30 research outputs found

    Down-Scaled 3D Medical Image Transfer System Using Instant Messenger

    Get PDF
    Objective: We have developed an instant messenger system that supports transmitting 3D medical image objects for telediagnostic use. Methods: We used thresholding and down-scaling technique to build down-scaled 3D object with 80 sliced Digital Imaging and Communication in Medicine(DICOM) images. And, we also construct instant messenger for medical data transfer and general communication. We measured total image size and transmission time which were decreased when applied peer to peer connection using instant messenger for medicine. Results: Our study showed that total DICOM image size was decreased around 1% and transmission time was also decreased by 1.59% when we use proposed system. Conclusion: Proposed methods have a potential to be a useful tool in ubiquitous health network system. Also, we expect the synergy effect is increased by developing 3D object technique and security solutions.ope

    ์‹ค๋ฆฌ์ฝ˜ ๊ธฐ๋ฐ˜ ์†Œ์ž๋ฅผ ์ด์šฉํ•œ ์ ์™ธ์„  ๊ฒ€์ถœ

    Get PDF
    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ์ „๊ธฐยท์ปดํ“จํ„ฐ๊ณตํ•™๋ถ€, 2015. 8. ๋ฐ•์˜์ค€.Lights in nature can be classified into various bands depending on the wavelength. Among the many types of light, near infrared (NIR) light has a wavelength of 780?2500 nm. The NIR wavelength band is widely used in various types of sensor devices, as well as in communication. Therefore, there is substantial demand for efficient and cost-effective NIR detectors. However, although materials such as InGaAs, Ge, and PbS are applied in detectors to detect NIR wavelengths, these materials are not compatible with the widely used and cost-effective Si-based integration process. Thus, this dissertation focuses on detection of NIR light using a Si based device. However, the crucial obstacle in using Si as an NIR detection material is that it has band gap energy of 1.12 eV, and therefore, it does not absorb wavelengths longer than 1150nm. One possible solution is utilizing the Franz?Keldysh effect (FKE) in the Si devices. The FKE dictates that a semiconductor can absorb a photon with lower energy than the band-gap energy by tunneling the valence electrons to the conduction band in the presence of a strong electric field. This phenomenon can be used to detect infrared (IR) photons if the junction is biased in the FKE bias region. In this dissertation, to investigate the detection of NIR with a Si-based device, we attempt to use the Zener diode and the NMOSFET, which can generate tunneling currents in the presence of a strong electric field. When a strong reverse bias is applied to the Zener junction, a tunneling current is generatedthe NMOSFET also has a tunneling current when the bias condition generates a gate-induced drain leakage (GIDL) current. In such a bias condition for both devices, NIR with wavelengths of 1310nm and 1550nm, which have lower energy than the band-gap energy of Si, are irradiated to the Zener diode and the NMOSFET. In the case of the Zener diode, an avalanche multiplication is investigated to cause more absorption by applying an additional, stronger electric field than the normal reverse bias condition, which causes a tunneling current to flow. However, because the negative temperature coefficient is due to the Joule heat generation of the junction in the bias regime of the avalanche multiplication, the methodology of a pulsed bias scheme is applied to mitigate the unintentional increase in the junction temperature and the associated degradation of the photo-responsivity under a DC bias. Accordingly, the NMOSFET in the condition in which GIDL flows can also absorb wavelengths of 1310nm and 1550nm by FKE. Additionally, the photo-generated current can be amplified by avalanche multiplication under a strong electric field with the pulsed bias scheme between the drain and the substrate. Thus, this dissertation concludes that Si-based junctions can be used to detect IR signals using the FKE generation followed by multiplication through the newly proposed methodology of pulse measurement, which minimizes both the thermal effect and the degradation of photo-responsivity.1 Introduction (1) 1.1 Motivation (1) 1.2 Optical characteristics of Silicon for IR detectors (3) 1.3 Common view of the Franz-Keldysh effect (5) 1.4 Si devices for an IR photo detector (5) 1.5 Infrareds laser sources (6) 1.6 Outline of the Dissertation (8) 2 Fundamentals of optical transition in Silicon (10) 2.1 The Franz-Keldysh effect (10) 2.2 Tunneling current based on the Franz-Keldysh effect (14) 2.2.1 Tunneling probability (14) 2.2.2 Tunneling Current of the Zener diode (15) 2.2.3 Gate Induced Drain Leakage Current of NMOS (15) 2.3 Phonon-assisted tunneling in the indirect band gap of semiconductor (17) 2.4 Photo Responsivity (18) 3 IR detection with the Zener diode (19) 3.1 Zener diode as a photodetector (19) 3.1.1 Reverse current characteristics of the Zener junction (18) 3.1.2 Feature of the experimental Zener diode (23) 3.1.3 Temperature coefficient of the reverse current (24) 3.2 DC Measurement (25) 3.2.1 Degradation in photo sensitivity (25) 3.2.2 Temperature dependency of the photo sensitivity (28) 3.3 The pulsed bias scheme (31) 3.3.1 Circuit diagram for the pulsed bias scheme (31) 3.3.2 Response of the input pulsed wave (33) 3.4 IR Photo response in the pulsed bias scheme (35) 3.4.1 Bias dependency of photo generated current (35) 3.4.2 Photo responsivity for the infrared signal (38) 3.5 Effect of defects in the junction on the FKE (40) 3.5.1 Correlation of the FKE current with the trap density (40) 4 GIDL regime in the NMOSFET for IR detection (42) 4.1 MOSFET as the photodetector of the infrared light (42) 4.1.1 Energy band of the surface junction in the GIDL bias (42) 4.1.2 Structure of the NMOSFET test pattern (45) 4.2 DC Measurement results (50) 4.2.1 Limitation of the photo sensitivity in the DC bias scheme (50) 4.3 Pulsed bias scheme to induce the NMOS GIDL (58) 4.3.1 Circuit diagram for the pulsed bias scheme (58) 4.3.2 Current response to the Pulsed wave (60) 4.4 IR photo response under the pulsed bias scheme (62) 5 Multiplication of IR signal with NMOSFET (65) 5.1 Multiplication of the FKE current (65) 5.1.1 Schematics of the multiplication of FKE current (65) 5.2 Results of the DC Measurement (68) 5.2.1 Multiplication by the substrate bias (68) 5.2.2 Temperature dependency (72) 5.2.3 Degradation in the photo sensitivity (74) 5.3 Pulsed bias scheme (79) 5.3.1 Circuit diagram for pulsed bias scheme (79) 5.3.2 Response to the input pulsed wave (81) 5.4 Enhanced response by the multiplication (84) 5.5 Simulated results for the NMOS (87) 6 Conclusions (92) 6.1 Summary (92) 6.2 Further works (94)Docto

