• 제목/요약/키워드: 14 MeV

검색결과 152건 처리시간 0.035초

유리선량계를 이용한 고에너지 전자선 측정 이용 가능성에 관한 연구 (Feasibility Study of the Radiophotoluminescent Glass Dosimeter for High-energy Electron Beams)

  • 손기홍;정해조;신상훈;이현호;이성현;김미숙;지영훈;김금배
    • 한국의학물리학회지:의학물리
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    • 제22권1호
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    • pp.52-58
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    • 2011
  • 본 연구에서는 유리선량계를 이용하여 전자선 치료빔의 선량평가 이용 가능성을 판단하고자 하였다. GD-302M 유리선량계에 선형가속기를 이용한 전자선과 $^{60}Co$ 방사선조사기로부터 감마선을 조사하였다. 유리선량계의 전자선에서의 선량 선형성, 재현성, 방향성, 선량률의존성, 에너지의존성의 총 5개 항목에 대해서 평가를 하였다. 측정은 물팬톰 $40{\times}40{\times}40cm^3$을 이용하여 유리선량계의 흡수선량을 측정하였다. 명목상 전자선에너지 6, 9, 12, 16, 20 MeV에서의 선량 1 Gy부터 15 Gy까지 유리선량계의 반응도를 평가해 본 결과 5개 전자선 에너지에서 같은 $R^2$=0.999의 선형계수를 확인할 수 있었다. 또한 5개의 에너지에서 총 100개의 유리선량계를 판독한 결과, 재현성은 5개 전자선에너지 평균 ${\pm}1.2%$ (1SD) 이내에서 잘 일치함을 확인할 수 있었다. 유리선량계의 방향성은 유리선량계의 수직방향인 $90^{\circ}$를 기준으로 하였을때 $0^{\circ}$에서 $90^{\circ}$사이에서 빔방향에 따라 1.5% 이내의 차이를 나타내었다. 선량률의존성은 500 MU/min을 기준으로 200 MU/min에서 1,000 MU/min 사이에서 ${\pm}1.5%$의 차이를 나타내었다. 유리선량계의 에너지 의존성은 원통형 전리함으로 측정한 선량과 비교했을때 5개의 명목상 전자선에너지(6 MeV에서 20 MeV) 각각에 대해 $^{60}Co$ 감마선의 반응도로 일반화시킨 결과 1.1%에서 3.5% 사이에서 낮은값을 나타내었다. 본 연구결과를 통하여 측정환경에 따라 결과값을 적절히 환산인자로 활용한다면 유리선량계를 이용한 전자선치료빔 선량평가가 가능하리라 사료된다.

Development of Meander-shaped Metallic Magnetic Calorimeters

  • Yoon, W.S.;Jang, Y.S.;Kim, G.B.;Lee, H.J.;Lee, J.Y.;Lee, M.K.;Kim, Y.H.
    • Progress in Superconductivity
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    • 제14권2호
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    • pp.102-105
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    • 2012
  • We are developing meander-shaped metallic magnetic calorimeters using micro-fabrication methods. A planar Nb coil in a meander shape was fabricated on a Si substrate. The coil was designed to have a persistent current using a metal heater evaporated on a part of the coil. A paramagnetic sensor, $5{\mu}m$ thick Au:Er foil, was glued on top of the meander structure with epoxy. The magnetization and heat capacity were measured at different temperatures, and applied field currents matched well with expected values. The detector showed an energy resolution of 4 keV FWHM for the 5.5 MeV alpha particles.

X-Ray Absorption Spectroscopic Study of 120 MeV $Ag^{9+}$ Ion-Irradiated N-Doped ZnO Thin Films

