• Title/Summary/Keyword: electron beam deflection

Search Result 22, Processing Time 0.023 seconds

Characteristic Studies for Scan-Field Size and Visibility of Current Image in a Low Voltage Micro-Column (저 전압 초소형 전자칼럼의 주사면적 크기 및 전류영상 특성 연구)

  • Noriyuki, Ichimura;Kim, Young-Chul;Kim, Ho-Seob;Jang, Won-Kweon
    • Korean Journal of Optics and Photonics
    • /
    • v.19 no.5
    • /
    • pp.365-369
    • /
    • 2008
  • The optimal condition for focusing an electron beam was investigated employing an electrostatic deflector in a low voltage micro-column. At fixed voltage of the electron emission tip, the focusing electron beam with source lens showed a larger scan field size and poorer visibility than those with an Einzel lens. Theoretical 3-D simulation indicated that a focusing electron beam with a source lens should have a larger spot size and deflection than those of a focusing Einzel lens.

Analysis of 3-Dimensional Magnetic Field Distribution in CPM Considering Magnetization Vector Distribution and Design of CPM (자화 벡터 분포를 고려한 CPM의 3차원 자계 분포 해석 및 설계)

  • Lee, Cheol-Gyu;Gwon, Byeong-Il;Park, Seung-Chan;U, Gyeong-Il
    • The Transactions of the Korean Institute of Electrical Engineers B
    • /
    • v.51 no.10
    • /
    • pp.545-553
    • /
    • 2002
  • This paper is about the analysis of 3-dimensional magnetic field distribution in CPM(Convergence Purity Magnet) considering magnetization vector and the optimum design of CPM. The magnetization vector of CPM is obtained using 2-dimensional magnetization FEA(Finite Element Analysis) coupled with Priesach model. Using this magnetization vector of CPM, we analysed the 2-dimensional and 3-dimensional magnetostatic field of CPM and know that these analysis results are not equal. From experimental result, we know that the 3-dimensional analysis is accurate because the magnetic field distribution in CPM cannot be considered correctly by 2-dimensional analysis because of the shape of CPM. Finally, the optimum designing of CPM which control accurately the electron beam deflection in CRT(Cathode Ray Tube) was possible using 3-dimensional magnetic field analysis result.

A design of transmission-type multi-target X-ray tube based on electric field modulation

  • Zhao, Lei;Jia, Wenbao;Jin, Limin;Shan, Qing;Cheng, Can;Zhu, Hongkui;Hei, Daqian
    • Nuclear Engineering and Technology
    • /
    • v.53 no.9
    • /
    • pp.3026-3034
    • /
    • 2021
  • Multi-target X-ray tube is a new type X-ray source, and can be applied in many fields such as sensitive X-ray fluorescence analysis and medical imaging. In this work, we report an electric field modulation multi-target X-ray tube, which contains four targets (Cr, Ni, Au, Mo) coated on a Beryllium (Be) window. A four-valve electric field deflector was developed to deflect the electron beam to bombard the corresponding targets. Particle dynamics analysis software was employed to simulate the particle tracking of electron beam. The results show that the 30 keV electron beam could get a 6.7 mm displacement on the target plane by 105 V/m electric field. The focus areas are about 2 mm × 5 mm and 4 mm × 2.5 mm after deflection in two directions. Thermal behavior calculated by ANSYS shows that the designed target assembly could withstand a 10 W continuous power. The optimum target thicknesses and emission spectra were obtained by Geant4 when the thickness of Be window was 300 mm and the electron beam incident angle was 0.141 rad. The results indicate that this multi-target X-ray tube could provide different X-ray sources effectively.

