• 제목/요약/키워드: v-ray

검색결과 2,493건 처리시간 0.028초

다층박막 거울을 이용한 단색 엑스선 획득 (Acquisition of Monochromatic X-ray Using Multilayer Mirror)

  • 천권수
    • 대한방사선기술학회지:방사선기술과학
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    • 제33권3호
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    • pp.179-184
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    • 2010
  • 나노 공간분해능을 갖는 영상을 얻기 위한 경엑스선 현미경 시스템에서는 단색 엑스선이 요구된다. 엑스선관에서 발생되는 화이트 빔으로부터 8.4 keV의 텅스텐 $L_{\alpha}$ 특성방사선을 84% 이상 반사시킬 수 있는 5.65 nm의 단위막 두께를 가지는 C/W 다층박막 거울을 설계하였고, 이온빔 스파터링 장치를 이용하여 $50{\times}50\;mm$ 크기로 제작하였다. 제작된 C/W 다층박막 거울은 99.5% 이상의 균일도(Uniformity)를 가지며, TEM 사진을 이용해 그 구조를 확인하였다. 8.05 keV의 구리 특성방사선을 광원으로 하는 엑스선 반사율 측정 장치를 이용한 다층박막 거울의 반사율을 측정함으로써 C/W 다층박막 거울의 8.4 keV에서의 반사율을 예상할 수 있었다. 제작된 C/W 다층박막 거울과 엑스선관을 이용하여 8.4 keV의 특성방사선을 획득함으로써 단색 엑스선을 획득하였다. 이때의 반사율은 77.1%였고, 단색 엑스선의 반치폭은 0.21 keV이었다. 엑스선관에서 높은 효율로 단색 엑스선을 획득할 수 있어 실험실 규모의 경엑스선 현미경 장치의 광원으로써 사용될 수 있는 가능성을 확인하였고, 다층박막 거울의 단위막 두께를 수 나노미터로 제작한다면 17.5 keV의 몰리브덴 특성방사선에 해당하는 단색 엑스선을 얻어 유방촬영에도 적용할 수 있을 것이다.

이중 적층 구조 표적을 갖는 투과형 엑스선관의 몬테카를로 전산모사 (Monte Carlo Simulation of Transmission-Type X-ray Tube with Dual-Structured Target)

  • 천권수
    • 한국방사선학회논문지
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    • 제17권1호
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    • pp.107-114
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    • 2023
  • 엑스선형광분석은 비파괴적으로 시료에 포함된 원소와 농도를 분석할 수 있는 기법으로 과학 및 산업 분야에 광범위하게 사용되고 있다. 다양한 물질을 포함한 혼합물 또는 화합물 분석의 정밀도 향상을 위해 10 keV 근방의 저에너지와 20 keV 근방의 에너지 영역에 높은 강도 분포를 갖는 엑스선관이 요구된다. 두 에너지 영역에서 높은 강도 분포를 갖는 스펙트럼을 얻기 위하여 9.65 keV의 특성엑스선을 가지는 텅스텐과 17.48 keV의 몰리브덴 두 물질을 적층한 구조의 표적을 가지는 투과형 엑스선관을 몬테카를로 전산모사를 통해 스펙트럼을 분석하였다. W-Mo 구조의 표적을 통해 10 keV와 20 keV 근방의 강한 강도를 갖는 특성엑스선을 얻었다. 또한 4 ㎛ 두께의 Mo-W multilayers 구조의 표적을 통해 최적의 강도 분포를 갖는 스펙트럼을 얻을 수 있음을 확인하였다. 다양한 표적 물질을 선택 조합하고 두께 최적화를 통해 원하는 에너지 대역에서 높은 강도 분포를 갖는 스펙트럼을 얻는 것이 가능하다.

W-target 투과 양극형 Soft x-ray tube의 개발 및 특성분석 (Development and Characteristics of the Soft x-ray transmission W-target tube)

  • 김성수;김도윤
    • 한국진공학회지
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    • 제16권4호
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    • pp.305-310
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    • 2007
  • W-target 투과양극형 x-ray tube를 개발하고, 특성을 조사하였다. 관전압이 12kV이하에서는 연속 x-ray만 방출되었고, 12kV 이상에서부터 특성 x-ray가 관측되었다. 연속 x-ray와 특성 x-ray의 에너지 분포 및 선량 특성을 조사한 결과 알려진 결과와 잘 일치함을 알 수 있었다. 또한 상용화된 제품과의 비교에서, 기존 제품 이상의 성능을 가질 수 있음을 확인하였다. 따라서 본 연구에서 개발된 x-ray tube는 상용화할 수 있을 만큼 충분히 우수한 특성을 가지고 있음을 확인하였다.

