• Journal of radiological science and technology
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• v.40 no.3
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• pp.443-451
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• 2017

Mammography is commonly used for screening early breast cancer. However, mammographic images, which depend on the physical properties of breast components, are limited to provide information about whether a lesion is malignant or benign. Although a dual-energy subtraction technique decomposes a certain material from a mixture, it increases radiation dose and degrades the accuracy of material decomposition. In this study, we simulated a breast phantom using attenuation characteristics, and we proposed a technique to enable the accurate material decomposition by applying weighting factors for the dual-energy mammography based on a photon-counting detector using a Monte Carlo simulation tool. We also evaluated the contrast and noise of simulated breast images for validating the proposed technique. As a result, the contrast for a malignant tumor in the dual-energy weighted subtraction technique was 0.98 and 1.06 times similar than those in the general mammography and dual-energy subtraction techniques, respectively. However the contrast between malignant and benign tumors dramatically increased 13.54 times due to the low contrast of a benign tumor. Therefore, the proposed technique can increase the material decomposition accuracy for malignant tumor and improve the diagnostic accuracy of mammography.

• Proceedings of the Korean Vacuum Society Conference
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• 2016.02a
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• pp.240-240
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• 2016

반도체 양자점은 불연속적인 에너지준위의 특성 때문에 고전적인 빛과는 다른 단일광자를 방출하여 양자정보 처리과정에 기본 요소로써 사용 될 수 있다. III-Nitride (III-N) 반도체 물질은 III족 원소의 구성비를 조절하였을 때 밴드갭 에너지차이가 크므로 깊은 양자 우물을 만들 수 있으며 최근에는 기존에 연구되던 III-Arsenide 기반의 반도체 양자점과 다르게 상온 (300 K) 동작 가능한 단일광자 방출원이 개발되었다.[1] 또한 약한 split-off 에너지 때문에 양자점 모양에 작은 비대칭성만 존재해도 큰 선형편광도를 가질 수 있다. 하지만 III-N 반도체 양자점의 이러한 특성에도 불구하고 이종기판과의 격자상수 불일치에 따른 많은 threading dislocation, 압전효과에 의한 큰 내부전기장에 의해 발광 효율이 떨어지는 등의 문제가 있다. 이를 해결하기 위해 반도체 양자점을 3차원 구조체와 결합하여 threading dislocation 및 내부전기장을 줄이는 연구들이 진행되고 있다.[2] 본 연구에서는 선택적 영역 성장 방식을 통해 마이크로미터 크기를 가지는 피라미드 형태의 3차원 구조체를 이용, 피라미드의 꼭지점에 형성된 InGaN/GaN 양자점의 광학적 특성에 대해 분석하였다. 저온(9 K)에서 마이크로 photoluminescence 측정을 통해 양자점의 발광파장이 피라미드의 옆면의 파장과는 다름을 확인하였다. 여기광의 세기에 따른 양자점의 발광 세기 측정하여 여기광에 선형 비례함을 보이고, 양자점의 편광도를 측정하여 선형 편광임을 확인하였다. 마지막으로, 광량에 대해 시간에 따른 상관관계를 측정함으로써 양자점이 양자 발광체의 특성을 보이는 지 확인하였다.

• Proceedings of the Korean Vacuum Society Conference
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• 2014.02a
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• pp.132.2-132.2
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• 2014

란탄족 원소가 도핑된 세라믹 나노결정, 즉, 나노형광체는 도핑되는 원소의 종류에 따라 다양한 색을 발광할 수 있다. 일반적으로 형광체는 외부에너지에 의해 여기된 후 흡수한 에너지 보다 작은 에너지의 가시광을 발광하게 된다. 이러한 현상은 downconversion 발광으로 알려져 있다. 그러나 모체에 Yb3+와 Er3+를 도핑하는 경우 적외선을 흡수하여 가시광선을 발광하는 upconversion 현상이 관찰된다. Upconversion 형광체를 이용하여 적외선을 가시광으로 변환시키면 sub-band gap 손실을 줄임으로써 태양전지 효율을 높일 수 있고, 바이오 이미징 감도를 높일 수도 있다. 그러나, upconversion 발광기구에서는 두 개의 적외선 광자가 흡수되어 하나의 가시광 광자가 방출되기 때문에 upconversion 발광 효율은 downconversion 발광 효율에 비하여 매우 낮은 특성을 보인다. 특히 형광체의 크기가 작아져 나노미터 영역의 크기가 되면 효율이 더욱 낮아지기 때문에 upconversion 나노형광체의 경우 효율을 증가시키기 위하여 형광체 주위로 결정질 쉘을 형성시키는 것이 필요하다. 이 때, 결정질 쉘에 downconversion 특성을 보일 수 있는 란탄족 원소를 도핑하는 경우 upconversion 발광 강도가 증대될 뿐 아니라, 하나의 나노입자에서 upconversion과 downconversion 두 가지 서로 다른 발광 특성을 관찰할 수 있다. 본 발표에서는 단일 나노입자에서 upconversion과 downconversion 발광을 보이는 이중발광 코어/쉘 나노형광체의 발광 특성에 대하여 논의하고자 한다.

