• 대한기계학회논문집B
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• 제35권7호
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• pp.685-691
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• 2011

본 연구는 도플러 광 단층촬영법이 미세유동 및 미세구조를 동시에 측정하는 첨단 장비임을 보일뿐 아니라 기존의 도플러 광 단층촬영법의 한계를 극복한 새로운 방법을 제시하였다. 기존의 도플러 광단층촬영법은 샘플로 입사되는 광과 같은 방향의 속도성분만을 측정할 수 있다. 본 연구에서는 임의의 속도벡터의 세 성분을 동시에 측정할 수 있는 다관점 도플러 광 단층촬영법을 개발하였고 심전도 게이트를 사용하여 맥동혈류유동의 3 차원 공간 내에서 위상속도 벡터장을 측정하는 심전도 게이트 다관점 도플러 광 단층촬영법의 타당성 조사를 햄스터 모래주머니 모델을 사용하여 수행하였다. 이를 통해 측정 가능한 속도성분의 수를 증가할 뿐 아니라 프레임 레이트가 심박에 비해 상대적으로 느리기 때문에 발생하는 엘리아싱 문제를 해결하였다.

• Imaging Science in Dentistry
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• 제46권3호
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• pp.173-178
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• 2016

Purpose: Optical coherence tomography (OCT) has been investigated as a novel diagnostic imaging tool. The utilisation of this equipment has been evaluated through several studies in the field of dentistry. The aim of this preliminary study was to determine through basic experiments the effectiveness of OCT in implant dentistry. Materials and Methods: To assess detection ability, we captured OCT images of implants in each of the following situations: (1) implants covered with mucosae of various thicknesses that were harvested from the mandibles of pigs; (2) implants installed in the mandibles of pigs; and (3) implants with abutments and crowns fixed with temporary cement. The OCT images were captured before cementation, after cementation, and after removing the excess submucosal cement. Results: If the thickness of the mucosa covering the implant body was less than 1 mm, the images of the implants were clearly detected by OCT. In the implants were installed in pigs' mandibles, it was difficult to capture clear images of the implant and alveolar bone in most of the samples. Remnants of excess cement around the implants were visible in most samples that had a mucosa thickness of less than 3 mm. Conclusion: Currently, OCT imaging of implants is limited. Cement remnants at the submucosal area can be detected in some cases, which can be helpful in preventing peri-implant diseases. Still, though there are some restrictions to its application, OCT could have potential as an effective diagnostic instrument in the field of implant dentistry as well.

• Journal of Periodontal and Implant Science
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• 제47권1호
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• pp.13-19
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• 2017

Purpose: The purpose of this study was to examine whether periodontal pocket could be satisfactorily visualized by optical coherence tomography (OCT) and to suggest quantitative methods for measuring periodontal pocket depth. Methods: We acquired OCT images of periodontal pockets in a porcine model and determined the actual axial resolution for measuring the exact periodontal pocket depth using a calibration method. Quantitative measurements of periodontal pockets were performed by real axial resolution and compared with the results from manual periodontal probing. Results: The average periodontal pocket depth measured by OCT was $3.10{\pm}0.15mm$, $4.11{\pm}0.17mm$, $5.09{\pm}0.17mm$, and $6.05{\pm}0.21mm$ for each periodontal pocket model, respectively. These values were similar to those obtained by manual periodontal probing. Conclusions: OCT was able to visualize periodontal pockets and show attachment loss. By calculating the calibration factor to determine the accurate axial resolution, quantitative standards for measuring periodontal pocket depth can be established regardless of the position of periodontal pocket in the OCT image.

• Journal of Periodontal and Implant Science
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• 제47권1호
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• pp.41-50
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• 2017

Purpose: The aims of the present study were to compare the image quality and visibility of tooth cracks between conventional methods and swept-source optical coherence tomography (SS-OCT) and to develop an automatic detection technique for tooth cracks by SS-OCT imaging. Methods: We evaluated SS-OCT with a near-infrared wavelength centered at 1,310 nm over a spectral bandwidth of 100 nm at a rate of 50 kHz as a new diagnostic tool for the detection of tooth cracks. The reliability of the SS-OCT images was verified by comparing the crack lines with those detected using conventional methods. After performing preprocessing of the obtained SS-OCT images to emphasize cracks, an algorithm was developed and verified to detect tooth cracks automatically. Results: The detection capability of SS-OCT was superior or comparable to that of trans-illumination, which did not discriminate among the cracks according to depth. Other conventional methods for the detection of tooth cracks did not sense initial cracks with a width of less than $100{\mu}m$. However, SS-OCT detected cracks of all sizes, ranging from craze lines to split teeth, and the crack lines were automatically detected in images using the Hough transform. Conclusions: We were able to distinguish structural cracks, craze lines, and split lines in tooth cracks using SS-OCT images, and to automatically detect the position of various cracks in the OCT images. Therefore, the detection capability of SS-OCT images provides a useful diagnostic tool for cracked tooth syndrome.

