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Dive into the research topics where Kyung Hwan Chang is active.

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Featured researches published by Kyung Hwan Chang.


Radiation Protection Dosimetry | 2010

Dose reduction in CT using bismuth shielding: measurements and Monte Carlo simulations.

Kyung Hwan Chang; Wonho Lee; Dong Myung Choo; Choon Sik Lee; Youhyun Kim

In this research, using direct measurements and Monte Carlo calculations, the potential dose reduction achieved by bismuth shielding in computed tomography was evaluated. The patient dose was measured using an ionisation chamber in a polymethylmethacrylate (PMMA) phantom that had five measurement points at the centre and periphery. Simulations were performed using the MCNPX code. For both the bare and the bismuth-shielded phantom, the differences of dose values between experiment and simulation were within 9%. The dose reductions due to the bismuth shielding were 1.2-55% depending on the measurement points, X-ray tube voltage and the type of shielding. The amount of dose reduction was significant for the positions covered by the bismuth shielding (34 - 46% for head and 41 - 55% for body phantom on average) and negligible for other peripheral positions. The artefact on the reconstructed images were minimal when the distance between the shielding and the organs was >1 cm, and hence the shielding should be selectively located to protect critical organs such as the eye lens, thyroid and breast. The simulation results using the PMMA phantom was compared with those using a realistically voxelised phantom (KTMAN-2). For eye and breast, the simulation results using the PMMA and KTMAN-2 phantoms were similar with each other, while for thyroid the simulation results were different due to the discrepancy of locations and the sizes of the phantoms. The dose reductions achieved by bismuth and lead shielding were compared with each other and the results showed that the difference of the dose reductions achieved by the two materials was less than 2-3%.


Journal of Applied Clinical Medical Physics | 2012

Evaluation of mechanical accuracy for couch-based tracking system (CBTS)

Suk Lee; Kyung Hwan Chang; Jand Bo Shim; Y. Cao; Chang Ki Lee; Sam Ju Cho; Dae Sik Yang; Young Je Park; Won Seob Yoon; Chul Yong Kim

This study evaluated the mechanical accuracy of an in‐house–developed couch‐based tracking system (CBTS) according to respiration data. The overall delay time of the CBTS was calculated, and the accuracy, reproducibility, and loading effect of the CBTS were evaluated according to the sinusoidal waveform and various respiratory motion data of real patients with and without a volunteer weighing 75 kg. The root mean square (rms) error of the accuracy, the reproducibility, and the sagging measurements were calculated for the three axes (X, Y, and Z directions) of the CBTS. The overall delay time of the CBTS was 0.251 sec. The accuracy and reproducibility in the Z direction in real patient data were poor, as indicated by high rms errors. The results of the loading effect were within 1.0 mm in all directions. This novel CBTS has the potential for clinical application for tumor tracking in radiation therapy. PACS number: 87.55.ne


Physica Medica | 2015

Development of a 3D optical scanner for evaluating patient-specific dose distributions.

Kyung Hwan Chang; Suk Lee; Hong Jung; Yeon Wook Choo; Yuan Jie Cao; Jang Bo Shim; Kwang Hyeon Kim; Nam Kwon Lee; Young Je Park; Chul Yong Kim; Sam Ju Cho; Sang Hoon Lee; Chul Kee Min; Woo Chul Kim; Kwang Hwan Cho; Hyun Do Huh; Sangwook Lim

PURPOSE This paper describes the hardware and software characteristics of a 3D optical scanner (P3DS) developed in-house. The P3DS consists of an LED light source, diffuse screen, step motor, CCD camera, and scanner management software with 3D reconstructed software. MATERIALS AND METHOD We performed optical simulation, 2D and 3D reconstruction image testing, and pre-clinical testing for the P3DS. We developed the optical scanner with three key characteristics in mind. First, we developed a continuous scanning method to expand possible clinical applications. Second, we manufactured a collimator to improve image quality by reducing scattering from the light source. Third, we developed an optical scanner with changeable camera positioning to enable acquisition of optimal images according to the size of the gel dosimeter. RESULTS We confirmed ray-tracing in P3DS with optic simulation and found that 2D projection and 3D reconstructed images were qualitatively similar to the phantom images. For pre-clinical tests, the dose distribution and profile showed good agreement among RTP, optical CT, and external beam radiotherapy film data for the axial and coronal views. The P3DS has shown that it can scan and reconstruct for evaluation of the gel dosimeter within 1 min. We confirmed that the P3DS system is a useful tool for the measurement of 3D dose distributions for 3D radiation therapy QA. Further experiments are needed to investigate quantitative analysis for 3D dose distribution.


Medical Dosimetry | 2015

Patient performance-based plan parameter optimization for prostate cancer in tomotherapy.

