• Title/Summary/Keyword: parallel beam

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Development of Monitor Chamber Prototype and Basic Performance Testing (모니터 전리함 시작품 개발과 기초 성능 평가)

  • Lee, Mujin;Lim, Heuijin;Lee, Manwoo;Yi, Jungyu;Rhee, Dong Joo;Kang, Sang Koo;Jeong, Dong Hyeok
    • Progress in Medical Physics
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    • v.26 no.2
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    • pp.99-105
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    • 2015
  • The monitor chamber is a real time dosimetry device for the measurement and the control of radiation beam intensity of the linac system. The monitor chamber prototype was developed for monitoring and controlling radiation beam from the linac based radiation generator. The thin flexible printed circuit boards were used for electrodes of the two independent plane-parallel ionization chambers to minimize the attenuation of radiation beam. The dosimetric characteristics, saturation and linearity of the measured charge, were experimentally evaluated with the Co-60 gamma rays. The performance of the developed monitor chamber prototype was in an acceptable range and this study shows the possibility of the further development of the chamber with additional functions.

Radiomorphometric analysis of edentulous posterior mandibular ridges in the first molar region: a cone-beam computed tomography study

  • Magat, Guldane
    • Journal of Periodontal and Implant Science
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    • v.50 no.1
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    • pp.28-37
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    • 2020
  • Purpose: The aim of our study was to determine the prevalence and degree of lingual concavities in the first molar region of the mandible to reduce the risk of perforating the lingual cortical bone during dental implant insertion. Methods: A total of 163 suitable cross-sectional cone-beam computed tomography images of edentulous mandibular first molar regions were evaluated. The mandibular morphology was classified as a U-configuration (undercut), a P-configuration (parallel), or a C-configuration (convex), depending on the shape of the alveolar ridge. The characteristics of lingual concavities, including their depth, angle, vertical location, and additional parameters, were measured. Results: Lingual undercuts had a prevalence of 32.5% in the first molar region. The mean concavity angle was 63.34°±8.26°, and the mean linear concavity depth (LCD) was 3.03±0.99 mm. The mean vertical distances of point P from the alveolar crest (Vc) and from the inferior mandibular border were 9.39±3.39 and 16.25±2.44, respectively. Men displayed a larger vertical height from the alveolar crest to 2 mm coronal to the inferior alveolar nerve (Vcb) and a wider LCD than women (P<0.05). Negative correlations were found between age and buccolingual width at 2 mm apical to the alveolar crest, between age and Vcb, between age and Vc, and between age and LCD (P<0.05). Conclusions: The prevalence of lingual concavities was 32.5% in this study. Age and gender had statistically significant effects on the lingual morphology. The risk of lingual perforation was higher in young men than in the other groups analyzed.

Study on Decoding Strategies in Neural Machine Translation (인공신경망 기계번역에서 디코딩 전략에 대한 연구)

  • Seo, Jaehyung;Park, Chanjun;Eo, Sugyeong;Moon, Hyeonseok;Lim, Heuiseok
    • Journal of the Korea Convergence Society
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    • v.12 no.11
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    • pp.69-80
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    • 2021
  • Neural machine translation using deep neural network has emerged as a mainstream research, and an abundance of investment and studies on model structure and parallel language pair have been actively undertaken for the best performance. However, most recent neural machine translation studies pass along decoding strategy to future work, and have insufficient a variety of experiments and specific analysis on it for generating language to maximize quality in the decoding process. In machine translation, decoding strategies optimize navigation paths in the process of generating translation sentences and performance improvement is possible without model modifications or data expansion. This paper compares and analyzes the significant effects of the decoding strategy from classical greedy decoding to the latest Dynamic Beam Allocation (DBA) in neural machine translation using a sequence to sequence model.