  • Gautam, Sanjeev;Lim, Weon Cheol;Kang, Hee Kyung;Lee, Ki Soo;Song, Jaebong;Song, Jonghan;Asokan, K.;Chae, Keun Hwa
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2013년도 제44회 동계 정기학술대회 초록집
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    • pp.315-315
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    • 2013
  • We report the electronic structure modification in the swift heavy ion (SHI) irradiated N-doped ZnO thin films prepared by RF sputtering from ZnO target in different ratio of Ar/$N_2$ gas mixture using highly pure $N_2$ gas. The different N-ZnO thin lms were then irradiated with 120 MeV Ag ion beam with different doses ranging from $1{\times}10^{11}$ to $5{\times}10^{12}$ ions/$cm^2$ and characterized by XRD and near edge X-ray absorption ne structure (NEXAFS) at N and O K-edges. The NEXAFS measurements provide direct evidence of O 2p and Zn 3d orbital hybridization and also the bonding of N ions with Zn and O ions. The minimum value of resistivity of $790{\Omega}cm$, a Hall mobility of $22cm^2V^-1s^-1$ and the carrier concentration of $3.6{\times}10^{14}cm^{-3}$ were yielded at 75% $N_2$. X-ray diffraction (XRD) measurements revealed that N-doped ZnO films had the preferential orientation of (002) plane for all samples, while crystallinity start decreasing at 32.5% $N_2$. The average crystallite size varies from 5.7 to 8.2 nm for 75% and then decreases to 7.8 nm for 80% $Ar:N_2$ ratio.

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MC-50 싸이클로트론을 이용한 $^{123}I$ 제법 연구 (The Development of Iodine-123 with MC-50 Cyclotron)

  • 서용섭;양승대;전권수;이종두;한현수
    • 대한핵의학회지
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    • 제25권2호
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    • pp.286-293
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    • 1991
  • $^{123}I$, which is applied for the thyroid and other in vivo kinetic study, has a special role in life sciences. The 159 KeV $\gamma-ray$ from $^{123}I$ is almost ideally appropriate for the current imaging instrumentation. Its decay mode (electron capture) and short half-life (13.3 hr) reduced the burden of radiation dose to the patients, and its chemical property makes it easy to synthesize the labelling compounds. In this experiment, the production of $^{123}I$ via the nuclear reaction $^{124}Te(p,2n)^{123}I$ with 28 MeV protons was sutdied. $TeO_2$ is used as a target material, because it has good physical properties. The target was prepared with $TeO_2$ powder and was molten into a ellipsoidal cavity (a=14 mm, b=10 mm, $270.8mg/cm^2$ thick) of pure platinum. The irradiation was carried out in the external proton beam with incident energies range from 28 MeV to 22 MeV, and current was $30{\mu}A$. The loss of $TeO_2$ target was significantly reduced by using $4\pi-cooling$ system in irradiation. The dry distillation method was adopted for the separation of $^{123}I$ from irradiated target, and when it was kept 5 minutes at $780^{\circ}C$, its result was quantitative. The loss of the target material $(TeO_2)$ was below 0.2% for each production run and $^{123}I$ from the dry distillation apparatus was captured with 0.01 N NaOH in $Na^{123}I$ form, then the pH of the solution was adjusted to $7.5\sim9.0$ with HC1/NaOH. The $Na^{123}I$ solution was passed through $0.2{\mu}m$ membrane filter, and sterilized under high pressure and temperature for 30 minutes. The production of $^{123}I$ is acceptable for clinical application based on the quality of USP XXI.

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방사선 치료용 고에너지 전자선의 조직 내 선량분포 특성에 관한 연구 (Study on Characteristics of Dose Distribution in Tissue of High Energy Electron Beam for Radiation Therapy)