• Korean Journal of Optics and Photonics
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• v.2 no.4
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• pp.203-208
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• 1991

We investigated the nonradiative energy transfer process from Rhodamine 6G to Malachite Green in ethylen glycol solvent using time correlated single photon counting system equipped with a modelocked Ar ' laser. The reduced concentration and critical transfer distance for various acceptor concentration were obtained by using a full-fitting analysis of the fluorescence decay curves. We found that Huber model is more suitable than Forster model and the influence of energy migration through the dipole-dipole interaction becomes more significant for the low acceptor concentrations relative to the donor concentration($5\times 10^4$mol/l).

• Journal of the Korean Society of Radiology
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• v.10 no.8
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• pp.591-596
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• 2016

The purpose of this study is to determine the equivalent energy of a 6MV X-ray beam in the experiment. The half-value layer (HVL) of lead for the 6 MV X-ray beam was measured using an ionization chamber. The linear attenuation coefficients were calculated with HVL. And, the mass attenuation coefficient was obtained by dividing the linear attenuation coefficient by the density of lead. The equivalent energy of mass attenuation coefficient was determined using the photon energy versus mass attenuation coefficient data of lead given by National Institute of Standards and Technology (NIST). In conclusion, the equivalent energy of the 6 MV X-ray beam was determined to be 1.61 MeV. This equivalent energy was determined to be about 30% lower than reported by Reft. The reason is presumed to be due to the presence of an air cavity between the lead attenuators.

• The Journal of Korean Society for Radiation Therapy
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• v.25 no.1
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• pp.1-8
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• 2013

Purpose: A selection of proper energy in treatment planning is very important because of having different dose distribution in body as photon energy. In generally, the low energy photon has been used in intensity-modulated radiation therapy (IMRT) for head and neck (H&N) cancer. The aim of this study was to evaluate the effect of partially used high energy photon at posterior oblique fields on IMRT plan for H&N cancer. Materials and Methods: The study was carried out on 10 patients (nasopharyngeal cancer 5, tonsilar cancer 5) treated with IMRT in Seoul National University Bundang Hospital. CT images were acquired 3 mm of thickness in the same condition and the treatment plan was performed by Eclipse (Ver.7.1, Varian, Palo Alto, USA). Two plans were generated under same planing objectives, dose volume constraints, and eight fields setting: (1) The low energy plan (LEP) created using 6 MV beam alone, (2) the partially used high energy plan (PHEP) created partially using 15 MV beam at two posterior oblique fields with deeper penetration depths, while 6 MV beam was used at the rest of fields. The plans for LEP and PHEP were compared in terms of coverage, conformity index (CI) and homogeneity index (HI) for planning target volume (PTV). For organs at risk (OARs), $D_{mean}$ and $D_{50%}$ were analyzed on both parotid glands and $D_{max}$, $D_{1%}$ for spinal cord were analyzed. Integral dose (ID) and total monitor unit (MU) were compared as addition parameters. For the comparing dose to normal tissue of posterior neck, the posterior-normal tissue volume (P-NTV) was set on the patients respectively. The $D_{mean}$, $V_{20Gy}$ and $V_{25Gy}$ for P-NTV were evaluated by using dose volume histogram (DVH). Results: The dose distributions were similar with regard to coverage, CI and HI for PTV between the LEP and PHEP. No evident difference was observed in the spinal cord. However, the $D_{mean}$, $D_{50%}$ for both parotid gland were slightly reduced by 0.6%, 0.7% in PHEP. The ID was reduced by 1.1% in PHEP, and total MU for PHEP was 1.8% lower than that for LEP. In the P-NTV, the $D_{mean}$, $V_{20Gy}$ and $V_{25Gy}$ of the PHEP were 1.6%, 1.8% and 2.9% lower than those of LEP. Conclusion: Dose to some OARs and a normal tissue, total monitor unit were reduced in IMRT plan with partially used high energy photon. Although these reduction are unclear how have a clinical benefit to patient, application of the partially used high energy photon could improve the overall plan quality of IMRT for head and neck cancer.

