„ν•΄ ν‘μˆ˜ν˜• 색 ν•„ν„°λ₯Ό μ‚¬μš©ν•œλ‹€. μ΄λŠ” ν•˜λ‚˜μ˜ 픽셀을 κ΅¬μ„±ν•˜λŠ” μ²­, λ…Ή, 적색 필터에 μ˜ν•΄ 이미지 μ„Όμ„œμ˜ 전체 κ΄‘ 효율이 33 %둜 μ œν•œλ˜λŠ” 것을 μ˜λ―Έν•œλ‹€. λ”°λΌμ„œ, μ„œλΈŒ 픽셀에 μž…μ‚¬ν•˜λŠ” 빛을 색에 따라 λ‹€λ₯Έ λ°©ν–₯으둜 빛을 λΆ„λ°°ν•˜μ—¬ 기쑴의 κ΄‘ 효율 ν•œκ³„λ₯Ό λ„˜μ–΄μ„œλŠ” μžμœ ν˜• λ©”νƒ€ν‘œλ©΄ μ†Œμžλ₯Ό μ„€κ³„ν•œλ‹€. λ§ˆμ§€λ§‰μœΌλ‘œ, μ €μ‘°λ„μ˜ κ·Όμ μ™Έμ„ μ—μ„œ μ‹ ν˜Έ λŒ€ μž‘μŒλΉ„λ₯Ό 높일 수 μžˆλŠ” κ΄‘ 집속 μ†Œμžλ₯Ό μ œμ‹œν•œλ‹€. κΉ”λŒ€κΈ° λͺ¨μ–‘μ˜ ν”ŒλΌμ¦ˆλͺ¨λ‹‰ 개ꡬλ₯Ό 톡해 빛을 파μž₯보닀 맀우 μž‘μ€ 크기의 μ˜μ—­μ— μ§‘μ€‘μ‹œν‚¨λ‹€. μ§‘μ†λœ μ „κΈ°μž₯κ³Ό 자기μž₯은 κ³΅κ°„μ μœΌλ‘œ λΆ„ν¬λœ λ°˜λ„μ²΄μ™€ μƒν˜Έμž‘μš©ν•¨μœΌλ‘œμ¨, λ©”νƒ€ν‘œλ©΄μ˜ μ‘΄μž¬μ— 따라 κ°•ν™”λœ Purcell 효과λ₯Ό μ–»λŠ”λ‹€. λ³Έ λ°•μ‚¬ν•™μœ„ 논문은 이미지 μ„Όμ„œλ₯Ό μœ„ν•œ 기쑴의 μ œν•œλœ λ©”νƒ€ν‘œλ©΄ μ†Œμžλ₯Ό κ·Ήλ³΅ν•˜κ³ , μ΄ˆμ†Œν˜• ν”½μ…€μ˜ 이미지 μ„Όμ„œ 개발의 μ΄ˆμ„μ΄ 될 κ²ƒμœΌλ‘œ κΈ°λŒ€λœλ‹€. λ‚˜μ•„κ°€, 이미지 μ„Όμ„œλ₯Ό κ΅¬μ„±ν•˜λŠ” κ΄‘ν•™ μ‹œμŠ€ν…œμ„ λ©”νƒ€ν‘œλ©΄μœΌλ‘œ λŒ€μ²΄ν•  μƒˆλ‘œμš΄ ν”Œλž«νΌμ„ κ΅¬μΆ•ν•˜λŠ” 것에 κΈ°μ—¬ν•  κ²ƒμœΌλ‘œ κΈ°λŒ€λœλ‹€.Chapter 1 Introduction 1 1.1 Overview of CMOS image sensors 1 1.2 Toward high-resolution miniaturized pixel 2 1.3 Nanophotonic elements for high-resolution camera 3 1.4 Dissertation overview 5 Chapter 2 Light interaction with subwavelength antennas 7 2.1 Overview of plasmonic antenna 7 2.2 Overview of dielectric metasurface 9 2.3 Overview of hyperbolic metamaterials 11 Chapter 3. Absorptive metasurface color filter based on hyperbolic metamaterial for noise reduction 14 3.1 Introduction 14 3.2 Principle of hyperbolic metamaterial absorbers 17 3.3 Absorptive color filter design based on particle swarm optimization method 19 3.4 Numerical analysis on optimized metasurface color filters 23 3.4.1 Single color filter optimization 23 3.4.2 Angle tolerance for optimized metasurface color filters 26 3.5 Sub-micron metasurface color filter array 29 3.6 Conclusion 35 Chapter 4 High-efficient full-color pixel array based on freeform nanostructures for high-resolution image sensor 37 4.1 Introduction 37 4.2 Optimization of metasurface full-color splitter 40 4.3 Implementation of color splitters 46 4.4 Image quality evaluation 52 4.5 Discussion about off-axis color splitters 55 4.6 Conclusion 59 Chapter 5 Plasmonic metasurface cavity for simultaneous enhancement of optical electric and magnetic fields 60 5.1 Introduction 60 5.2 Working principle and numerical results 63 5.2.1 Principle of funnel-shaped metasurface cavity 63 5.2.2 Discussion 67 5.3 Experimental results 69 5.4 Purcell effect 72 5.5 Conclusion 74 Chapter 6 Conclusion 75 Appendix 78 A.1 Colorimetry 78 A.2 Color difference CIEDE2000 79 B. Related work 80 Bibliography 81λ°•

    Study of current measurement method based on circular magnetic field sensing array

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    Β© 2018 by the authors. Licensee MDPI, Basel, Switzerland. Classic core-based instrument transformers are more prone to magnetic saturation. This affects the measurement accuracy of such transformers and limits their applications in measuring large direct current (DC). Moreover, protection and control systems may exhibit malfunctions due to such measurement errors. This paper presents a more accurate method for current measurement based on a circular magnetic field sensing array. The proposed measurement approach utilizes multiple hall sensors that are evenly distributed on a circle. The average value of all hall sensors is regarded as the final measurement. The calculation model is established in the case of magnetic field interference of the parallel wire, and the simulation results show that the error decreases significantly when the number of hall sensors n is greater than 8. The measurement error is less than 0.06% when the wire spacing is greater than 2.5 times the radius of the sensor array. A simulation study on the off-center primary conductor is conducted, and a kind of hall sensor compensation method is adopted to improve the accuracy. The simulation and test results indicate that the measurement error of the system is less than 0.1%
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