• Title/Summary/Keyword: CT-Simulator

Search Result 80, Processing Time 0.027 seconds

Consideration of the Effect of Artifact during the Image Guided Radiation Therapy Using the Fiducial Marker (영상 유도 방사선치료 시 Fiducial Marker의 Artifact에 관한 연구)

  • Kim, Jong-Min;Kim, Dae-Sup;Back, Geum-Mun;Kang, Tae-Yeong;Hong, Dong-Ki;Yun, Hwa-Yong;Kwon, Kyeong-Tae
    • The Journal of Korean Society for Radiation Therapy
    • /
    • v.22 no.1
    • /
    • pp.1-10
    • /
    • 2010
  • Purpose: The effect of artifact was analyzed, which occurs from fiducial marker during the liver Image Guided Radiation Therapy (IGRT) using the fiducial marker. Materials and Methods: The size of artifact of fixed fiducial marker and length of mobile fiducial marker locus were measured using the On-Board Imager system (OBI) and CT simulator, and 2D-2D matching and 3D-3D matching were carried out, respectively, and at this time, the coordinates transition value of couch was analyzed. Results: The measurement of fixed fiducial marker artifact size indicated CT 4.90, 8.10, 12.90, 19.70 mm and OBI 5.60, 10.60, 14.70, 29.40 mm based on the reference CT slice thickness of 1.25, 2.50, 5.00, and 10.00 mm. Meanwhile, the measurement of mobile fiducial marker locus length indicated CT 42.00, 43.10, 46.50 mm, and OBI 43.40, 46.00, 49.30 mm. The coordinates transition of 1.00, 2.00, and 8.00 mm occurred between 2D-2D matching and 3D-3D matching. Conclusion: It was confirmed that the therapy error increased during IGRT due to the influence of artifact when CT slice thickness increased. Thus, it may be desirable to acquire the image less than 2.50 mm in slice thickness when IGRT is implemented using the fiducial marker.

  • PDF

Development of an MCNP-Based Cone-Beam CT Simulator (MCNP 기반의 CBCT 전산모사 시스템 개발)

  • Lim, Chang-Hwy;Cho, Min-Kook;Han, Jong-Chul;Youn, Han-Bean;Yun, Seung-Man;Cheong, Min-Ho;Kim, Ho-Kyung
    • Journal of the Korean Society for Nondestructive Testing
    • /
    • v.29 no.4
    • /
    • pp.351-359
    • /
    • 2009
  • We have developed a computer simulator fur cone-beam computed tomography (CBCT) based on the commercial Monte Carlo code, MCNP. All the functions to generate input files, run MCNP, convert output files to image data, reconstruct tomographs were realized in graphical user-interface form. The performance of the simulator was demonstrated by comparing with the experimental data. Although some discrepancies were observed due to the ignorance of the detailed physics in the simulation, such as scattered X-rays and noise in image sensors, the overall tendency was well agreed between the measured and simulated data. The developed simulator will be very useful for understanding the operation and the better design of CT systems.

Accuracy evaluation of treatment plan according to CT scan range in Head and Neck Tomotherapy (두경부 토모테라피 치료 시 CT scan range에 따른 치료계획의 정확성 평가)

