• Title/Summary/Keyword: Proton Generation

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Design Study for Pulsed Proton Beam Generation

  • Kim, Han-Sung;Kwon, Hyeok-Jung;Seol, Kyung-Tae;Cho, Yong-Sub
    • Nuclear Engineering and Technology
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    • v.48 no.1
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    • pp.189-199
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    • 2016
  • Fast neutrons with a broad energy spectrum, with which it is possible to evaluate nuclear data for various research fields such as medical applications and the development of fusion reactors, can be generated by irradiating proton beams on target materials such as beryllium. To generate short-pulse proton beam, we adopted a deflector and slit system. In a simple deflector with slit system, most of the proton beam is blocked by the slit, especially when the beam pulse width is short. Therefore, the available beam current is very low, which results in low neutron flux. In this study, we proposed beam modulation using a buncher cavity to increase the available beam current. The ideal field pattern for the buncher cavity is sawtooth. To make the field pattern similar to a sawtooth waveform, a multiharmonic buncher was adopted. The design process for the multiharmonic buncher includes a beam dynamics calculation and three-dimensional electromagnetic simulation. In addition to the system design for pulsed proton generation, a test bench with a microwave ion source is under preparation to test the performance of the system. The design study results concerning the pulsed proton beam generation and the test bench preparation with some preliminary test results are presented in this paper.

RESEARCH ON LASER-ACCELERATED PROTON GENERATION AT KAERI

  • PARK SEONG HEE;LEE KITAE;CHA YOUNG HO;JEONG YOUNG UK;BAIK SUNG HOON;YOO BYUNG DUK
    • Nuclear Engineering and Technology
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    • v.37 no.3
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    • pp.279-286
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    • 2005
  • A prototype of a relativistic proton generation system, based on laser-induced plasma interaction, has been designed and fabricated. The system is composed of three major parts: a fs TW laser; a target chamber, including targets and controls; and a diagnostic system for charged particles and lasers. An Offner-type pulse stretcher for chirped pulse amplification (CPA) and eight pass pre-amplifier are installed. The main amplifier will be integrated with a new pumping laser. The design values of the laser at the first stage are 1 TW in power and 50 fs in pulse duration. We expect to generate protons with their maximum energy of approximately 3 MeV and the flux of at least $10^6$ per pulse using a 10 $\mu$m Al target. A prototype target chamber with eight 8-inch flanges, including target mounts, has been designed and fabricated. For laser diagnostics, an adaptive optics based on the Shack-Hartmann type, beam monitoring, and alignment system are all under development. For a charged particle, CR-39 detectors, a Thomson parabola spectrometer, and Si charged-particle detectors will be used for the density profile and energy spectrum. In this paper, we present the preliminary design for laser-induced proton generation. We also present plans for future work, as well as theoretical simulations.

Production of Haploids from Proton Ion and Gamma-Ray Irradiation Treated $M_2$ Generation of Isolated Microspores in Brassica napus L. ssp. oleifera (앙성자 및 감마선을 처리한 유채 $M_2$ 세대의 소포자로부터 반수체 배발생)

  • Kim, Kwang-Soo;Li, Mei-Yang;Jang, Young-Seok;Park, Yoon-Jung;Bang, Jin-Ki
    • KOREAN JOURNAL OF CROP SCIENCE
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    • v.53 no.2
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    • pp.150-155
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    • 2008
  • This experiment was carried out to investigate the effect of proton ion and gamma-ray irradiation on microspore culture of the flower buds of $M_2$ generation in winter type of Brassica napus L. ssp. oleifera. The seeds of three rape varieties, 'Halla', 'Naehan' and 'Tammi' were pretreated with proton ion and gamma-ray 400 Gy and 600 Gy, respectively. When microspore culture techniques were used, embryogenesis was increased in some varieties by proton ion and gamma-ray irradiation treated flower buds of $M_2$ generation than control. In genotypes 'Naehan' showed the highest embryo production frequency, but 'Tammi' showed lowest embryo production frequency. Some of the embryoids developed directly into plantlets, whereas others developed abnormally multilobe. Plants were regenerated and successfully acclimatized in pots.

