• Title/Summary/Keyword: Flattening Filter

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Characteristics of Scattered Rays Depending on the Use of a Flattening Filter (선속평탄 여과판 사용 유무에 따른 산란선 특성)

  • Jin, SeongJin;Park, ChulWoo;Je, Jaeyong
    • Journal of the Korean Society of Radiology
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    • v.10 no.1
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    • pp.15-19
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    • 2016
  • This Study aims at measuring scattered rays depending on the use of a flattening filter when radiation is irradiated using a linear accelerator. measurement of the scattered rays, an ionization chamber was used, and the energy of the irradiated radiation was 6 MV and 10 MV. The ionization chamber was located at the spot 15 cm, 25 cm, 35 cm and 45 cm far away from the center of gantry rotation, and the scattered rays were measured according to whether a flattening filter was used or not and to the distance. As the result of investigation of 100 cGy about each energy, when the flattening filter was not used with 6 MV, it occurred at a low level of 65%, and with 10 MV at that of 55%. In other words, it's been concluded that when a flattening filter is not used for radiation dose of the parts around the critical organ, scattered rays generate in a small quantity, and it's a useful way to decrease the stochastic effect of radiation.

A Study on the Photoneutron Dose Estimation in Flattening Filter Mode and Flattening Filter Free Mode for Medical Linear Accelerator (의료용 선형가속기의 Flattening Filter Mode와 Flattening Filter Free Mode 간에 광중성자 선량 평가)

  • Yang, Oh Nam;Lim, Cheong Hwan
    • Journal of radiological science and technology
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    • v.40 no.2
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    • pp.297-302
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    • 2017
  • In this study, the generation of photoneutrons between the 10 MV FF mode and the FFF mode was evaluated and the amount of photoneutrons generated by the 10 MV and 15 MV energy changes in the FFF mode was evaluated. The generated neutrons were evaluated at 13 measurement points and the KTEPC was used to collect the generated neutrons. 10 MV FF mode was measured at 10 MV FF mode and FFF mode at all measurement points. In the superior direction, 0.455mSv and 0.152mSv were the largest, and more than 33% optical neutron was generated in FF. 10 MV in FFF mode, 15 MV in 15 MV, and 0.402 mSv in the direction of Superior, and 6.9% in the direction.

A Study on the Estimation of Glottal Spectrum Slope Using the LSP (Line Spectrum Pairs) (LSP를 이용한 성문 스펙트럼 기울기 추정에 관한 연구)

  • Min, So-Yeon;Jang, Kyung-A
    • Speech Sciences
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    • v.12 no.4
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    • pp.43-52
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    • 2005
  • The common form of pre-emphasis filter is $H(z)\;=\;1\;- az^{-1}$, where a typically lies between 0.9 and 1.0 in voiced signal. Also, this value reflects the degree of filter and equals R(1)/R(0) in Auto-correlation method. This paper proposes a new flattening algorithm to compensate the weaked high frequency components that occur by vocal cord characteristic. We used interval information of LSP to estimate formant frequency. After obtaining the value of slope and inverse slope using linear interpolation among formant frequency, flattening process is followed. Experimental results show that the proposed algorithm flattened the weaked high frequency components effectively. That is, we could improve the flattened characteristics by using interval information of LSP as flattening factor at the process that compensates weaked high frequency components.

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The design of the EDEA gain flattening filter using an asymmetrical directional coupler (비대칭 구조의 커플러를 이용한 EDFA 이득평탄필터 설계)

  • 조준용;이경식
    • Korean Journal of Optics and Photonics
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    • v.13 no.5
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    • pp.373-376
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    • 2002
  • An asymmetrical directional coupler with two nonidentical fibers has, for the first time, been proposed and analyzed for an EDFA gain flattening filter (GFF). The characteristics of the transmission spectra of the GFFs have been theoretically investigated for the core spacings, the coupling lengths and the fiber parameters of the asymmetrical directional coupler. The analytical results show that an EDFA gain spectrum with flatness of ~7 ㏈ can be flattened to within $\pm$0.75 ㏈ over a bandwidth of 30 nm by using the asymmetrical directional coupler-based GFF.