    A Study on the Performance Improvement of OpenGL based 3D Graphics Applications on Engineering Workstations

    Get PDF
    In 1992, OpenGL from SGI became the most important 3D-API for engineering graphics applications including 3D CAD. The accelerating performance for OpenGL-based 3D graphics application is the first issue of current engineering workstation market. The performance of 3D CAD application is adopted in the area of the hardware devices like microprocessor, main memories, and sub memories. And software includes device drives and operating system. Although the higher performance of 3D CAD application is acquired by the optimized balance of these parts, workstation has many difficulties by generic constructing of computer system. In this paper, the improvement of the performance of OpenGL based 3D graphics for the developers and users of 3D CAD applications on engineering workstations is studied. The analysis of the performance in the configuration of microprocessor, amount of memories, OpenGL acceleration of graphic subsystem and operating environments are investigated. The effects on improving OpenGL 3D-API and 3D CAD applications by the configuration of microprocessors, memories, graphics subsystems and operating environments are also examined. The single configuration of microprocessor is better than multiple configuration. The amounts of memories are major impact element of workstation and applications. And the accelerating performance of OpenGL in graphics subsystem is not proportioned to that of 3D CAD applications. Controlling by configuring of environmental factors of graphics subsystem, operating systems, and device drivers make the higher improvements of performance. Therefore, users and developers of graphics engineering workstations should apply it for the optimized systems for 3D CAD applications.