• 한국초전도ㆍ저온공학회논문지
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• 제17권3호
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• pp.62-66
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• 2015

The cryostat is designed for the superconducting quadrupole magnets to be used in a heavy-ion accelerator facility. The main accelerator is superconducting linac, which can accelerate a $^{238}U$ beam to 200 MeV/u (Mega electron voltage per nucleon). The cryostat for the magnet employs an innovative design primarily driven by the requirement of the compactness, user-friendliness and reliability. Also, several ancillary requirements such as background field, space restriction due to the beam line and cryostat structure need technical attentions. The development of the cryostat for three quadrupole magnets in the in-flight fragmentation separator is presented in the paper. The concept of cryogenic design is reported and the amount of cryogenic load is estimated by a relevant analysis. The structure of the cryostat to endure the heavy iron yoke including three quadrupole magnets is presented. In addition, the design as well as the performance test of the support link for the cold mass is described.

• Journal of the Korean Association of Oral and Maxillofacial Surgeons
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• 제47권4호
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• pp.315-320
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• 2021

Carbon-ion radiotherapy (CIRT) is on the rise as a treatment choice for malignant tumor. Compared to conventional radiotherapy, particle beams have different physical and biological properties. Particle beam provides a low entry dose, deposits most of the energy at the endpoint of the flight path, and forms an asymptotic dose peak (the "Bragg peak"). Compared to protons, carbon with its larger mass decreases beam scattering, resulting in a sharper dose distribution border. We report a 50-year-old male who underwent CIRT without surgical resection on osteosarcoma of the mandible. After CIRT, the patient's pain was gone, and the malignant mass remained stable with accompanying necrosis. Nine months later, however, magnetic resonance imaging demonstrated progression of the left mandibular osteosarcoma with pulmonary metastases. After multidisciplinary discussion, concurrent chemoradiotherapy was conducted. While necrotic bone segments came out of the mandible during subsequent periodic outpatient visits, the tumor itself was stable. Thirty months after his first visit and diagnosis, the patient is waiting for chemotherapy. Although CIRT is superior in treating radioresistant hypoxic disease, CIRT is in its infancy, so care must be taken for its indications and complications.

• 식물조직배양학회지
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• 제26권4호
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• pp.245-250
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• 1999

수분 후 담배의 배에 중이온 ($^{14}$ N) beam을 조사하여 유도한 variegated담배의 잎 조직을 기내배양하여 재생된 식물체의 특성을 조사하였다. NAA 0.1mg/L 와 BAP 1/0mg/L를 첨가한 MS배지에서 variegated담배의 잎을 배양하면 백색부위에서는 백색 식물체만이 유도되었으나 녹색부위에서는 녹색 식물체가 47.2%, 백색 식물체가 37.4%, variegated식물체가 15.4% 유도되었다. 재생된 녹색 식물체는 자가수분한 후대 (F$_1$)에서 녹색 식물체 1,651 개:백색 식물체 54개로 분리되었다. 또한 variegated 잎에서 재생된 녹색 식물체와 정상주를 정역교배 한 결과, 전부 녹색체가 분리되었다. 이 결과는 variegated잎의 표현형 유전은 최소한 모성 유전이 아님을 보여준다. Variegated잎의 녹색부위를 배양하여 재생된 variegated식물체의 잎을 이용하여 DNA gel blot한 결과, 엽록체 유전자인 psbA, rbcL, 165 rDNA, 23S rDNA의 양은 흰색부위 잎에서 정상주인 녹색 잎과 variegated식물체 잎의 녹색부위 보다 많았다.