  • Kwon, Dong Yeol;Kim, Jin Man;Chae, Moon Ki;Park, Tae Yang;Seo, Sung Gook;Kim, Jong Sik
    • The Journal of Korean Society for Radiation Therapy
    • /
    • v.31 no.2
    • /
    • pp.13-24
    • /
    • 2019
  • Purpose: CT scan range is insufficient for various reasons in head and neck Tomotherapy®. To solve that problem, Re-CT simulation is good because CT scan range affects accurate dose calculations, but there are problems such as increased exposure dose, inconvenience, and a change in treatment schedule. We would like to evaluate the minimum CT scan range required by changing the plan setup parameter of the existing CT scan range. Materials and methods: CT Simulator(Discovery CT590 RT, GE, USA) and In House Head & Neck Phantom are used, CT image was acquired by increasing the image range from 0.25cm to 3.0cm at the end of the target. The target and normal organs were registered in the Head & Neck Phantom and the treatment plan was designed using ACCURAY Precision®. Prescription doses are Daily 2.2Gy, 27 Fxs, Total Dose 59.4Gy. Target is designed to 95%~107% of prescription dose and normal organ dose is designed according to SMC Protocol. Under the same treatment plan conditions, Treatment plans were designed by using five methods(Fixed-1cm, Fixed-2.5cm, Fixed-5cm, Dynamic-2.5cm Dynamic-5cm) and two pitches(0.43, 0.287). The accuracy of dose delivery for each treatment plan was analyzed by using EBT3 film and RIT(Complete Version 6.7, RIT, USA). Results: The accurate treatment plan that satisfying the prescribed dose of Target and the tolerance dose in normal organs(SMC Protocol) require scan range of at least 0.25cm for Fixed-1cm, 0.75cm for Fixed-2.5cm, 1cm for Dynamic-2.5cm, and 1.75cm for Fixed-5cm and Dynamic-5cm. As a result of AnalysisAnalysis by RIT. The accuracy of dose delivery was less than 3% error in the treatment plan that satisfied the SMC Protocol. Conclusion: In case of insufficient CT scan range in head and neck Tomotherapy®, It was possible to make an accurate treatment plan by adjusting the FW among the setup parameter. If the parameter recommended by this author is applied according to CT scan range and is decide whether to re-CT or not, the efficiency of the task and the exposure dose of the patient are reduced.

Analysis of Set-up Errors during CT-scan, Simulation, and Treatment Process in Breast Cancer Patients (유방암 환자의 모의치료, CT 스캔 및 치료 과정에서 발생되는 준비 오차 분석)

  • Lee, Re-Na
    • Radiation Oncology Journal
    • /
    • v.23 no.3
    • /
    • pp.169-175
    • /
    • 2005
  • Purpose: Although computed tomography (CT) simulators are commonly used in radiation therapy department, many Institution still use conventional CT for treatments. In this study the setup errors that occur during simulation, CT scan (diagnostic CT scanner), and treatment were evaluated for the twenty one breast cancer patients. Materials and Methods: Errors were determined by calculating the differences in isocenter location, SSD, CLD, and locations of surgical clips implanted during surgery. The anatomic structures on simulation film and DRR image were compared to determine the movement of isocenter between simulation and CT scan. The isocetner point determined from the radio-opaque wires placed on patient's surface during CT scan was moved to new position if there was anatomic mismatch between the two images Results: In 7/21 patients, anatomic structures on DRR Image were different from the simulation Image thus new isocenter points were placed for treatment planning. The standard deviations of the diagnostic CT setup errors relative to the simulator setup in lateral, longitudinal, and anterior-posterior directions were 2.3, 1.6, and 1.6 mm, respectively. The average variation and standard deviation of SSD from AP field were 1.9 mm and 2.3 mm and from tangential fields were 2.8 mm and 3.7 mm. The variation of the CLD for the 21 patients ranged from 0 to 6 mm between simulation and DRR and 0 to 5 mm between simulation and treatment. The group systematic errors analyzed based on clip locations were 1.7 mm in lateral direction, 2.1 mm in AP direction, and 1.7 mm in SI direction. Conclusion: These results represent that there was no significant differences when SSD, CLD, clips' locations and isocenter locations were considered. Therefore, it is concluded that when a diagnostic CT scanner is used to acquire an image, the set-up variation is acceptable compared to using CT simulator for the treatment of breast cancer. However, the patient has to be positioned with care during CT scan in order to reduce the setup error between simulation and CT scan.