๏ผ‘. ์„œ๋ก  = 1 ๏ผ‘.๏ผ‘. ์—ฐ๊ตฌ ๋ฐฐ๊ฒฝ = 1 ๏ผ‘.๏ผ’. ์—ฐ๊ตฌ ๋ชฉ์  = 2 ๏ผ‘.๏ผ“. ์—ฐ๊ตฌ ๋ฐฉ๋ฒ• = 3 ๏ผ’. ๋งˆ์ดํฌ๋กœํ”„๋กœ์„ธ์„œ ๊ตฌ์„ฑ์— ๋”ฐ๋ฅธ 3D ๊ทธ๋ž˜ํ”ฝ์Šค ์„ฑ๋Šฅ ๋ณ€ํ™” = 10 ๏ผ’.๏ผ‘. OpenGL 3D-API ์„ฑ๋Šฅ ๋ถ„์„ = 11 ๏ผ’.๏ผ’. OpenGL ๊ธฐ๋ฐ˜ 3D CAD ์–ดํ”Œ๋ฆฌ์ผ€์ด์…˜ ์„ฑ๋Šฅ ๋ถ„์„ = 18 ๏ผ’.๏ผ“. ๋งˆ์ดํฌ๋กœํ”„๋กœ์„ธ์„œ ์„ฑ๋Šฅ์— ๋”ฐ๋ฅธ 3D ๊ทธ๋ž˜ํ”ฝ์Šค ์„ฑ๋Šฅ ๋ณ€ํ™” = 25 ๏ผ“. ๊ธฐ์–ต์žฅ์น˜ ์šฉ๋Ÿ‰ ๋ณ€ํ™”์— ๋”ฐ๋ฅธ 3D ๊ทธ๋ž˜ํ”ฝ์Šค ์„ฑ๋Šฅ ๋ณ€ํ™” = 28 ๏ผ“.๏ผ‘. ๋งˆ์ดํฌ๋กœํ”„๋กœ์„ธ์„œ์™€ ์ฃผ๊ธฐ์–ต์žฅ์น˜ ๊ตฌ์„ฑ์— ๋”ฐ๋ฅธ ์„ฑ๋Šฅ ๋ณ€ํ™” = 28 ๏ผ“.๏ผ’. ๋ณด์กฐ๊ธฐ์–ต์žฅ์น˜ ์šด์šฉ์— ๋”ฐ๋ฅธ 3D ๊ทธ๋ž˜ํ”ฝ์Šค ์„ฑ๋Šฅ ๋ณ€ํ™” = 38 ๏ผ“.๏ผ’.๏ผ‘. I/O ์„œ๋ธŒ์‹œ์Šคํ…œ ๋ณ€ํ™”์— ๋”ฐ๋ฅธ ์„ฑ๋Šฅ ๊ฐœ์„  = 38 ๏ผ“.๏ผ’.๏ผ’. ๊ฐ€์ƒ ๊ธฐ์–ต์žฅ์น˜ ๋ณ€ํ™”์— ๋”ฐ๋ฅธ 3D ๊ทธ๋ž˜ํ”ฝ์Šค ์„ฑ๋Šฅ ๋ณ€ํ™” = 39 ๏ผ”. ๊ทธ๋ž˜ํ”ฝ์Šค ์„œ๋ธŒ์‹œ์Šคํ…œ์— ๋”ฐ๋ฅธ OpenGL ๊ฐ€์† ์„ฑ๋Šฅ ๋ณ€ํ™” = 41 ๏ผ”.๏ผ‘. OpenGL ๊ทธ๋ž˜ํ”ฝ์Šค ์„œ๋ธŒ์‹œ์Šคํ…œ์— ๋”ฐ๋ฅธ 3D ๊ทธ๋ž˜ํ”ฝ์Šค ์„ฑ๋Šฅ = 45 ๏ผ”.๏ผ’. OpenGL 3D ์„ฑ๋Šฅ ์š”์†Œ ๋ถ„์„ = 53 ๏ผ”.๏ผ“. ๊ทธ๋ž˜ํ”ฝ์Šค ์„œ๋ธŒ์‹œ์Šคํ…œ ์„ค์ •์— ๋”ฐ๋ฅธ 3D-API ๊ฐ€์† ์„ฑ๋Šฅ ๋ถ„์„ = 55 ๏ผ”.๏ผ”. ๊ทธ๋ž˜ํ”ฝ์Šค ์„œ๋ธŒ์‹œ์Šคํ…œ์˜ 3D CAD ์–ดํ”Œ๋ฆฌ์ผ€์ด์…˜ ์„ฑ๋Šฅ ๋ถ„์„ = 67 ๏ผ”.๏ผ•. ๋“œ๋ผ์ด๋ฒ„ ๊ฐœ์ •์— ์˜ํ•œ OpenGL ๊ฐ€์† ์„ฑ๋Šฅ ๋ณ€ํ™” = 77 ๏ผ•. ์šด์˜ ํ™˜๊ฒฝ์— ๋”ฐ๋ฅธ 3D ๊ทธ๋ž˜ํ”ฝ์Šค ์„ฑ๋Šฅ ๋ถ„์„ = 82 ๏ผ•.๏ผ‘. ์šด์˜ ์ฒด์ œ์— ๋”ฐ๋ฅธ 3D ๊ทธ๋ž˜ํ”ฝ์Šค ์„ฑ๋Šฅ ๋ณ€ํ™” = 82 ๏ผ•.๏ผ’. OpenGL ํ”„๋กœ๊ทธ๋ž˜๋ฐ ๋‹จ๊ณ„์˜ ์„ฑ๋Šฅ ์ €ํ•˜ ์š”์†Œ ๋ถ„์„ = 90 ๏ผ–. ๊ณ ์ฐฐ = 93 ๏ผ–.๏ผ‘. ๋งˆ์ดํฌ๋กœํ”„๋กœ์„ธ์„œ์™€ ๊ธฐ์–ต์žฅ์น˜ ๊ตฌ์„ฑ = 93 ๏ผ–.๏ผ’. ๊ทธ๋ž˜ํ”ฝ์Šค ์„œ๋ธŒ์‹œ์Šคํ…œ ๊ตฌ์„ฑ = 98 ๏ผ–.๏ผ“. ์šด์˜ ํ™˜๊ฒฝ ๊ฐœ์„ ์— ์˜ํ•œ ์„ฑ๋Šฅ ๋ณ€ํ™” = 99 ๏ผ—. ๊ฒฐ๋ก  = 10