• 대한방사선기술학회지:방사선기술과학
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• 제44권4호
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• pp.359-365
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• 2021

A heavy particle accelerator is a device that accelerates particles using high energy and is used in various fields such as medical and industrial fields as well as research. However, secondary neutrons and particle fragments are generated by the high-energy particle beam, and among them, the neutrons do not have an electric charge and directly interact with the nucleus to cause radiation of the material. Quantitative evaluation of the radioactive material produced in this way is necessary, but there are many difficulties in actual measurement during or after operation. Therefore, this study compared and evaluated the generated radioactive material in the concrete shield for protons and carbon ions of specific energy by using the simulation code FLUKA. For the evaluation of each energy of proton beam and carbon ion, the reliability of the source term was secured within 2% of the relative error with the data of the NASA Space Radiation Laboratory(NSRL), which is an internationally standardized data. In the evaluation, carbon ions exhibited higher neutron flux than protons. Afterwards, in the evaluation of radioactive materials under actual operating conditions for disposal, a large amount of short-lived beta-decay nuclides occurred immediately after the operation was terminated, and in the case of protons with a high beam speed, more radioactive products were generated than carbon ions. At this time, radionuclides of ⁴⁴Sc, ³H and ²²Na were observed at a high rate. In addition, as the cooling time elapsed, the ratio of long-lived nuclides increased. For nonparticulate radionuclides, ³H, ²²Na, and for particulate radionuclides, ⁴⁴Ti, ⁵⁵Fe, ⁶⁰Co, ¹⁵²Eu, and ¹⁵⁴Eu nuclides showed a high ratio. In this study, it is judged that it is possible to use the particle accelerator as basic data for facility maintenance, repair and dismantling through the prediction of radioactive materials in concrete according to the cooling time after operation and termination of operation.

• IEIE Transactions on Smart Processing and Computing
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• 제4권6호
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• pp.384-390
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• 2015

There are two main artifacts in reconstructed images from in-beam positron emission tomography (PET). Unlike generic PET, in-beam PET uses the annihilation photons that occur during heavy ion therapy. Therefore, the geometry of in-beam PET is not a full ring, but a partial ring that has one or two openings around the rings in order for the hadrons to arrive at the tumor without prevention of detector blocks. This causes truncation in the projection data due to an absence of detector modules in the openings. The other is a ring artifact caused by the gaps between detector modules also found in generic PET. To sum up, in-beam PET has two kinds of gap: openings for hadrons, and gaps between the modules. We acquired three types of simulation results from a PET system: full-ring, C-ring and dual head. In this study, we aim to compensate for the artifacts that come from the two types of gap. In the case of truncation, we propose a method that uses prior knowledge of the location where annihilations occur, and we applied the discrete-cosine transform (DCT) gap-filling method proposed by Tuna et al. for inter-detector gap.

• Nuclear Engineering and Technology
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• 제56권5호
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• pp.1754-1761
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• 2024

In hadrontherapy, secondary fragments are generated by nuclear interactions of the incident heavy ion beam with the atomic nuclei of the target. It is important to determine the yield of production and the dose contribution of these secondary fragments in order to determine the radiobiological effectiveness more accurately. This work aims to fully identify the secondary fragments generated by nuclear interactions of proton and helium (⁴He) ion beams in a High-Density Polyethylene (HDPE) target and to investigate the dose contributions by secondary fragments. Incident protons with energies of 55.90 MeV and 105.20 MeV and helium ions with energies of 52.55 MeV/u and 103.50 MeV/u in the HDPE phantom have been investigated by the means of Geant4 Monte Carlo (MC) simulations. Simulated results were validated using NASA Space Radiation Laboratory (NSRL) Bragg curves experimental data. The results showed that the dose contribution of secondary fragments deriving from helium ion beams is three times higher than in the case of proton beams. This is due to a higher production of nuclear fragments in the case of helium ion beams. This work contributes to a better understanding of secondary fragments generated by protons and helium ions in the HDPE target.

