• The Journal of Korea Institute of Information, Electronics, and Communication Technology
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• v.16 no.4
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• pp.187-192
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• 2023

This paper deposited CdTe thin films on ITO glass substrates using sputtering equipment while changing RF power. As a result of measuring the thickness of the thin film, 1481Å at 100W, 2985Å at 150W, and 4684Å at 200W. And the mobility was measured as 8.43 cm2/Vs for 100W, 7.91 cm2/Vs for 150W, and 6.57 cm2/Vs for 200W. It can be seen that the thickness and mobility of the thin film are inversely proportional. As a result of confirming the transmittance, the transmittance was 84% at 905nm for 100W, the transmittance was 71% at 825nm for 150W, and 77% at 874nm for 200W. At 100 W, the thickness of the thin film was thin, so the transmittance was measured to be high. In other words, the correlation between transmittance and thickness can be seen. As a result of measuring the FHWM and particle size by changing the RF Power, 100W was calculated as 0.18, 150W was calculated as 0.19, and 200W was calculated as 0.73. The size of the particles was formed at 8.47Å at 100W, 7.98Å at 150W, and 8.7Å, which is the largest at 200W. In conclusion, it was found that the FHWM and particle size were inversely proportional.

• Korean Journal of Optics and Photonics
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• v.10 no.4
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• pp.318-322
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• 1999

Perdeuterated hexaflouroacetylacetonato-neodymium [$Nd(HFA-D)_3$] complexes were synthesized by the keto-enol tautomerism reaction of $Nd(HFA-D)_3$ in methanol-d$_4$ in order to reduce the radiationless transition to the ligands. The emission properties of $Nd(HFA-D)_3$ complex were measured in the following anhydrous deuterated organic solvents; $Methanol-d_4$, $Aceton-d_6$, $THE-d_8$ and $DMSO-d_6$, and these properties depended on the coordination ability of solvent molecules. The intensity and lifetime of the emission in dimethysulfoxide (DMSO-$d_6$) were superior to those in other in other deuterated solvents. It was suggested that the anhydrous $DMSO-d_6$might be the most appropriate solvent for the liquid laser material of $Nd(HFA-D)_3$ complex.

• Progress in Medical Physics
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• v.25 no.1
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• pp.37-45
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• 2014

The accuracy and uniformity of CT numbers are the main causes of radiation dose calculation error. Especially, for the dose calculation based on kV-Cone Beam Computed Tomography (CBCT) image, the scatter affecting the CT number is known to be quite different by the object sizes, densities, exposure conditions, and so on. In this study, the scatter impact on the CBCT based dose calculation was evaluated to provide the optimal condition minimizing the error. The CBCT images was acquired under three scatter conditions ("Under-scatter", "Over-scatter", and "Full-scatter") by adjusting amount of scatter materials around a electron density phantom (CIRS062, Tissue Simulation Technology, Norfolk, VA, USA). The CT number uniformities of CBCT images for water-equivalent materials of the phantom were assessed, and the location dependency, either "inner" or "outer" parts of the phantom, was also evaluated. The electron density correction curves were derived from CBCT images of the electron density phantom in each scatter condition. The electron density correction curves were applied to calculate the CBCT based doses, which were compared with the dose based on Fan Beam Computed Tomography (FBCT). Also, 5 prostate IMRT cases were enrolled to assess the accuracy of dose based on CBCT images using gamma index analysis and relative dose differences. As the CT number histogram of phantom CBCT images for water equivalent materials was fitted with a gaussian function, the FHWM (146 HU) for "Full-scatter" condition was the smallest among the FHWM for the three conditions (685 HU for "under scatter" and 264 HU for "over scatter"). Also, the variance of CT numbers was the smallest for the same ingredients located in the center and periphery of the phantom in the "Full-scatter" condition. The dose distributions calculated with FBCT and CBCT images compared in a gamma index evaluation of 1%/3 mm criteria and in the dose difference. With the electron density correction acquired in the same scatter condition, the CBCT based dose calculations tended to be the most accurate. In 5 prostate cases in which the mean equivalent diameter was 27.2 cm, the averaged gamma pass rate was 98% and the dose difference confirmed to be less than 2% (average 0.2%, ranged from -1.3% to 1.6%) with the electron density correction of the "Full-scatter" condition. The accuracy of CBCT based dose calculation could be confirmed that closely related to the CT number uniformity and to the similarity of the scatter conditions for the electron density correction curve and CBCT image. In pelvic cases, the most accurate dose calculation was achievable in the application of the electron density curves of the "Full-scatter" condition.