A Design of Solar Proton Telescope for Next Generation Small Satellite

  • Sohn, Jongdae;Oh, Suyeon;Yi, Yu;Min, Kyoung-Wook;Lee, Dae-Young;Seon, Jongho
    • Journal of Astronomy and Space Sciences
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    • v.29 no.4
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    • pp.343-349
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    • 2012
  • The solar proton telescope (SPT) is considered as one of the scientific instruments to be installed in instruments for the study of space storm (ISSS) which is determined for next generation small satellite-1 (NEXTSat-1). The SPT is the instrument that acquires the information on energetic particles, especially the energy and flux of proton, according to the solar activity in the space radiation environment. We performed the simulation to determine the specification of the SPT using geometry and tracking 4 (GEANT4). The simulation was performed in the range of 0.6-1,000 MeV considering that the proton, which is to be detected, corresponds to the high energy region according to the solar activity in the space radiation environment. By using aluminum as a blocking material and adjusting the energy detection range, we determined total 7 channels (0.6~5, 5~10, 10~20, 20~35, 35~52, 52~72, and >72 MeV) for the energy range of SPT. In the SPT, the proton energy was distinguished using linear energy transfer to compare with or discriminate from relativistic electron for the channels P1-P3 which are the range of less than 20 MeV, and above those channels, the energy was determined on the basis of whether silicon semiconductor detector (SSD) signal can pass or not. To determine the optimal channel, we performed the conceptual design of payload which uses the SSD. The designed SPT will improve the understanding on the capture and decline of solar energetic particles at the radiation belt by measuring the energetic proton.

Non volatile memory device using mobile proton in gate insulator by hydrogen neutral beam treatment

  • Yun, Jang-Won;Jang, Jin-Nyeong;Hong, Mun-Pyo
    • Proceedings of the Korean Vacuum Society Conference
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    • 2015.08a
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    • pp.192.1-192.1
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    • 2015
  • We demonstrated the nonvolatile memory functionality of nano-crystalline silicon (nc-Si) and InGaZnOxide (IGZO) thin film transistors (TFTs) using mobile protons that are generated by very short time hydrogen neutral beam (H-NB) treatment in gate insulator (SiO2). The whole memory fabrication process kept under $50^{\circ}C$ (except SiO2 deposition process; $300^{\circ}C$). These devices exhibited reproducible hysteresis, reversible switching, and nonvolatile memory behaviors in comparison with those of the conventional FET devices. We also executed hydrogen treatment in order to figure out the difference of mobile proton generation between PECVD and H-NB CVD that we modified. Our study will further provide a vision of creating memory functionality and incorporating proton-based storage elements onto a probability of next generation flexible memorable electronics such as low power consumption flexible display panel.

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A Feasibility Design of PEMFC Parallel Operation for a Fuel Cell Generation System

  • Kang, Hyun-Soo;Choe, Gyu-Yeong;Lee, Byoung-Kuk;Hur, Jin
    • Journal of Electrical Engineering and Technology
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    • v.3 no.3
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    • pp.408-421
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    • 2008
  • In this paper, the parallel operation for a FC generation system is introduced and designed in order to increase the capacity for the distributed generation of a proton exchange membrane fuel cell (PEMFC) system. The equipment is the type that is used by parallel operated PEMFC generation systems which have two PEMFC systems, two dc/dc boost converters with shared dc link, and a grid-connected dc/ac inverter for embedded generation. The system requirement for the purpose of parallel operated generation using PEMFC system is also described. Aspects related to the mechanical (MBOP) and electrical (EBOP) component, size, and system complexity of the distributed generation system, it is explained in order to design an optimal distributed generation system using PEMFC. The optimal controller design for the parallel operation of the converter is suggested and informative simulations and experimental results are provided.