  • 나수경
    • 대한방사선치료학회지
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    • 제14권1호
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    • pp.175-186
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    • 2002
  • The purpose of this study is directly measure and evaluate about absorbed dose change according to nominal energy and electron cone or medical accelerator on isodose curve, percentage depth dose, contaminated X-ray, inhomogeneous tissue, oblique surface and irradiation on intracavitary that electron beam with high energy distributed in tissue, and it settled standard data of hish energy electron beam treatment, and offer to exactly data for new dote distribution modeling study based on experimental resuls and theory. Electron beam with hish energy of $6{\sim}20$ MeV is used that generated from medical linear accelerator (Clinac 2100C/D, Varian) for the experiment, andwater phantom and Farmer chamber md Markus chamber und for absorbe d dose measurement of electron beam, and standard absorbed dose is calculated by standard measurements of International Atomic Energy Agency(IAEA) TRS 277. Dose analyzer (700i dose distribution analyzer, Wellhofer), film (X-OmatV, Kodak), external cone, intracavitary cone, cork, animal compact bone and air were used for don distribution measurement. As the results of absorbed dose ratio increased while irradiation field was increased, it appeared maximum at some irradiation field size and decreased though irradiation field size was more increased, and it decreased greatly while energy of electron beam was increased, and scattered dose on wall of electron cone was the cause. In percentage depth dose curve of electron beam, Effective depth dose(R80) for nominal energy of 6, 9, 12, 16 and 20 MeV are 1.85, 2.93, 4.07, 5.37 and 6.53 cm respectively, which seems to be one third of electron beam energy (MeV). Contaminated X-ray was generated from interaction between electron beam with high energy and material, and it was about $0.3{\sim}2.3\%$ of maximum dose and increased with increasing energy. Change of depth dose ratio of electron beam was compared with theory by Monte Carlo simulation, and calculation and measured value by Pencil beam model reciprocally, and percentage depth dose and measured value by Pencil beam were agreed almost, however, there were a little lack on build up area and error increased in pendulum and multi treatment since there was no contaminated X-ray part. Percentage depth dose calculated by Monte Carlo simulation appeared to be less from all part except maximum dose area from the curve. The change of percentage depth dose by inhomogeneous tissue, maximum range after penetration the 1 cm bone was moved 1 cm toward to surface then polystyrene phantom. In case of 1 cm and 2 cm cork, it was moved 0.5 cm and 1 cm toward to depth, respectively. In case of air, practical range was extended toward depth without energy loss. Irradiation on intracavitary is using straight and beveled type cones of 2.5, 3.0, 3.5 $cm{\phi}$, and maximum and effective $80\%$ dose depth increases while electron beam energy and size of electron cone increase. In case of contaminated X-ray, as the energy increase, straight type cones were more highly appeared then beveled type. The output factor of intracavitary small field electron cone was $15{\sim}86\%$ of standard external electron cone($15{\times}15cm^2$) and straight type was slightly higher then beveled type.

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Fingerprint of Carcinogenic Semi-Volatile Organic Compounds (SVOCs) during Bonfire Night

  • Pongpiachan, Siwatt
    • Asian Pacific Journal of Cancer Prevention
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    • 제14권5호
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    • pp.3243-3254
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    • 2013
  • It is well known that increased incidences of lung, skin, and bladder cancers are associated with occupational exposure to PAHs. Animal studies show that certain PAHs also can affect the hematopoietic and immune systems and can produce reproductive, neurologic, and developmental effects. As a consequence, several studies have been attempted to investigate the fate of PAHs in atmospheric environment during the past decades. However, there is still a lack of information in regard to the atmospheric concentration of PAHs during the "Bon Fire Night". In this study, twenty-three polycyclic aromatic hydrocarbons and twenty-eight aliphatics were identified and quantified in the $PM_{10}$ and vapour range in Birmingham ($27^{th}$ November 2001-$19^{th}$ January 2004). The measured concentrations of total particulate and vapour (P+V) PAHs were consistently higher at the BROS in both winter and summer. Arithmetic mean total (P+V) PAH concentrations were $51.04{\pm}47.62$ ng $m^{-3}$ and $22.30{\pm}19.18$ ng $m^{-3}$ at the Bristol Road Observatory Site (BROS) and Elms Road Observatory Site (EROS) respectively. In addition arithmetic mean total (P+V) B[a]P concentrations at the BROS were $0.47{\pm}0.39$ ng $m^{-3}$ which exceeded the EPAQS air quality standard of 0.25 ng $m^{-3}$. On the other hand, the arithmetic mean total (P+V) aliphatics were $81.80{\pm}69.58$ ng $m^{-3}$ and $48.00{\pm}35.38$ ng $m^{-3}$ at the BROS and EROS in that order. The lowest average of CPI and $C_{max}$ measured at the BROS supports the idea of traffic emissions being a principle source of SVOCs in an urban atmosphere. The annual trend of PAHs was investigated by using an independent t-test and oneway independent ANOVA analysis. Generally, there is no evidence of a significant decline of heavier MW PAHs from the two data sets, with only Ac, Fl, Ph, An, 2-MePh, 1+9-MePh, Fluo and B[b+j+k]F showing a statistically significant decline (p<0.05). A further attempt for statistical analysis had been conducted by dividing the data set into three groups (i.e. 2000, 2001-2002 and 2003-2004). For lighter MW compounds a significant level of decline was observed by using one-way independent ANOVA analysis. Since the annual mean of $O_3$ measured in Birmingham City Centre from 2001 to 2004 increased significantly (p<0.05), it may be possible to attribute the annul reduction of more volatile PAHs to the enhanced level of annual average $O_3$. By contrast, the heavier MW PAHs measured at the BROS did not show any significant annual reduction, implying the difficulties of 5- and 6-ring PAHs to be subject to photochemical decomposition. The deviation of SVOCs profile measured at the EROS was visually confirmed during the "Bonfire Night" festival closest to the $6^{th}$ November 2003. In this study, the atmospheric PAH concentrations were generally elevated on this day with concentrations of Fl, Ac, B[a]A, B[b+j+k]F, Ind and B[g,h,i]P being particularly high.