Evaluation of Usefulness of Iterative Metal Artifact Reduction(IMAR) Algorithm In Proton Therapy Planning (양성자 치료계획에서 Iterative Metal Artifact Reduction(IMAR) Algorithm 적용의 유용성 평가)

  • Han, Young Gil;Jang, Yo Jong;Kang, Dong Heok;Kim, Sun Young;Lee, Du Hyeon
    • The Journal of Korean Society for Radiation Therapy
    • /
    • v.29 no.1
    • /
    • pp.49-56
    • /
    • 2017
  • Purpose: To evaluate the accuracy of the Iterative Metal Artifact Reduction (IMAR) algorithm in correcting CT (computed tomography) images distorted due to a metal artifact and to evaluate the usefulness when proton therapy plan was plan using the images on which IMAR algorithm was applied. Materials and Methods: We used a CT simulator to capture the images when metal was not inserted in the CIRS model 062 Phantom and when metal was inserted in it and Artifact occurred. We compared the differences in the CT numbers from the images without metal, with a metal artifact, and with IMAR algorithm by setting ROI 1 and ROI 2 at the same position in the phantom. In addition, CT numbers of the tissue equivalents located near the metal were compared. For the evaluation of Rando Phantom, CT was taken by inserting a titanium rod into the spinal region of the Rando phantom modelling a patient who underwent spinal implant surgery. In addition, the same proton therapy plan was established for each image, and the differences in Range at three sites were compared. Results: In the evaluation of CIRS Phantom, the CT numbers were -6.5 HU at ROI 1 and -10.5 HU at ROI 2 in the absence of metal. In the presence of metal, Fe, Ti, and W were -148.1, -45.1 and -151.7 HU at ROI 1, respectively, and when the IMAR algorithm was applied, it increased to -0.9, -2.0, -1.9 HU. In the presence of metal, they were 171.8, 63.9 and 177.0 HU at ROI 2 and after the application of IMAR algorithm they decreased to 10.0 6,7 and 8.1 HU. The CT numbers of the tissue equivalents were corrected close to the original CT numbers except those in the lung located farthest. In the evaluation of the Rando Phantom, the mean CT numbers were 9.9, -202.8, and 35.1 HU at ROI 1, and 9.0, 107.1, and 29 HU at ROI 2 in the absence, presence of metal, and in the application of IMAR algorithm. The difference between the absence of metal and the range of proton beam in the therapy was reduced on the average by 0.26 cm at point 1, 0.20 cm at point 2, and 0.12 cm at point 3 when the IMAR algorithm was applied. Conclusion: By applying the IMAR algorithm, the CT numbers were corrected close to the original ones obtained in the absence of metal. In the beam profile of the proton therapy, the difference in Range after applying the IMAR algorithm was reduced by 0.01 to 3.6 mm. There were slight differences as compared to the images absence of metal but it was thought that the application of the IMAR algorithm could result in less error compared with the conventional therapy.

  • PDF

초고속 통신망을 이용한 척추 경나사못 삽입술 Simulator

  • 윤승식;성정환;최희원;김영호;강석호;염진섭
    • Proceedings of the Korean Operations and Management Science Society Conference
    • /
    • 1999.04a
    • /
    • pp.105-107
    • /
    • 1999
  • 본 연구의 목적은 CT장비로부터 얻어지는 단면 영상을 이용하여 재구성한 3차원 Voxel 정보를 기반으로 의료 시술 중 위험도가 높으며 장기간의 수술 훈련이 필요한 수술인 척추경나사 삽입술에 대한 모의 시술기를 개발하는 것이다. 모의 시술기의 입력은 환자의 환부에 대한 CT와 모의 시술을 해보고자 하는 의사 (사용자)의 입력 (경나사의 진입 위치와 각도)이 되며 출력은 의사들이 시술장에서 받을 수 있는 유일한 방법인 Voxel데이터로부터 재생성된 X-Ray이미지, 혹은 C-Arm의 동영상이며, 최종 결과 출력은 나사못이 삽입된 재구성 CT 이미지들과 3차원 정보를 볼 수 있는 Image Based Rendering의 Image data set이 된다. 본 연구에서는 각 시각화 부분의 특성을 고려하여 direct volume projection, surface modeling, 그리고 최근 많은 관심을 받고 있는 Image Based Rendering 기법을 intergrate하여 사용하였으며 각 시각화 모듈의 초고속 정보 통신망에서의 정보 교환에 대한 방법론에 대해 다루고 있다.