Yuan Jie Cao; Suk Lee; Kyung Hwan Chang; Jang Bo Shim; Kwang Hyeon Kim; Young Je Park; Chul Yong Kim

The purpose of this study is to evaluate the influence of treatment-planning parameters on the quality of treatment plans in tomotherapy and to find the optimized planning parameter combinations when treating patients with prostate cancer under different performances. A total of 3 patients with prostate cancer with Eastern Cooperative Oncology Group (ECOG) performance status of 2 or 3 were included in this study. For each patient, 27 treatment plans were created using a combination of planning parameters (field width of 1, 2.5, and 5cm; pitch of 0.172, 0.287, and 0.43; and modulation factor of 1.8, 3, and 3.5). Then, plans were analyzed using several dosimetrical indices: the prescription isodose to target volume (PITV) ratio, homogeneity index (HI), conformity index (CI), target coverage index (TCI), modified dose HI (MHI), conformity number (CN), and quality factor (QF). Furthermore, dose-volume histogram of critical structures and critical organ scoring index (COSI) were used to analyze organs at risk (OAR) sparing. Interestingly, treatment plans with a field width of 1cm showed more favorable results than others in the planning target volume (PTV) and OAR indices. However, the treatment time of the 1-cm field width was 3 times longer than that of plans with a field width of 5cm. There was no substantial decrease in treatment time when the pitch was increased from 0.172 to 0.43, but the PTV indices were slightly compromised. As expected, field width had the most significant influence on all of the indices including PTV, OAR, and treatment time. For the patients with good performance who can tolerate a longer treatment time, we suggest a field width of 1cm, pitch of 0.172, and modulation factor of 1.8; for the patients with poor performance status, field width of 5cm, pitch of 0.287, and a modulation factor of 3.5 should be considered.


Journal of Physics: Conference Series | 2010

Development of PDRESS (Patient Specific Dose Real Evaluation Systems) using a TENOMAG Gel and Optical CT (VISTA TM) in Clinical IMRT Prostate Case

Suk Lee; Jang Bo Shim; Kyung Hwan Chang; Y. Cao; Jaeyoun Yi; Jin Woo Park; Sam Ju Cho; Sang Hoon Lee; HyunDo Huh; Kwang Hwan Cho; Chul Kee Min; Dae Sik Yang; Young Je Park; Won Seob Yoon; Chul Yong Kim

The aims of this study, we present the preliminary results of 3 dimensional dose evaluation software (PDRESS, patient specific dose real evaluation systems). In this work, we compared planned 3D dose distribution with measured 3D dose distribution using a novel normoxic polymer gel dosimeter (TENOMAG) and a commercial cone-beam optical CT scanner (VISTATM, Modus Medical Devices, Inc., London, ON, Canada) to verify the 3D dose distribution in intensity-modulated radiation therapy (IMRT) prostate case. And we developed PDRESS using the Xelis Flatform which is developed by INFINITT Corporation is used to display the 3D dose distribution by loading the DICOM RT Data which is exported from RTP and optical-CT reconstructed VFF file. Data analysis is achieved by comparing the RTP data with the VFF data using profile, gamma map, and DTA. The profiles showed good agreement between RTP data, gel dosimeter, and gamma distribution and the precision of the dose distribution is within ± 5%. The results from this study show that there are no significantly discrepancies between the calculated dose distribution from treatment plan and the measured dose distribution from a TENOMAG gel scanned with an optical CT scanner. The 3D dose evaluation software (PDRESS) which is developed in this study evaluates the accuracy of the three dimensional dose distributions.


Journal of the Korean Physical Society | 2013

Spectrophotometric determination of the optimal wavelength for a polymer-gel dosimeter

Kyung Hwan Chang; Suk Lee; Yuan Jie Cao; Jang Bo Shim; Jung Ae Lee; Dae Sik Yang; Young Je Park; Won Sup Yoon; Chul Yong Kim; Sam Ju Cho; Sang Hoon Lee; Woo Chul Kim; Chul Kee Min; Kwang Hwan Cho; Hyun Do Huh


Journal of Radiotherapy in Practice | 2017

Predictive modelling analysis for development of a radiotherapy decision support system in prostate cancer: a preliminary study

Kwang Hyeon Kim; Suk Lee; Jang Bo Shim; Kyung Hwan Chang; Y. Cao; Suk Woo Choi; Se Hyeong Jeon; Dae Sik Yang; Won Sup Yoon; Young Je Park; Chul Yong Kim


Journal of the Korean Physical Society | 2015

Optimized planning target volume margin in helical tomotherapy for prostate cancer: Is there a preferred method?

Yuan Jie Cao; Suk Lee; Kyung Hwan Chang; Jang Bo Shim; Kwang Hyeon Kim; Min Sun Jang; Won Sup Yoon; Dae Sik Yang; Young Je Park; Chul Yong Kim


Journal of the Korean Physical Society | 2014

Physical and radiological properties of radiochromic gel as of its composition

Sang Hoon Lee; Juree Kim; Su Jung Shim; Kyung Hwan Chang; Sangwook Lim; Hyun Do Huh; Dong Oh Shin; Sam Ju Cho


Journal of the Korean Physical Society | 2014

Comparison of the BANGkit™ and the PRESAGE™ gel dosimeters for use with a CCD-based optical CT scanner

Kyung Hwan Chang; Suk Lee; Yuan Jie Cao; Jang Bo Shim; Jieun Lee; Nam Kwon Lee; Jung Ae Lee; Dae Sik Yang; Young Je Park; Won Sup Yoon; Chul Yong Kim; Sam Ju Cho; Sang Hoon Lee; Woo Chul Kim; Chul Kee Min; Kwang Hwan Cho; Hyun Do Huh

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