Control of Convergence for Deflection Yoke Using Neuro-Fuzzy Model (뉴로 퍼지 모델을 이용한 편향요크의 RGB색 일치에 대한 제어)

  • 정병묵;임윤규;정창욱
    • Journal of the Korean Society for Precision Engineering
    • /
    • v.15 no.5
    • /
    • pp.19-27
    • /
    • 1998
  • Color Display Tube (CDT) used in computer monitors, consists of many components. Deflection Yoke(DY) among them supplies the vertical and horizontal magnetic fields so that the spatial trajectories of electron beams are deflected according to the synchronization signals. If the magnetic fields are not correctly formed, there will be color blurring or blooming by a mis-convergence of each beam and the color image on screen may not be clear. Therefore, in the manufacture of DY. its quality is strictly examined to get the desired convergence and the occurred mis-convergence can be cured by sticking ferrite sheets on the inner part of DY. However, because it needs expert's knowledge and experience to find the proper position of the sheet, this article introduces an intelligent controller that the knowledge-base represented by a neuro-fuzzy model is used to find the optimal position of the ferrite sheet for the convergence.

  • PDF

Design Verification of the DY (Deflection Yoke) Using a CAI (Computer-Aided Inspection) Technique (전산역설계(Reverse Engineering) 기술을 이용한 편향코일(DY)의 설계 검증 연구)

  • 윤정호;전형환;최광일;김용환;이관행
    • Korean Journal of Computational Design and Engineering
    • /
    • v.3 no.1
    • /
    • pp.22-30
    • /
    • 1998
  • The deflection yoke (DY) controls the direction of the electron beam that falls on the screen of the television monitor. Its quality depends on the shape and density of coils wound around the DY coil separator. Winding frames are used to make these coils, and therefore, their shapes are essential in making quality coils. A reverse engineering(RE) is applied to create the 3D model of the winding frame. It considerably shortens the design verification time and shows the level of accuracy that is feasible in the production mode. The paper explains each step of the reverse engineering process in detail.

  • PDF

A Study on Design and Analysis for Magnetic Lenses of a Scanning Electron Microscope using Finite Element Method (유한요소법을 사용한 주사전자 현미경의 전자렌즈 설계 및 해석에 관한 연구)

  • Park, Keun;Jung, Hyun-Woo;Park, Man-Jin;Kim, Dong-Hwan;Jang, Dong-Young
    • Journal of the Korean Society for Precision Engineering
    • /
    • v.24 no.9
    • /
    • pp.95-102
    • /
    • 2007
  • The scanning electron microscope (SEM) is one of the most popular instruments available for the measurement and analysis of the micro/nano structures. It is equipped with an electron optical system that consists of an electron beam source, magnetic lenses, apertures, deflection coils, and a detector. The magnetic lenses playa role in refracting electron beams to obtain a focused spot using the magnetic field driven by an electric current from a coil. A SEM column usually contains two condenser lenses and an objective lens. The condenser lenses generate a magnetic field that forces the electron beams to form crossovers at desired locations. The objective lens then focuses the electron beams on the specimen. The present work concerns finite element analysis for the electron magnetic lenses so as to analyze their magnetic characteristics. To improve the performance of the magnetic lenses, the effect of the excitation current and pole-piece design on the amount of resulting magnetic fields and their peak locations are analyzed through the finite element analysis.

The Fast Intelligent Tracking (F!T) Tube: Feedback Signal Acquisition

  • Lieshout, P.J.G. van;Engelaar, P.J.
    • 한국정보디스플레이학회:학술대회논문집
    • /
    • 2002.08a
    • /
    • pp.351-354
    • /
    • 2002
  • The F!T tube is a new type of CRT without a shadow mask. Correct color reproduction is performed by an electronic system that measures the landing positions of the electron beams and corrects through a dedicated deflection system. This paper describes in detail the position sensor and some of the electronics needed to build a functional control system. The principle has been shown in single- and triple-beam 17" and 32" tubes, of which results are included.