    Comparison of Unmonochromatized Synchrotron Radiation and Conventional X-rays in the Imaging of Mammographic Phantom and Human Breast Specimens: A Preliminary Result

    Get PDF
    A simple imaging setup based on the principle of coherence-based contrast X-ray imaging with unmonochromatized synchrotron radiation was used for studying mammographic phantom and human breast specimens. The use of unmonochromatized synchrotron radiation simplifies the instrumentation, decreases the cost and makes the procedure simpler and potentially more suitable for clinical applications. The imaging systems consisted of changeable silicon wafer attenuators, a tungsten slit system, a CdWO4 scintillator screen, a CCD (Charge Coupled Device) camera coupled to optical magnification lenses, and a personal computer. In preliminary studies, a spatial resolution test pattern and glass capillary filled with air bubbles were imaged to evaluate the resOolution characteristics and coherence-based contrast enhancement. Both the spatial resolution and image quality of the proposed system were compared with those of a conventional mammography system in order to establish the characteristic advantages of this approach. The images obtained with the proposed system showed a resolution of at least 25 ยตm on the test pattern with much better contrast, while the images of the capillary filled with air bubbles revealed coherence-based edge enhancement. This result shows that the coherence-based contrast imaging system, which emphasizes the refraction effect from the edge of materials of different refractive indexes, is applicable to imaging studies in fundamental medicine and biology, although further research works will be required before it can be used for clinical applications.ope