THE TeV GAMMA-RAY MILKY WAY

  • ROWELL, GAVIN
    • 천문학논총
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    • 제30권2호
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    • pp.553-557
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    • 2015
  • This review summarises the current status of the Galactic TeV ($10^{12}$ eV) gamma-ray source population. It also briefly looks at the future beyond the current generation of TeV gamma-ray facilities, and highlights the role of the interstellar medium (ISM) in helping to resolve some of the challenges in interpreting the wealth of results which have been found in recent years.

Novel bricks based lightweight Vietnam's white clay minerals for gamma ray shielding purposes: An extensive experimental study

  • Ta Van Thuong;O.L. Tashlykov;K.A. Mahmoud
    • Nuclear Engineering and Technology
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    • 제56권2호
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    • pp.666-672
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    • 2024
  • In the present work, a new brick series based on the Vietnamese white clay minerals from the Bat Trang was fabricated to be applied in the radiation protection applications during the decommissioning of the nuclear power reactors. The bricks were constructed under various pressure rates varied from 7.61 MPa to 114.22 MPa. The influence of pressure rate on the physical and γ-ray shielding properties were investigated in the study. The experimental measurement for the material's density using the MH-300A density meter showed an enhancement in the prepared bricks' density by 22.5 % with increasing the applied pressure rate while the bricks' porosity reduced by 31.2 % when the pressure rate increased from 7.61 MPa to 114.22 MPa. The increase in the fabricated bricks density and the reduction in their porosities enhances the bricks' linear attenuation coefficients as measured by the NaI (Tl) detector along the energy range extended from 0.662 MeV to 1.332 MeV. The linear attenuation coefficient increased by 13.8 %, 17.6 %, 17.0 %, and 17.1 % at gamma ray energies of 0.662 MeV, 1.173 MeV, 1.252 MeV, and 1.332 MeV, respectively. The enhancement in the linear attenuation coefficient increases the bricks' radiation protection efficiency by 10.22 %, 14.48 %, 14.09 %, and 14.26 % at gamma ray energies of 0.662 MeV, 1.173 MeV, 1.252 MeV, and 1.332 MeV, respectively.

$^{99}Mo-^{99m}TcO_4$ Generator의 감마선량 분포에 관한 연구 (A Study of Gamma-ray Distribution around the $^{99}Mo-^{99m}TcO_4$ Generator)

  • 박성옥
    • 대한방사선기술학회지:방사선기술과학
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    • 제24권1호
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    • pp.49-53
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    • 2001
  • A number of radionuclides of interest in nuclear medicine are short lived isotopes that emit only gamma ray. The most of all Dept. of Nuclear Medicine in the hospt. are using the $^{99}Mo-^{99m}Tc$ generator for elution of the short lived isotope $^{99m}TcO_4$. A $^{99}Mo-^{99m}Tc$ generator consists of an alumina column on which $^{99}Mo$ is bound. The parent isotope($^{99}Mo$ : half life 67 hr.) decays to its daughter $^{99m}TcO_4^-$ which is a different element with a shorter half-life. $^{99}Mo$ emitted 41-keV(1.3%), 141-keV(5.6%) 181-keV(6.6%) and 366-keV(1.5%) gamma rays. But $^{99m}TcO_4$ emitted only 140-keV gamma ray. We study about the gamma ray distribution around the $^{99}Mo$ generator. And obtained the result as follows ; 1. Total counted gamma ray from generator smaller in front side than back. 2. The gamma ray emitted from $^{99}Mo$ generator without $^{99m}TcO_4$ vial increased in the back side(Mo column posited side) 3. The gamma ray only from the $^{99m}TcO_4$ vial increased in the front side. 4. Apron can protect gamma ray above 60% of total radiation from the $^{99}Mo$ generator.

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40kV용 투과양극형 x-ray tube에 의한 X-ray 형광 특성 (Characteristics of the X-ray Fluorescence by the 40kV transmission anode x-ray tube)

  • 김성수;김도윤
    • 한국진공학회지
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    • 제17권3호
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    • pp.247-252
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    • 2008
  • 휴대용 XRF(X-Ray Fluorescence) 장치에 적용하기 위하여 개발한 투과 양극형 x-ray tube를 이용하여 XRF 실험을 하고, x-ray tube가 XRF data에 미치는 영향을 조사하였다. W-target tube와 Rh-target tube를 이용하여 측정한 XRF data는 알려진 결과와 잘 일치하였다. 35 kV와 관전압과 $40{\mu}A$의 관전류에서 W-target tube로 측정한 Fe $K_{\alpha}$-line의 FWHM은 약 180 eV로써, 이 값은 물질의 성분분석을 하기에 충분한 것으로 확인하였다. XRF data와 x-ray tube의 적분강도 곡선을 비교 분석해 본 결과, 휴대용 XRF 장치에는 W-Target tube보다는 Rh-Target tube를 사용하는 것이 더 유리함을 밝혀내었다.