Three-dimensional morphometric analysis of mandibule in coronal plane after bimaxillary rotational surgery

  • Lee, Sung-Tak;Choi, Na-Rae;Song, Jae-Min;Shin, Sang-Hun
    • Maxillofacial Plastic and Reconstructive Surgery
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    • 제38권
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    • pp.49.1-49.9
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    • 2016
  • Background: The aim of this report is to present a new reference for aesthetic mandible surgery using three-dimensional cone-beam computed tomography-based treatment planning for orthognathic surgery which can be implemented in surgical planning and perioperative procedure. Methods: To make an objective standard for evaluating aesthetic mandibular outline, we make an aesthetic scoring criteria with consideration of asymmetry, broad mandibular border line, and prominent mandibular angle. Two maxillofacial surgeons and two orthodontists rated their aesthetical evaluation from 1 to 5. Experimental group consisting of 47 female and 38 male patients who had rotational orthognathic two-jaw surgery from 2010 to 2011 were chosen according to aesthetic scoring done by two maxillofacial surgeons and two orthodontists. A high aesthetic score (${\geq}16$) means the facial contour is symmetric, with no broad and narrow aesthetic mandible frontal profiles. Control A group consisted of ten female and ten male patients who had no orthognathic surgery experience and low aesthetic score (${\geq}10$). Control B group consisted of ten female and ten male patients who had no orthognathic surgery experience and had anaesthetic mandibular frontal profile and a high aesthetic score (${\geq}16$). The three-dimensional image of the patient was taken from dental cone-beam CT (DCT) scanning (experimental group and control A group: 6 months DCT after surgery, control B group: 1st visit DCT). Each DCT was reformatted to reorient the 3D image using 3D analyzing program (OnDemand3D, cybermed Inc, CA, USA). After selection of 12 landmarks and the construction of reoriented horizontal, vertical, and coronal reference lines, 15 measurements were taken in 3D analysis of frontal mandibular morphology. Afterwards, horizontal and vertical linear measurements and angular measurements, linear ratio were obtained. Results: Mean $Go^{\prime}_{Rt}-Me^{\prime}-Go^{\prime}_{Lt}$ angular measurement was $100.74{\pm}2.14$ in female patients and $105.37{\pm}3.62$ in male patients. These showed significant difference with control A group in both genders. Ratio of $Go^{\prime}_{Rt}-Go^{\prime}_{Lt}-Me^{\prime}$ length to some linear measurements (ratio of $Me^{\prime}-Cd^{\prime}_{Rt}Cd^{\prime}_{Lt}$ to $Me^{\prime}-Go^{\prime}_{Rt}Go^{\prime}_{Lt}$, ratio of $Me^{\prime}-Go^{\prime}$ to $Me^{\prime}-Go^{\prime}_{Rt}Go^{\prime}_{Lt}$, ratio of $Go^{\prime}_{Rt}-Go^{\prime}_{Lt}$ to $Me^{\prime}-Go^{\prime}_{Rt}Go^{\prime}_{Lt}$) showed significant difference with control A group in both genders. Conclusion: This study was intended to find some standard measurement of mandible frontal view in 3D analysis of aesthetic patient. So, these potential measurement value may be helpful for orthognathic treatment planning to have more aesthetic and perspective outcomes.