    Assessment of Attenuation Correction Techniques with a 137Cs Point Source

    Get PDF
    Purpose: The objective of this study was to assess attenuation correction algorithms with the 137Cs point source for the brain positron emission tomography (PET) imaging process. Materials & Methods: Four different types of phantoms were used in this study for testing various types of the attenuation correction techniques. Transmission data of a 137Cs point source were acquired after infusing the emission source into phantoms and then the emission data were subsequently acquired in 3D acquisition mode. Scatter corrections were performed with a background tail-fitting algorithm. Emission data were then reconstructed using iterative reconstruction method with a measured (MAC), elliptical (ELAC), segmented (SAC) and remapping (RAC) attenuation correction, respectively. Reconstructed images were then both qualitatively and quantitatively assessed. In addition, reconstructed images of a normal subject were assessed by nuclear medicine physicians. Subtracted images were also compared. Results: ELAC, SAC, and RAC provided a uniform phantom image with less noise for a cylindrical phantom. In contrast, a decrease in intensity at the central portion of the attenuation map was noticed at the result of the MAC. Reconstructed images of Jaszack and Hoffan phantoms presented better quality with RAC and SAC. The attenuation of a skull on images of the normal subject was clearly noticed and the attenuation correction without considering the attenuation of the skull resulted in artificial defects on images of the brain. Conclusion: the complicated and improved attenuation correction methods were needed to obtain the better accuracy of the quantitative brain PET images.ope

    Three-dimensional image analysis of the skull using variable CT scanning protocols-effect of slice thickness on measurement in the three-dimensional CT images

    Get PDF
    Purpose : To evaluate the quantitative accuracy of three-dimensional (3D) images by means of comparing distance measurements on the 3D images with direct measurements of dry human skull according to slice thickness and scanning modes. Materials and Mathods : An observer directly measured the distance of 21 line items between 12 orthodontic landmarks on the skull surface using a digital vernier caliper and each was repeated five times. The dry human skull was scanned with a Helical CT with various slice thickness (3, 5, 7 mm) and acquisition modes (Conventional and Helical). The same observer measured corresponding distance of the same items on reconstructed 3D images with the internal program of V-works 4.0/supTM(Cybermed Inc., Seoul, Korea). The quantitative accuracy of distance measurements were statistically evaluated with Wilcoxons' two-sample test. Results: 11 line items in Conventional 3 mm, 8 in Helical 3mm, 11 in Conventional 5mm, 10 in Helical 5mm, 5 in Conventional 7mm and 9 in Helical 7mm showed no statistically significant difference. Average difference between direct measurements and measurements on 3D CT images was within 2mm in 19 line items of Conventional 3mm, 20 of Helical 3mm, 15 of Conventional 5mm, 18 of Helical 5mm, II of Conventional 7mm and 16 of Helical 7mm. Conclusion: Considering image quality and patient's exposure time, scanning protocol of Helical 5mm is recommended for 3D image analysis of the skull in CT.ope

    Transflective LCD using hybrid substrate made by soft lithography

    No full text
    ํ•™์œ„๋…ผ๋ฌธ(์„์‚ฌ) --์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :์ „๊ธฐ. ์ปดํ“จํ„ฐ๊ณตํ•™๋ถ€, 2009.2.Maste

    A Study of cavity varnish application on the marginal leakage of the various dental restorations