Effect of the amount of battery charge on tube voltage in different hand-held dental x-ray systems

  • Kim, Eun-Kyung
    • Imaging Science in Dentistry
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    • 제42권1호
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    • pp.1-4
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    • 2012
  • Purpose : Hand-held dental x-ray system is a self contained x-ray machine designed to perform intraoral radiography with one or two hands. The issue about its usage as general dental radiography is still in dispute. The aim of the present study was to assess the relationship between the amount of battery charge and the tube voltage in different handheld dental x-ray systems. Materials and Methods : Seven hand-held dental x-ray units were used for the study. Tube voltage was measured with Unfors ThinX RAD (Unfors Instruments AB, Billdal, Sweden) for 3 consecutive exposures at the different amount of battery charge of each unit. The average and the deviation percentage of measured kV from indicated kV of each unit were calculated. Results : Tube voltage of only 1 unit was 70 kV (indicated by manufacturer) and those of the others were 60 kV. Tube voltage deviation percentage from the indicated kV at the fully charged battery was from 2.5% to -5.5% and from -0.8% to -10.0% at the lowest charged battery. Conclusion : Tube voltages of all units decreased as the residual amount of the battery charge decreased. It is suggested that the performance test for hand-held x-ray system should be performed for the minimum residual charged battery as well as the full charged one. Persistent battery charging is suggested to maintain the proper tube voltage of the hand-held portable x-ray system.

변형 DEEP X-ray를 이용한 마이크로 렌즈 및 V-groove 제작 (Microlens Micro V-groove Fabrication by the Modified LIGA Process)

  • 이정아;이승섭;전병희
    • 소성∙가공
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    • 제13권3호
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    • pp.290-295
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    • 2004
  • Mircolens and microlens V-groove are realized using a novel fabrication technology based on the exposure of a resist, usually PMMA, to deep X-rays and subsequent thermal treatment and inclined deep X-ray lithography, respectively. The fabrication technology is very simple and produces microlenses and microlens V-groove with good surface roughness of several nm. The molecular weight and glass transition temperature of PMMA is reduced when it is irradiated with deep X-rays. The microlenses were produced through the effects of volume change, surface tension, and reflow during thermal treatment of irradiated PMMA. Microlenses were produced with diameters ranging from 30 to $1500\mu\textrm{m}$. The surface X-ray mask is also fabricated to realize microlens arrays on PMMA sheet with a large area. The size of the micro V-groove is fabricated in the range of 12~$60\mu\textrm{m}$.

Monte Carlo N-Particle Extended Code를 이용한 연 X선 정전기제거장치의 최적제작에 관한 연구(II) (A Study on the Optimal Make of X-ray Ionizer using the Monte Carlo N-Particle Extended Code(II))

  • 정필훈;이동훈
    • 한국안전학회지
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    • 제32권6호
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    • pp.29-33
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    • 2017
  • In order to solve this sort of electrostatic failure in Display and Semiconductor process, Soft X-ray ionizer is mainly used. Soft X-ray Ionizer does not only generate electrical noise and minute particle but also is efficient to remove electrostatic as it has a wide range of ionization. There exist variable factors such as type of tungsten thickness deposited on target, Anode voltage etc., and it takes a lot of time and financial resource to find optimal performance by manufacturing with actual X-ray tube source. Here, MCNPX (Monte Carlo N-Particle Extended) is used for simulation to solve this kind of problem, and optimum efficiency of X-ray generation is anticipated. In this study, X-ray generation efficiency was compared according to target material thickness using MCNPX and actual X-ray tube source under the conditions that tube voltage is 5 keV, 10 keV, 15 keV and the target Material is Tungsten(W). At the result, In Tube voltage 5 keV and distance 100 mm, optimal target thickness is $0.05{\mu}m$ and fastest decay time appears + decay time 0.28 sec. - deacy time 0.30 sec. In Tube voltage 10keV and distance 100 mm, optimal target Thickness is $0.16{\mu}m$ and fastest decay time appears + decay time 0.13 sec. - deacy time 0.12 sec. In the tube voltage 15 keV and distance 100 mm, optimal target Thickness is $0.28{\mu}m$ and fastest decay time appears + decay time 0.04 sec. - deacy time 0.05 sec.