• Nuclear Engineering and Technology
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• 제55권3호
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• pp.919-926
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• 2023

To analyze the cause of the destruction of thin, carbon-backed lithium fluoride targets during a measurement of the fusion of ⁷Li and ¹⁷O, we estimate theoretically the lifetimes of carbon and LiF films due to sputtering, thermal evaporation, and lattice damage and compare them with the lifetime observed in the experiment. Sputtering yields and thermal evaporation rates in carbon and LiF films are too low to play significant roles in the destruction of the targets. We estimate the lifetime of the target due to lattice damage of the carbon backing and the LiF film using a previously reported model. In the experiment, elastically scattered target and beam ions were detected by surface silicon barrier (SSB) detectors so that the product of the beam flux and the target density could be monitored during the experiment. The areas of the targets exposed to different beam intensities and fluences were degraded and then perforated, forming holes with a diameter around the beam spot size. Overall, the target thickness tends to decrease linearly as a function of the beam fluence. However, the thickness also exhibits an increasing interval after SSB counts per beam ion decreases linearly, extending the target lifetime. The lifetime of thin LiF film as determined by lattice damage is calculated for the first time using a lattice damage model, and the calculated lifetime agrees well with the observed target lifetime during the experiment. In experiments using a thin LiF target to induce nuclear reactions, this study suggests methods to predict the lifetime of the LiF film and arrange the experimental plan for maximum efficiency.

• 한국식물생명공학회:학술대회논문집
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• 한국식물생명공학회 2003년도 식물바이오벤처 페스티발
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• pp.156-156
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• 2003

• 한국식물생명공학회:학술대회논문집
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• 한국식물생명공학회 2003년도 추계학술대회 발표논문 초록집
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• pp.126-126
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• 2003

• 한국의학물리학회지:의학물리
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• 제26권1호
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• pp.12-17
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• 2015

본 연구에서 한국형 중이온 가속기 RAON에서의 의생물 실험을 위하여 요구되는 빔 조건을 만족할 수 있도록 Monte Carlo 전산모사를 통한 노즐 설계를 최적화하고자 하였다. 의생명 실험을 위한 빔 조건으로 최대 조사면 크기, 선량균일도 그리고 빔 오염도의 특정 조건을 만족하는 $C^{12}$ 빔 생산이 요구되었다. 이때 최적화된 빔 노즐 설계를 위하여 Monte Carlo 시뮬레이션인 GEANT4 toolkit이 사용되었다. $15{\times}15cm^2$ 이상의 빔 조사면 크기와 3% 이내의 선량 균일도 그리고 전체 선량의 5% 보다 낮은 빔 오염도를 기본적인 조건으로 설정 되었다. 조사면 크기는 쌍극자 자석에 의해서 빔의 각도를 기울여 원형으로 회전하면서 쌍극자 자석의 아래쪽에 위치한 산란판의 두께를 조정하여 최적화 하였다. 빔 스캐닝 각도와 산란판의 두께는 Monte Carlo 시뮬레이션 분석에 의해서 각각 $0.5^{\circ}$와 0.05 cm로 최적의 값을 나타내었다. 선량 균일도와 최대 조사면 크기를 만족하기 위하여 static과 scanning beam을 복합하는 기술을 이용한 새로운 빔 전달 방법을 소개하였다. 중앙 고정용 빔과 빔 축으로부터 $0.5^{\circ}$ 경사각을 가지고 회전하는 빔과 경사각이 없이 바로 들어오는 빔을 조합하여 선량균일도가 1.1%와 빔 조사면의 최대크기가 $15{\times}15cm^2$가 되는 것을 확인하였다. 빔 오염도는 $C^{12}$ 이온과 다른 입자들에 의해서 전달된 흡수선량의 비율로 나타내었다. 물등가 깊이(water equivalent depth) 5 cm에서 17 cm 사이에서의 빔 오염도는 전체 선량에서의 2.5% 미만임을 확인하였으며 이와 같은 결과를 바탕으로, 본 연구에서는 의생명 실험을 위하여 요구되는 빔 조건을 만족하는 노즐 구조를 설정할 수 있었다.