A study of Curved Dosimeter for Flattening Filter Free Beam Quality Assurance Evaluation using Curved Dosimeter in Radiotherapy (Flattening Filter Free Beam의 정도관리를 위한 곡면선량계 가능성 연구)

  • Han, Moojae;Shin, Yohan;Jung, Jaehoon;Heo, Seunguk;Kim, Kyotae;Heo, Yeji;Cho, Heunglae;Park, Sungkwang
    • Journal of the Korean Society of Radiology
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    • v.13 no.1
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    • pp.119-124
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    • 2019
  • Radiation therapy using flattening filter free beam can prevent beam attenuation caused by flattening filter and can improve treatment efficiency. However, accurate dose control is not established for nonuniform iso dose distributions. In this study, curved dosimeter based on photoconductive material $HgI_2$ was fabricated and its reproducibility and linearity were evaluated at 6 MV photon energy to verify its performance. In order to show the usefulness of the curved measurement, the signals measured on the flat substrate and the curved substrate were compared in the flattening filter free beam using the acrylic filter. As a result, the reproducibility of the unit cell dosimeter was evaluated as SE 0.613%, and the linearity was evaluated as R-sq 0.9999. The usability evaluation of the array curve dosimeter demonstrated its usefulness by indicating a curvature error rate of 11.073%p and a reduced error rate.

THE NEW GAIN FLATTENING FILTERS USING PERIODIC TAPERED FIBER

  • G.H Yang;Park, G.T;Park, Y.B
    • Proceedings of the Optical Society of Korea Conference
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    • 2003.07a
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    • pp.24-25
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    • 2003
  • We propose the new gain-flattened filter utilizing tapered silica-based fiber for high capacity WDM optical communication systems. The gain excursion of Gain flattening filters is less than 0.5 dB over the 40 nm(1525 nm ~1565 nm).

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The Flattening Algorithm of Speech Spectrum by Quadrature Mirror Filter (QMF에 의한 음성스펙트럼의 평탄화 알고리즘)

  • Min, So-Yeon
    • Journal of the Korea Academia-Industrial cooperation Society
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    • v.7 no.5
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    • pp.907-912
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    • 2006
  • Pre-emphasizing the speech compensates for falloff at high frequencies. The most common form of pre-emphasis is y(n)=s(n)-A${\cdot}$s(n-1), where A typically lies between 0.9 and 1.0 in voiced signal. And, this value reflects the degree of pre-emphasis and equals R(1)/R(0) in conventional method. This paper proposes a new flattening method to compensate the weaked high frequency components that occur by vocal cord characteristic. We used QMF(Quardrature Mirror Filter) to minimize the output signal distortion. After using the QMF to compensate high frequency components, flattening process is followed by R(1)/R(0) at each frame. Experimental results show that the proposed method flattened the weaked high frequency components effectively than auto correlation method. Therefore, the flattening algorithm will apply in speech signal processing like speech recognition, speech analysis and synthesis.

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The evaluation of properties for radiation therapy techniques with flattening filter-free beam and usefulness of time and economy to a patient with the radiation therapy (Flattening filter-free beam을 이용한 방사선 치료 기법의 특성 및 환자의 시간적.경제적 유용성 평가)

  • Goo, Jang Hyeon;Won, Hui Su;Hong, Joo Wan;Chang, Nam Jun;Park, Jin Hong
    • The Journal of Korean Society for Radiation Therapy
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    • v.26 no.2
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    • pp.363-368
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    • 2014
  • Purpose : The aim of this study was to appraise properties for radiation therapy techniques and effectiveness of time and economy to a patient in the case of applying flattening filter-free (3F) and flattening filter (2F) beam to the radiation therapy. Materials and Methods : Alderson rando phantom was scanned for computed tomography image. Treatment plans for intensity modulated radiation therapy (IMRT), volumetric modulated arc therapy (VMAT) and stereotactic body radiation therapy (SBRT) with 3F and 2F beam were designed for prostate cancer. To evaluate the differences between the 3F and 2F beam, total monitor units (MUs), beam on time (BOT) and gantry rotation time (GRT) were used and measured with $TrueBeam^{TM}$ STx and Surveillance And Measurement (SAM) 940 detector was used for photoneutron emitted by using 3F and 2F. To assess temporal and economical aspect for a patient, total treatment periods and medical fees were estimated. Results : In using 3F beam, total MUs in IMRT plan increased the highest up to 34.0% and in the test of BOT, GRT and photoneutron, the values in SBRT plan decreased the lowest 39.8, 38.6 and 48.1%, respectively. In the temporal and economical aspect, there were no differences between 3F and 2F beam in all of plans and the results showed that 10 days and 169,560 won was lowest in SBRT plan. Conclusion : According as the results, total MUs increased by using 3F beam than 2F beam but BOT, GRT and photoneutron decreased. From above the results, using 3F beam can decrease intra-fraction setup error and risk of radiation-induced secondary malignancy. But, using 3F beam did not make the benefits of temporal and economical aspect for a patient with the radiation therapy.