    No full text
    ์น˜์˜ํ•™๊ณผ/์„์‚ฌ[์˜๋ฌธ] [ํ•œ๊ธ€] ๋ชจ๋“  ์น˜๊ณผ์šฉ ์ถฉ์ „๋ฌผ์€ ๋ณ€์—ฐ๋ˆ„์ถœ์ด ์ผ์–ด๋‚œ๋‹ค. ์ด ๋ณ€์—ฐ๋ˆ„์ถœ์„ ๋ง‰๊ธฐ ์œ„ํ•˜์—ฌ ์น˜๊ณผ์šฉ varnis h๋ฅผ ์•„๋ง๊ฐ ์ถฉ์ „์—์„œ ํŠนํžˆ ๋งŽ์ด ์‚ฌ์šฉํ•˜๊ณ  ์žˆ๋‹ค. ์ด์— ์ €์ž๋Š” copal resin varnish์ธ Copa lite**(R) (Cooley and Cooley, Ltd., Houston, Texas, U.S.A.)์™€ ๋ถˆ์†Œ๊ฐ€ ํ•จ์œ ๋œ Durapha t**(R) (Woelm Pharma., Eschwege, West Germany)์˜ ๋ณ€์—ฐํ์‡„ ํšจ๊ณผ๋ฅผ ๊ตฌ๋ช…ํ•˜๊ณ ์ž ๋ฐœ๊ฑฐ๋œ ์ƒํ•˜์•… ์†Œ๊ตฌ์น˜ 120๊ฐœ ํ˜‘๋ฉด๊ณผ ์„ค๋ฉด์— 240๊ฐœ์˜ 5๊ธ‰ ์™€๋™์„ ํ˜•์„ฑํ•˜๊ณ  varnish๋ฅผ 1ํšŒ, 2ํšŒ ๋˜ ๋Š” 3ํšŒ์”ฉ ๋„ํฌํ•˜๊ณ  Amalgam(Cavex, Holland BV Keur and Sneltjes), Heliosit**(R) (Viva dent, Schaan, Liechitenstein) ๊ทธ๋ฆฌ๊ณ  Hipol**(R) (๋ถ€ํ‰์น˜๊ณผํ™”ํ•™๊ณต์—…์‚ฌ, ์ธ์ฒœ, ํ•œ๊ตญ)๋กœ ์ถฉ์ „ํ•˜์˜€๋‹ค. ๊ทธํ›„ 24์‹œ๊ฐ„ ์ƒ๋ฆฌ์  ์‹์—ผ์ˆ˜์— ๋ณด๊ด€ 50ํšŒ์˜ ์˜จ๋„๋ณ€ํ™”๋ฅผ, 72์‹œ๊ฐ„ ์ƒ๋ฆฌ์  ์‹์—ผ ์ˆ˜์— ๋ณด๊ด€ 100ํšŒ์˜ ์˜จ๋„๋ณ€ํ™”๋ฅผ ๊ฐ๊ฐ 120๊ฐœ์˜ ์™€๋™์— ์‹ค์‹œํ•˜๊ณ  2% methylene blue์— 24์‹œ ๊ฐ„ ์นจ์œค์‹œ์ผฐ๋‹ค. ์‹œํŽธ์„ ๊ต์ •์šฉ ๋ ˆ์ง„์— ํฌ๋งคํ•œ ํ›„ ์ ˆ๋‹จํ•˜๊ณ  ์ƒ‰์†Œ์˜ ์นจํˆฌ ์ •๋„๋ฅผ ๊ธˆ์†ํ˜„๋ฏธ ๊ฒฝ(PME/MG, Olympus Optical Co., LTD., Japan)์œผ๋กœ ๊ด€์ฐฐํ•˜์—ฌ ๋‹ค์Œ๊ณผ ๊ฐ™์€ ๊ฒฐ๋ก ์„ ์–ป์—ˆ๋‹ค . 1. ์•„๋ง๊ฐ ์ถฉ์ „์‹œ Copalite**(R) 3ํšŒ ๋˜๋Š” Duraphat**(R) 1ํšŒ ๋„ํฌ์˜ ๊ฒฝ์šฐ๊ฐ€ varnish๋ฅผ ๋„ํฌํ•˜์ง€ ์•Š์€ ๊ตฐ๋ณด๋‹ค ๋ณ€์—ฐํŽ˜์‡„๊ฐ€ ์šฐ์ˆ˜ํ•˜์˜€๋‹ค. 2. Heliosit**(R) ๋˜๋Š” Hipol**(R) ์ถฉ์ „์‹œ varnish๋ฅผ ๋„ํฌํ•œ ๊ฒฝ์šฐ๊ฐ€ ๋„ํฌํ•˜์ง€ ์•Š์€ ๊ฒฝ ์šฐ๋ณด๋‹ค ๋ณ€์—ฐ๋ˆ„์ถœ์ด ๋งŽ์•˜๋‹ค. 3. ๋ชจ๋“  ์ถฉ์ „๊ตฐ์—์„œ Copalite**(R) ์™€ Duraphat**(R) ์‚ฌ์ด์—๋Š” ํ†ต๊ณ„์ ์œผ๋กœ ์œ ์˜ํ•  ๋งŒํ•œ ์ฐจ์ด๊ฐ€ ์—†์—ˆ๋‹ค.(P>0.05) 4. 