  • PDF

A Study on a Comparative Analysis of 2D and 3D Planning Using CT Simulator for Transbronchial Brachytherapy (전산화단층모의치료기를 이용한 경기관지 근접치료환자의 치료계획에 관한 고찰)

  • Seo, Dong Rin;Kim, Dae Sup;Back, Geum Mun
    • The Journal of Korean Society for Radiation Therapy
    • /
    • v.25 no.1
    • /
    • pp.69-75
    • /
    • 2013
  • Purpose: Transbronchial brachytherapy used in the two-dimensional treatment planning difficult to identify the location of the tumor in the affected area to determine the process analysis. In this study, we have done a comparative analysis for the patient's treatment planning using a CT simulator. Materials and Methods: The analysis was performed by the patients who visited the hospital to June 2012. The patient carried out CT-image by CT simulator, and we were plan to compare with a two-dimensional and threedimensional treatment planning using a Oncentra Brachy planning system (Nucletron, Netherland). Results: The location of the catheter was confirmed the each time on a treatment planning for fractionated transbronchial brachytherapy. GTV volumes were $3.5cm^3$ and $3.3cm^3$. Also easy to determine the dose distribution of the tumor, the errors of a dose delivery were confirmed dose distribution of the prescibed dose for GTV. In the first treatment was 92% and the second was 88%. Conclusion: In order to compensate for the problem through a two-dimensional treatment planning, it is necessary to be tested process for the accurate identification and analysis of the treatment volume and dose distribution. Quantitatively determine the dose delivery error process that is reflected to the treatment planning is required.

  • PDF

How to Determine the Moving Target Exactly Considering Target Size and Respiratory Motion: A Phantom Study (종양의 움직임과 호흡주기에 따른 체적 변화에 대한 연구: 팬텀 Study)

  • Kim, Min-Su;Back, Geum-Mun;Kim, Dae-Sup;Kang, Tae-Yeong;Hong, Dong-Ki;Kwon, Kyung-Tae
    • The Journal of Korean Society for Radiation Therapy
    • /
    • v.22 no.2
    • /
    • pp.145-153
    • /
    • 2010
  • Purpose: To accurately define internal target volume (ITV) for treatment of moving target considering tumor size and respiratory motion, we quantitatively investigated volume of target volume delineated on CT images from helical CT and 4D CT scans. Materials and Methods: CT images for a 1D moving phantom with diameters of 1.5, 3, and 6 cm, acryl spheres were acquired using a LightSpeed $RT^{16}CT$ simulator. To analyze effect of tumor motion on target delineation, the CT image of the phantoms with various moving distances of 1~4 cm, and respiratory periods of 3~6 seconds, were acquired. For investigating the accuracy of the target trajectory, volume ratio of the target volumes delineated on CT images to expected volumes calculated with diameters of spherical phantom and moving distance were compared. Results: Ratio$_{helical}$ for the diameter of 1, 5, 3, and 6 cm targets were $32{\pm}14%$, $45{\pm}14%$, and $58{\pm}13%$, respectively, in the all cases. As to 4DCT, RatioMIP were $98{\pm}8%$, $97{\pm}5%$, and $95{\pm}1%$, respectively. Conclusion: The target volumes delineated on MIP images well represented the target trajectory, in comparison to those from helical CT. Target volume delineation on MIP images might be reasonable especially for treatment of early stage lung cancer, with meticulous attention to small size target, large respiratory motion, and fast breathing.