A Study on IMRT (Intensity Modulated Radiation Therapy) Delivery Technique and FFF (Flattening Filter Free) Beam to Increase Skin Dose to Irregularly Shaped Skin Surface. (IMRT(Intensity Modulated Radiation Therapy)전달 기법과 FFF(Flattening Filter Free) 빔을 이용한 요철 부위 피부 선량 증가 방법에 대한 고찰)

  • Woo Heon;Son Sang Jun;Je Young Wan
    • The Journal of Korean Society for Radiation Therapy
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    • v.34
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    • pp.7-12
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    • 2022
  • Purpose: When it is difficult to secure the skin dose when treating Irregularly Shaped Skin Surface such as the nose where it is difficult to apply a bolus, increase the skin dose with a treatment plan that combines the IMRT (Intensity Modulated Radiation Therapy) delivery technique and FFF (Flattening Filter Free), It was tried to find out whether or not through the phantom experiment. Materials & Methods: Based on the 6MV-FF (Flattening Filter) and VMAT (Volumetric-Modulated Arc Therapy) treatment plans, which are the most commonly used treatment plans for head and neck cancer, A comparison group was created by combining VMAT and IMRT, FF and FFF, and the presence or absence of 5 mm bolus application. A virtual target was created on the Rando Phantom's nose, and a virtual bolus of 5 mm was applied assuming full contact on the Rando Phantom's nose. Five measurement points were determined based on the phantom's nose, and the absorbed dose was measured by irradiating each treatment plan 3 times per treatment plan according to the treatment technique and whether or not the bolus was applied. Result: The difference in skin dose in FF vs FFF increased in the case of FFF in VMAT bolus off, and there was no difference in case of IMRT bolus off. In VMAT bolus 5 mm and IMRT bolus 5 mm, it was confirmed that the skin dose was rather decreased in FFF. The difference in skin dose between VMAT and IMRT increased only in the case of FFF bolus off, and there was no statistical difference in the rest. For the difference in skin dose between bolus off vs bolus 5 mm, it was confirmed that the skin dose increased at bolus 5 mm, except for the case of using IMRT FFF. The treatment plan combining IMRT and FFF did not find any statistically significant difference as a result of analyzing the measured values of the treatment plan skin dose applied with a 5 mm bolus using the commonly used VMAT and FF. Therefore, it is thought that by using IMRT_FFF, it is possible to deliver a skin dose similar to that of applying a 5 mm bolus to VMAT_FF, which can be useful for patients who need a high skin dose but have difficulty applying a bolus. Conclusion: For patients who find it difficult to apply bolus, an increase in skin dose can be expected with a treatment plan that properly combines IMRT and FFF compared to VMAT and FF.

THE NEW GAIN FLATTENING FILTERS USING PERIODIC TEPERED FIBER

  • Choi Young-Bok;Cho Sung-Hyun;Oh Min-Chul;Kim Sang-In;Jeong Gi-Tae;Han Kwan-Hoon
    • 한국정보통신설비학회:학술대회논문집
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    • 2003.08a
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    • pp.42-43
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    • 2003
  • We propose the new gain-flattened filter utilizing tapered silica-based fiber for high capacity WDM optical communication systems. The gain excursion of Gain flattening filters is less than 0.5 dB over the 40 nm($1525nm{\sim}1565nm$).

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