50ํšŒ์™€ 100ํšŒ์˜ ์˜จ๋„๋ณ€ํ™” ์ฒ˜๋ฆฌ ์‚ฌ์ด์— ์•„๋ง๊ฐ์˜ ๋ณ€์—ฐ๋ˆ„์ถœ์€ ํ†ต๊ณ„์ ์œผ๋กœ ์œ ์˜ํ•  ๋งŒํ•œ ์ฐจ์ด๊ฐ€ ์žˆ์—ˆ์œผ๋‚˜ (P<0.05), Heliosit**(R) ๋˜๋Š” Hipol**(R) ์€ ์œ ์˜์ฐจ๋ฅผ ๋‚˜ํƒ€๋‚ด์ง€ ์•Š์•˜ ๋‹ค. (P>0.05) 5. Heliosit**(R) ์™€ Hipol**(R) ์‚ฌ์ด์˜ ๋ณ€์—ฐ๋ˆ„์ถœ์€ ํ†ต๊ณ„์ ์œผ๋กœ ์œ ์˜ํ•  ๋งŒํ•œ ์ฐจ์ด๊ฐ€ ์—† ์—ˆ๋‹ค. A STUDY OF CAVITY VARNISH APPLICATION OF THE MARGINAL LEAKAGE OF THE VARIOUS DENTAL RESTORATIONS Hee Joong Kim, D.D.S. Department of Dental Science, Graduate School, Yonsei Universtiy (Directe by Prof. Chung Suck Lee, D.D.S., Ph.D.) This study was undertaken to evaluate the effects of varnish application and thermocycling on the marginal leakage. 240 cavities of Class V were prepared on the 120 extracted premolars, and the cavities were filled with amalgam, Heliosit**(R) , and Hipol**(R) after application of Copalite**(R) or Duraphat**(R). All specimens were immersed in methylene blue solution for 24 hours after thermoparts. The sectioned specimens observed with the metallurgical microscope. The following results were obtained: 1. The marginal seal was more effective in the amalgam-filled cavitics after application of Copalite**(R) threethimes or an application of Duraphat**(R) varnish than in chose without varnish applicaions. 2. Of the composite resin-filled cavities, the leakage of the varnish applied cases showed much more than without aplication. 3. There was no significant difference in the effect of margical sealing between Copalite**(R) and Duraphar**(R) applications. 4. There was a significant difference in the degree of the marginal leakage of amalgam-filled cavities between the groups of thermocycling times, but no significant difference in resin-filled cavities. 5. There was no significant difference in the degree of the marginal leakage between the Heliosit**(R) and the Hipol**(R) resin-filled cavities.restrictio

    NPC ์ธ๋ฒ„ํ„ฐ์—์„œ์˜ PWM ๊ธฐ๋ฒ•์— ๊ด€ํ•œ ์—ฐ๊ตฌ

    No full text
    ํ•™์œ„๋…ผ๋ฌธ(์„์‚ฌ)--์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› :์ „๊ธฐ๊ณตํ•™๋ถ€,2000.Maste
    corecore