Behaviour and design of stainless steel shear connectors in composite beams

  • Yifan Zhou;Brian Uy;Jia Wang;Dongxu Li;Xinpei Liu
    • Steel and Composite Structures
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    • v.46 no.2
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    • pp.175-193
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    • 2023
  • Stainless steel-concrete composite beam has become an attractive structural form for offshore bridges and iconic high-rise buildings, owing to the superior corrosion resistance and excellent ductility of stainless steel material. In a composite beam, stainless steel shear connectors play an important role by establishing the interconnection between stainless steel beam and concrete slab. To enable the best use of high strength stainless steel shear connectors in composite beams, high strength concrete is recommended. To date, the application of stainless steel shear connectors in composite beams is still very limited due to the lack of research and proper design recommendations. In this paper, a total of seven pushout specimens were tested to investigate the load-slip behaviour of stainless steel shear connectors. A thorough discussion has been made on the differences between stainless steel bolted connectors and welded studs, in terms of the failure modes, load-slip behaviour and ultimate shear resistance. In parallel with the experimental programme, a finite element model was developed in ABAQUS to simulate the behaviour of stainless steel shear connectors, with which the effects of shear connector strength, concrete strength and embedded connector height to diameter ratio (h/d) were evaluated. The obtained experimental and numerical results were analysed and compared with existing codes of practice, including AS/NZS 2327, EN 1994-1-1 and ANSI/AISC 360-16. The comparison results indicated that the current codes need to be improved for the design of high strength stainless steel shear connectors. On this basis, modified design approaches were proposed to predict the shear capacity of stainless steel bolted connectors and welded studs in the composite beams.

Impact of the spatial orientation of the patient's head, metal artifact reduction, and tube current on cone-beam computed tomography artifact expression adjacent to a dental implant: A laboratory study using a simulated surgical guide

  • Matheus Barros-Costa;Julia Ramos Barros-Candido;Matheus Sampaio-Oliveira;Deborah Queiroz Freitas;Alexander Tadeu Sverzut;Matheus L Oliveira
    • Imaging Science in Dentistry
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    • v.54 no.2
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    • pp.191-199
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    • 2024
  • Purpose: The aim of this study was to evaluate image artifacts in the vicinity of dental implants in cone-beam computed tomography (CBCT) scans obtained with different spatial orientations, tube current levels, and metal artifact reduction algorithm (MAR) conditions. Materials and Methods: One dental implant and 2 tubes filled with a radiopaque solution were placed in the posterior region of a mandible using a surgical guide to ensure parallel alignment. CBCT scans were acquired with the mandible in 2 spatial orientations in relation to the X-ray projection plane (standard and modified) at 3 tube current levels: 5, 8, and 11 mA. CBCT scans were repeated without the implant and were reconstructed with and without MAR. The mean voxel and noise values of each tube were obtained and compared using multi-way analysis of variance and the Tukey test(α=0.05). Results: Mean voxel values were significantly higher and noise values were significantly lower in the modified orientation than in the standard orientation (P<0.05). MAR activation and tube current levels did not show significant differences in most cases of the modified spatial orientation and in the absence of the dental implant (P>0.05). Conclusion: Modifying the spatial orientation of the head increased brightness and reduced spatial orientation noise in adjacent regions of a dental implant, with no influence from the tube current level and MAR.

Analysis of Surface Dose Refer to Distance between Beam Spoiler and Patient in Total Body Irradiation (전신방사선조사(Total Body Irradiation) 시 Beam Spoiler와 환자 간의 거리에 관한 고찰)

  • Choi, Jong-Hwan;Kim, Jong-Sik;Choi, Ji-Min;Shin, Eun-Hyuk;Song, Ki-Won;Park, Young-Hwan
    • The Journal of Korean Society for Radiation Therapy
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    • v.19 no.1
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    • pp.51-54
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    • 2007
  • Purpose: Total body irradiation is used to kill the total malignant cell and for immunosuppression component of preparatory regimens for bone-marrow restitution of patients. Beam spoiler is used to increase the dose to the superficial tissues. This paper finds the property of the distance between beam spoiler and patient. Materials and Methods: Set-up conditions are 6 MV-Xray, 300 MU, SAD = 400 cm, field size = $40{\times}40cm^2$. The parallel plate chamber located in surface, midpoint and exit of solid water phantom. The surface dose is measured while the distance between beam spoiler and patient is altered. Because it should be found proper distance. The solid water phantom is fixer and beam spoiler is moving. Results: Central dose of phantom is 10.7 cGy and exit dose is 6.7 cGy. In case of distance of 50 cm to 60 cm between beam spoiler and solid water phantom, incidence dose is $14.58{\sim}14.92cGy$. Therefore, The surface dose was measured $99.4{\sim}101%$ with got near most to the prescription dose. Conclusion: In clinical case, distance between beam spoiler and patient affect surface dose. If once $50{\sim}60cm$ of distance between beam spoiler and patient, surface dose of patient got near prescription dose. It would be taken distance between beam spoiler and patient into account in clinical therapy.