Potential Feeding Value of Deoiled Rice Bran by Japanese Quails. 1. The Metabolisable Energy Content

  • Bhanja, S.K.;Verma, S.V.S.
    • Asian-Australasian Journal of Animal Sciences
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    • 제14권5호
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    • pp.680-683
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    • 2001
  • The apparent metabolisable energy (AME) and N-corrected ME (AMEn) of deoiled rice bran (DORB) were determined with adult quails at 6 and 10- week of age. The DORB obtained from two types of extraction process, Batch (DORB-B) and the Continuous (DORB-C), was each included in a practical type of the reference diet at 20 or 40% level. The analysed crude protein, ether extract, total ash, calcium, phosphorus, glucose and starch content of DORB-B and DORB-C were found at 19.0, 0.79, 17.05, 0.11, 1.92, 2.3, 11.22, and 15.02, 1.56, 13.0, 0.40, 2.76, 2.16, 19.0, respectively. The level of inclusion of DORB in diet appeared to exert a significant effect on the AME and AMEn values. When bioassayed at 20% inclusion level the DORB was found to have a significantly (p<0.01) lower value than that obtained at 40% inclusion level. However, no significant effect of age of quails on the AME values of DORB was evident. The ME bioassays with quails gave significantly (p<0.01) higher AME values for DORB-C than DORB-B thereby indicating that the continuous system of solvent extraction of rice bran is superior to the batch system from this point of view. The AME value of DORB predicted from its chemical composition also revealed that the DORB-C contained approximately 15% more energy than that in DORB-B.

CsI:Na 결정 육성과 섬광 특성 (Crystal growth and scintillation properties of CsI:Na)

  • 천종규;김성환;김홍주
    • 센서학회지
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    • 제19권6호
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    • pp.443-448
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    • 2010
  • In this work, the scintillation properties of CsI:Na crystal were investigated as radiation detection sensor. This scintillation material was grown by a 2-zone vertical Bridgman method. Under X-ray excitation the crystal shows a broad emission band between 280 nm and 690 nm wavelength range, peaking at 413 nm. Energy resolution for $^{137}Cs$ 662 keV $\gamma$-rays of the crystal was measured to be 6.9 %(FWHM). At room temperature, the crystal exhibits three exponential decay time components. The fast and major component of scintillation time profile of the crystal emission decays with a 457 ns time constant. Absolute light yield of the crystal was estimated to be 53,000 ph/MeV using LAAPD. The sample crystal shows proportionality of 30 % in the measured energy range from 31 to 1,333 keV. And the $\alpha/\beta$ ratio of the crystal was 0.14.

MBE 성장온도에 따른 GaAs 및 AlGaAs의 전기광학적 특성 (Growth and characterization of GaAs and AlGaAs with MBE growth temperature)

  • Seung Woong Lee;Hoon Young Cho;Eun Kyu Kim;Suk-Ki Min;Jung Ho Park
    • 한국결정성장학회지
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    • 제4권1호
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    • pp.11-20
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    • 1994
  • 분자선에피택시(molecular beam epitaxy)법을 이용하여 GaAs 및 ALGaAs layer를 undoped 반절연(100) GaAs 기판위에 성장하였고, 최적의 성장온도와 성장된 시료에 대한 전기적 및 광학적 특성을 조사 하였다. Undoped GaAs층의 성장에 있어서는 측정결과로 부터 As/Ga의유속비가 약 20, 성장온도가 $570^{\circ}C$일때 12K에서의 Photoluminescence 반폭치(FWHM)가 1.14meV인 결정성이 좋은 시료가 얻어졌으며, p형으로서 carrier 농도가 $1.5{\times}10^{14}cm^{-3}$ 미만이고, Hall 이동도가 300K에서 $579cm^2/V-s$인 양질의 에피층이 얻어졌다. 또한 이들 시료에서는 ODLTS, DLTS측정으로 부터 2개의 hole형 깊은 주위만이 관측되었다. Undoped AlGaAs층의 성장에 있어서는 As/(Ga+Al)의 유속비가 20이고 $60^{\circ}C$의 성장온도에서 표면 morphology와 결정성이 좋은 시료를 성장할 수 있었으며, 0.17~0.85eV에서 8개의 깊은 준위가 관측되엇다. Si이 도핑된 AlGaAs 층의 경우, PL 스펙트럼으로 부터 Si의 도핑효과를 관측할 수 있었으며, Hall 측정으로부터 300K에서 $1.5{\times}10^{16}cm^{-3}$일 때 Hall 이동도가 $2547cm^2/V-s$인 시료를 얻을 수 있었다.

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