Blue Light Generation in a Quasi-Phase-Matched $LiTaO_3$ Optical Waveguide (준위상정합된 리튬탄탈레이트 광도파로에서의 청색 광파 생성)

  • 이상윤;신상영;진용성
    • Journal of the Korean Institute of Telematics and Electronics A
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    • v.32A no.12
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    • pp.173-183
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    • 1995
  • Blue light of 0.15mW at 417.6nm is generated in a quasi-phase-matched LITaO$_{3}$ optical waveguide. A new heat-treatment technique using a metal-oxide mask is proposed to fabricate the periodic domain-inverted grating with less degraded optical properties. The mask promotes the proton indiffusion by inhibition of the proton outdiffusion during the heat treatment. It reduces the amount of the initial proton exchange for the domain inversion and prevents the formation of crystal defects on the surface accompanied by the proton outdiffusion. Consequently, it minimizes the degradation of nonlinear coefficient and scattering loss caused by the initial proton exchange.

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Preparation of Highly Concentrated Alumina Suspension through Investigstion of Proton Adsorption Density (수소이온 흡착밀도의 고찰을 통한 고농도 알루미나 현탁액의 제조)

  • Kim, Duk-Jun;Kim, Hwan
    • Journal of the Korean Ceramic Society
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    • v.33 no.2
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    • pp.163-168
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    • 1996
  • Measurements of proton adsorption density have been conducted in preparing alumina suspensions with aqueous solutions of HCL, HNO3, H2SO4 and H3PO4 And effects of anion acid concentration proton adsorption density and solid loading on the viscosity of the alumina suspensions have been investigated. Aqueous solutions of HCl. or HNO3 were suitable for the preparation of highly concentrated suspensions as the generation of surface charge on alumina particles was depressed by the specific adsorption of {{{{ {SO }`_{4 } ^{2- } }} and {{{{ { PO}`_{4 } ^{3- } }} Optimum conditions for maximizing solid loading were dependent upon proton adsorption density and acid concentration.

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MEASUREMENT OF THE D-D NEUTRON GENERATION RATE BY PROTON COUNTING

  • Kim, In-Jung;Jung, Nam-Suk;Choi, Hee-Dong
    • Nuclear Engineering and Technology
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    • v.40 no.4
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    • pp.299-304
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    • 2008
  • A detection system was set up to measure the neutron generation rate of a recently developed D-D neutron generator. The system is composed of a Si detector, He-3 detector, and electronics for pulse height analysis. The neutron generation rate was measured by counting protons using the Si detector, and the data was crosschecked by counting neutrons with the He-3 detector. The efficiencies of the Si and He-3 detectors were calibrated independently by using a standard alpha particle source $^{241}Am$ and a bare isotopic neutron source $^{252}Cf$, respectively. The effect of the cross-sectional difference between the D(d,p)T and $D(d,n)^3He$ reactions was evaluated for the case of a thick target. The neutron generation rate was theoretically corrected for the anisotropic emission of protons and neutrons in the D-D reactions. The attenuations of neutron on the path to the He-3 detector by the target assembly and vacuum flange of the neutron generator were considered by the Monte Carlo method using the MCNP 4C2 code. As a result, the neutron generation rate based on the Si detector measurement was determined with a relative uncertainty of ${\pm}5%$, and the two rates measured by both detectors corroborated within 20%.

Effects of the Micro-hole Target Structures on the Laser-driven Energetic Proton Generation

  • Pae, Ki-Hong;Choi, Il-Woo;Hahn, Sang-June;Lee, Jong-Min
    • Journal of the Optical Society of Korea
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    • v.13 no.1
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    • pp.48-52
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    • 2009
  • Micro-hole targets are studied to generate energetic protons from laser-thin foil targets by using 2-dimensional particle-in-cell simulations. By using a small hole, the maximum energy of the accelerated proton is increased to 4 times higher than that from a simple planar target. The main proton acceleration mechanism of the hole-targets is the electrostatic field created between the fast electrons accelerated by the laser pulse ponderomotive force combined with the vacuum heating and the target rear surface. But in this case, the proton angular distribution shows double-peak shape, which means poor collimation and low current density. By using a small cone-shaped hole, the maximum proton energy is increased 3 times higher than that from a simple planar target. Furthermore, the angular distribution of the accelerated protons shows good collimation.