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The Dependence of the Wedge Factor with the Variation of High Energy Photon Beam Fluences (고에너지 광자선의 선속 변화에 따른 쐬기인자의 의존성)

  • 오영기;윤상모;김재철;박인규;김성규
    • Progress in Medical Physics
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    • v.11 no.1
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    • pp.1-18
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    • 2000
  • For wedged photon beams, the variation of the wedge factor with field size was reported by several authors. However, until now such variation with field size had not been explained quantitatively. Therefore, the variation of the wedge factor was investigated by measuring outputs with field sizes increasing from 4 cm $\times$ 4 cm to 25 cm $\times$ 25 cm for open and wedged 6 and 10MV X-ray beams. The relative outputs for wedged fields to 10 cm $\times$ 10 cm have been obtained. The results show the Increase of the wedge factor caused by the change in fluence of high energy Photon beam with field size, up to 8.0% for KD77-6MV X-ray beam. This increase could be explained as a linear function of the irradiated wedge volume except small field size up to about 10 cm. In the cases of the narrow rectangular beam parallel to the wedge direction, the wedge factor decreases slightly with increasing field size up to about 10-15 cm due to a relatively reduced photon fluence from the change of the wedge thickness. We could explain the causes of a wedge factor variation with field size as the fluences of primary photon passed throughout the wedge, contributing to the dose at the central beam axis and that the fluences were affected by the gradient of the wedge with the change of field size. For clinical use, the formula developed to describe the wedge factor variation with field size has been corrected.

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Measurement of Electron Beam Output for the Prototype Compact Linac (콤팩트 전자 선형가속기 시작품의 출력측정에 관한 연구)

  • Kim, Sung-Woo;Kang, Sang Koo;Rhee, Dong Joo;Lim, Heuijin;Lee, Manwoo;Yi, Jungyu;Lee, Mujin;Yang, Kwangmo;Ro, Tae Ik;Jeong, Dong Hyeok
    • Progress in Medical Physics
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    • v.26 no.1
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    • pp.1-5
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    • 2015
  • The C-band compact linear accelerator (linac) is being developed at Dongnam Institute of radiological & Medical Sciences (DIRAMS) for medical and industrial applications. This paper was focused on the output measurement of the electron beam generated from the prototype electron linac. The dose rate was measured in unit of cGy/min per unit pulse frequency according to the IAEA TRS-398 protocol. Exradin-A10 Markus type plane parallel chamber used for the measurement was calibrated in terms of dose to water at the reference depth in water. The beam quality index ($R_{50}$) was determined by the radiochromic film with a solid water phantom approximately due to low energy electrons. As a result, the determined electron beam output was $17.0cGy/(min{\cdot}Hz$. The results were used to monitor the accelerator performance during the development procedure.

Electrical Characteristics of CdS/CdTe Heterojunction Solar Cells (CdS/CdTe 이종접합 태양전지의 전기적특성)

  • Song, Woo-Chang;Lee, Jae-Hyoung;Nam, Jun-Hyun;Park, Yong-Kwan
    • Proceedings of the KIEE Conference
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    • 1995.07c
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    • pp.1174-1177
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    • 1995
  • In this paper, electrical properties CdS/CdTe heterojunction solar cell prepared by electron beam evaporation method were investigated. Crystal structure of CdS films deposited at substrate temperature of $50{\sim}250^{\circ}C$ was hexagonal type with preferential orientation of the (002)plane parallel to the substrate. Optical transmittance of the CdS film is increasing and resistivity is decreasing with increasing subsrate temperature. CdS/CdTe Solar cell characteristics were improved by increasing of substrate and annealing temperature. However, low efficiency due to small Jsc, Voc below 0.3 $mA/cm^2$ and 430 mV are observed. Low efficiency is contributed to be high resistance of CdTe films and contact.

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The effect of substrate temperature on the Characteristics of CdTe thin film (기판온도에 따른 CdTe박막 특성)

  • Lee, Jae-Hyoung;Song, Woo-Chang;Park, Yong-Kwan
    • Proceedings of the KIEE Conference
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    • 1995.07c
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    • pp.1178-1180
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    • 1995
  • In this paper, structual, optical and electrical properties of CdTe thin films prepared by electron beam evaporation method were studied. The crystal structure of CdTe films deposited at substrate temperature of $100{\sim}400^{\circ}C$ was zincblend type with preferential orientation of the (111)plane parallel to the substrate. The result of optical absoption and transmittance show that solar radiation with energy larger than band gap is almost completely absorbed within an about $2{\mu}m$ thickness of the evaporated CdTe layer and optical band gap of the CdTe film was larger with increasing substrate temperature. The resistivity of CdTe films deposited on the glass substrate was about $10^5{\sim}10^7{\Omega}cm$.

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