• Journal of radiological science and technology
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• v.34 no.1
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• pp.43-50
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• 2011

In this study we modeled the varian 2100C/D linear accelerator head and multi-leaf collimator by simulation with the GEANT4 Monte Carlo toolkit. Then central axis percentage depth dose profiles and lateral dose profiles within homogeneous water phantom($50{\times}50{\times}50\;cm^3$) were evaluated with 6 MV photon beam. The simulations were performed in two stages. In the first stage, photon energy spectrum at the target were computed were computed. Then spectra data was directly irradiated in the water phantom using sampling techniques. The simulation data were compared with experimental data to evaluate the accuracy of the model. Results showed that two data were matched within 2% error boundary. The proposed method will be applied for simulation of dose calculation and dose distribution study.

• Progress in Medical Physics
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• v.13 no.1
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• pp.1-8
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• 2002

Accurate knowledge of the distribution of contamination electrons ( which comes from mainly gantry head by Compton scattering, pair production, and tray: henceforth called leptons ) at the surface and in the first centimeters of tissue is essential for the clinical practice of radiation oncology. Such lepton tends to reduce or eliminate the ‘skin-sparing’ advantage of megavoltage photon beam radiotherapy, This information is needed to prescribe a absorbed dose to a skin volume at a few millimeter depth in high energy therapeutic radiation photon beam All experiments were done with 15 MV photon beam from a dual energy linear accelerator (Clinac 1800, Varian). Field size is defined by ranged from 10.0$\times$10.0 to 30.0$\times$30.0 $\textrm{cm}^2$. The absorbed dose and distribution of leptons in therapeutic radiation beam (15 MV) are investigated by means of variable blocked beams of 30.0$\times$30.0 $\textrm{cm}^2$ and dose beam profiles partly removed leptons with a copper plate. A numerous leptons mainly are distributed as shape of broad cone in the central photon beam and leptons path length in the water are shorter than 2.5 cm because of the leptons energy having around 3.0 MeV. These results clearly appears that the subtraction of leptons from the total depth dose curve not only lower the absolute dose in the buildup region and surface dose, it also causes a shift of d$_{max}$ to a deeper depth.

• Progress in Medical Physics
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• v.23 no.2
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• pp.99-105
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• 2012

We investigated the influence of photon energy, couch and collimator angle differences between arcs on dose distribution of RapidArc treatment planning for prostate cancer. RapidArc plans were created for 6 MV and 10 MV photons using 2 arcs coplanar and noncoplanar fields. The collimator angle differences between two arcs were $0^{\circ}$, $15^{\circ}$, $30^{\circ}$, $45^{\circ}$, $60^{\circ}$, $75^{\circ}$ and $90^{\circ}$. The plans were optimized using same dose constrains for target and OAR (organ at risk). To evaluate the dose distribution, plans were analyzed using CI (conformity index), HI (homogeneity index), QOC (quality of coverage), etc. Photon energy, couch and collimator angle differences between arcs had a little influence on the target and OAR. The difference of dosimetric indices was less than 3.6% in the target and OAR. However, there was significant increase in the region exposed to low dose. The increase of V15% in the femur was 6.4% (left) and 5.5% (right) for the 6 MV treatment plan and 23.4% (left), 24.1% (right) for the noncoplanar plan. The increase of V10% in the Far Region distant from target was 54.2 cc for the 6 MV photon energy, 343.4 cc for the noncoplanar and 457.8 cc for the no collimator rotation between arcs.

• Journal of the Korean Institute of Telematics and Electronics D
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• v.35D no.8
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• pp.44-52
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• 1998

The theoretical modeling of transition energy and absorption coefficient for intersubband transitions in quantum wells in presented. We include, as well as hartree and exchange-correlation potentials, boht depolarization effect and exciton-like effect which play great roles in heavily doped cases where practically reasonable absorption coefficients are available. Also, the calculated results are compared with the existing experimental values for .delta.-doped Si quantum wells to check the validity of our theoretical calculation.