  • PDF

A Study on Particle Diffusion to Develop Faraday Cup Array of Particle Beam Mass Spectrometer System (Faraday cup array 개발을 위한 Particle Beam Mass Spectrometer 시스템 내에서의 입자 확산 연구)

  • Mun, Ji-Hun;Shin, Yong-Hyun;Kim, Tae-Sung;Kang, Sang-Woo
    • Particle and aerosol research
    • /
    • v.8 no.1
    • /
    • pp.29-35
    • /
    • 2012
  • The Faraday cup electrode of different size has been developed and evaluated to investigate the diffusion effect of particles by Brownian motion in a particle beam mass spectrometer(PBMS). Particles which focused and accelerated by aerodynamic lens are charged to saturation in an electron beam, and then deflected electrostatically into a Faraday cup detector for measurement of the particle current. The concentration of particles is converted from currents detected by Faraday cup. Measurements of particle current as a function of deflection voltage are combined with measured relationships between particle velocity and diameter, charge and diameter, and mass and diameter, to determine the particle size distribution. The particle currents were measured using 5, 10, 20, 40 mm sized Faraday cup that can be move to one direction by motion shaft. The current difference for each sizes as a function of position was compared to figure out diffusion effect during transport. Polystyrene latex(PSL) 100, 200 nm sized standard particles were used for evaluation. The measurement using 5 mm sized Faraday cup has the highest resolution in a diffusion distance and the smaller particles had widely diffused.

Nanoparticle Synthesis by Pulsed Laser Ablation of Consolidated Microparticles (압밀 금속 마이크로 입자의 펄스 레이저 ABLATION에 의한 나노입자 합성)

  • 장덕석;오부국;김동식
    • Laser Solutions
    • /
    • v.5 no.2
    • /
    • pp.31-38
    • /
    • 2002
  • This paper describes the process of nanoparticle synthesis by laser ablation of consolidated microparticles. We have generated nanoparticles by high-power pulsed laser ablation of Al, Cu and Ag microparticles using a Q-switched Nd:YAG laser (wavelength 355 nm, FWHM 5 ㎱, fluence 0.8∼2.0 J/㎠). Microparticles of mean diameter 18∼80 ㎛ are ablated in the ambient air The generated nanoparticles are collected on a glass substrate and the size distribution and morphology are examined using a scanning electron microscope and a transmission electron microscope. The effect of laser fluence and collector position on the distribution of particle size is investigated. The dynamics of ablation plume and shock wave is analyzed by monitoring the photoacoustic probe-beam deflection signal. Nanosecond time-resolved images of the ablation process are also obtained by laser flash shadowgraphy. Based on the experimental results, discussions are made on the dynamics of ablation plume.

  • PDF

Study on the Scan Field of Modified Octupole and Quadrupole Deflector in a Microcolumn (마이크로칼럼에서 변형된 4중극 디플렉터와 8중극 디플렉터의 스캔 영역 비교)

  • Kim, Young Chul;Kim, Ho-Seob;Ahn, Seong Joon;Oh, Tae-Sik;Kim, Dae-Wook
    • Journal of the Korea Academia-Industrial cooperation Society
    • /
    • v.19 no.11
    • /
    • pp.1-7
    • /
    • 2018
  • In a microcolumn, a miniaturized electrostatic deflector is often adopted to scan an electron beam. Usually, a double octupole deflector is used because it can avoid excessive spherical aberrations by controlling the electron beam path close to the optical axis of the objective lens and has a wide scan field. Studies on microcolumns have been performed to improve the low throughput of an electron column through multiple column applications. On the other hand, as the number of microcolumns increases, the number of wires connected to the components of the microcolumn increases. This will result in practical problems during the process of connecting the wires to electronic controllers outside of the vacuum chamber. To reduce this problem, modified quadrupole and octupole deflectors were examined through simulation analysis by selecting an ultraminiaturized microcolumn with the Einzel lens eliminated. The modified deflectors were designed changing the size of each electrode of the conventional Si octupole deflector. The variations of the scan field and electric field strength were studied by changing the size of active electrodes to which the deflection voltage was to be applied. The scan field increased linearly with increasing deflection voltage. The scan field of the quadrupole deflector and the electric field strength at the center were calculated to be approximately 1.3 ~ 2.0 times larger than those of the octupole deflector depending on the electrode size.