  • PDF

Analysis of the Imaging Dose for IGRT/Gated Treatments (영상유도 및 호흡동조 방사선치료에서의 영상장비에 의한 흡수선량 분석)

  • Shin, Jung-Suk;Han, Young-Yih;Ju, Sang-Gyu;Shin, Eun-Hyuk;Hong, Chae-Seon;Ahn, Yong-Chan
    • Radiation Oncology Journal
    • /
    • v.27 no.1
    • /
    • pp.42-48
    • /
    • 2009
  • Purpose: The introduction of image guided radiation therapy/four-dimensional radiation therapy (IGRT/4DRT) potentially increases the accumulated dose to patients from imaging and verification processes as compared to conventional practice. It is therefore essential to investigate the level of the imaging dose to patients when IGRT/4DRT devices are installed. The imaging dose level was monitored and was compared with the use of pre-IGRT practice. Materials and Methods: A four-dimensional CT (4DCT) unit (GE, Ultra Light Speed 16), a simulator (Varian Acuity) and Varian IX unit with an on-board imager (OBI) and cone beam CT (CBCT) were installed. The surface doses to a RANDO phantom (The Phantom Laboratory, Salem, NY USA) were measured with the newly installed devices and with pre-existing devices including a single slice CT scanner (GE, Light Speed), a simulator (Varian Ximatron) and L-gram linear accelerator (Varian, 2100C Linac). The surface doses were measured using thermo luminescent dosimeters (TLDs) at eight sites-the brain, eye, thyroid, chest, abdomen, ovary, prostate and pelvis. Results: Compared to imaging with the use of single slice non-gated CT, the use of 4DCT imaging increased the dose to the chest and abdomen approximately ten-fold ($1.74{\pm}0.34$ cGy versus $23.23{\pm}3.67$cGy). Imaging doses with the use of the Acuity simulator were smaller than doses with the use of the Ximatron simulator, which were $0.91{\pm}0.89$ cGy versus $6.77{\pm}3.56$ cGy, respectively. The dose with the use of the electronic portal imaging device (EPID; Varian IX unit) was approximately 50% of the dose with the use of the L-gram linear accelerator ($1.83{\pm}0.36$ cGy versus $3.80{\pm}1.67$ cGy). The dose from the OBI for fluoroscopy and low-dose mode CBCT were $0.97{\pm}0.34$ cGy and $2.3{\pm}0.67$ cGy, respectively. Conclusion: The use of 4DCT is the major source of an increase of the radiation (imaging) dose to patients. OBI and CBCT doses were small, but the accumulated dose associated with everyday verification need to be considered.

Development of Multi-Body Dynamics Simulator for Bio-Mimetic Motion in Lizard Robot Design (도마뱀 로봇 설계를 위한 생체운동 모사 다물체 동역학 시뮬레이터 개발)

  • Park, Yong-Ik;Seo, Bong Cheol;Kim, Sung-Soo;Shin, Hocheol
    • Transactions of the Korean Society of Mechanical Engineers A
    • /
    • v.38 no.6
    • /
    • pp.585-592
    • /
    • 2014
  • In this study, a multibody simulator was developed to analyze the bio-mimetic motion of a lizard robot design. A RecurDyn multibody dynamics model of a lizard was created using a micro-computerized tomography scan and motion capture data. The bio-mimetic motion simulator consisted of a trajectory generator, an inverse kinematics module, and an inverse dynamics module, which were used for various walking motion analyses of the developed lizard model. The trajectory generation module produces spinal movements and gait trajectories based on the lizard's speed. Using the joint angle history from an inverse kinematic analysis, an inverse dynamic analysis can be carried out, and the required joint torques can be obtained for the lizard robot design. In order to investigate the effectiveness of the developed simulator, the required joint torques of the model were calculated using the simulator.