• Journal of Veterinary Science
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• 제22권5호
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• pp.65.1-65.12
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• 2021

Background: To assess the normal retina of the pigeon eye using spectral domain optical coherence tomography (SD-OCT) and establish a normative reference. Methods: Twelve eyes of six ophthalmologically normal pigeons (Columba livia) were included. SD-OCT images were taken with dilated pupils under sedation. Four meridians, including the fovea, optic disc, red field, and yellow field, were obtained in each eye. The layers, including full thickness (FT), ganglion cell complex (GCC), thickness from the retinal pigmented epithelium to the outer nuclear layer (RPE-ONL), and from the retinal pigmented epithelium to the inner nuclear layer (RPE-INL), were manually measured. Results: The average FT values were significantly different among the four meridians (p < 0.05), with the optic disc meridian being the thickest (294.0 ± 13.9 ㎛). The average GCC was thickest in the optic disc (105.3 ± 27.1 ㎛) and thinnest in the fovea meridian (42.8 ± 15.3 ㎛). The average RPE-INL of the fovea meridian (165.5 ± 18.3 ㎛) was significantly thicker than that of the other meridians (p < 0.05). The average RPE-ONL of the fovea, optic disc, yellow field, and red field were 91.2 ± 5.2 ㎛, 87.7 ± 5.3 ㎛, 87.6 ± 6.5 ㎛, and 91.4 ± 3.9 ㎛, respectively. RPE-INL and RPE-ONL thickness of the red field meridian did not change significantly with measurement location (p > 0.05). Conclusions: Measured data could be used as normative references for diagnosing pigeon retinopathies and further research on avian fundus structure.

• BMB Reports
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• 제55권6호
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• pp.267-274
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• 2022

Molecular imaging is used to improve the disease diagnosis, prognosis, monitoring of treatment in living subjects. Numerous molecular targets have been developed for various cellular and molecular processes in genetic, metabolic, proteomic, and cellular biologic level. Molecular imaging modalities such as Optical Imaging, Magnetic Resonance Imaging (MRI), Positron Emission Tomography (PET), Single Photon Emission Computed Tomography (SPECT), and Computed Tomography (CT) can be used to visualize anatomic, genetic, biochemical, and physiologic changes in vivo. For in vivo cell imaging, certain cells such as cancer cells, immune cells, stem cells could be labeled by direct and indirect labeling methods to monitor cell migration, cell activity, and cell effects in cell-based therapy. In case of cancer, it could be used to investigate biological processes such as cancer metastasis and to analyze the drug treatment process. In addition, transplanted stem cells and immune cells in cell-based therapy could be visualized and tracked to confirm the fate, activity, and function of cells. In conventional molecular imaging, cells can be monitored in vivo in bulk non-invasively with optical imaging, MRI, PET, and SPECT imaging. However, single cell imaging in vivo has been a great challenge due to an extremely high sensitive detection of single cell. Recently, there has been great attention for in vivo single cell imaging due to the development of single cell study. In vivo single imaging could analyze the survival or death, movement direction, and characteristics of a single cell in live subjects. In this article, we reviewed basic principle of in vivo molecular imaging and introduced recent studies for in vivo single cell imaging based on the concept of in vivo molecular imaging.

• 비파괴검사학회지
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• 제31권5호
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• pp.466-471
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• 2011

광 단층촬영기법은 의료영상진단 기기로 최근에 주목받고 있는 분야이다. 현재 병원 초음파보다 공간 해상도가 10-100배 우수하지만 침투깊이가 조직 내에서 1-2 mm로 얇기 때문에 인체 내 장기 이미징을 위하여서 반드시 내시경 기법을 동반하여야 한다. 본 연구를 통하여 고속 광 단층촬영기법을 소개하고 초소형 기전공학 기술을 바탕으로 개발된 내시경을 사용하여 New Zealand white rabbit의 식도와 위장 벽을 3차원으로 이미징한 결과를 고찰하였다. 개발된 내시경에는, 2축 스캔 반사경이 정전기력에 의하여 구동하는 구 동부 위에 위치하여, 입력광을 2축으로 스캔할 수 있도록 하는 구조를 포함하고 있다. 내시경의 외경은 6 mm이며 스캔 반사경의 직경은 1.2 mm 였다. 3.5초 동안 스캔하면서 3차원 이미지를 획득하였다. 3차원 이미지는 200개의 2차원 이미지를 쌓아서 구현되었으며 각각의 2차원 단면이미지는 $200{\times}500$ 픽셀들로 구성되었다. 이미지의 공간해상도는 공기 중에서 8 ${\mu}m$ 였다.

• 치위생과학회지
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• 제16권4호
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• pp.257-262
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• 2016

TMR은 초기우식 평가의 gold standard로 여겨지나 시편을 파괴하여야만 시편의 무기질 밀도를 확인할 수 있는 실험법이다. 그러나 OCT는 비파괴적인 검사법으로 임상에서도 초기우식을 확인하는 데 사용하므로 본 연구에서는 $200{\mu}m$ 이상의 깊은 법랑질 초기우식에서의 OCT와 TMR에서 구한 integrated mineral loss값 간의 상관성을 확인하고자 하였다. $200{\mu}m$ 이상의 깊이를 갖는 인공 초기우식병소를 제작하여 TMR (${\Delta}Z_{TMR}$)과 OCT (${\Delta}R_{OCT}$)에서 구한 integrated mineral loss를 각각 구하여 상관성 분석을 시행하였으며 Bland-Altman plot을 그려 두 값 간의 오차 분석을 시행하였다. ${\Delta}R_{OCT}$과 ${\Delta}Z_{TMR}$ 간에는 유의한 상관성이 확인되었으며(r=0.491, p=0.003), Bland-Altman plot 상에서도 ${\Delta}Z_{TMR}$과 ${\Delta}R_{OCT}$값 간의 차이가 거의 대부분 오차 구간 내에 있는 것이 확인되어 두 측정 방법 간의 오차가 적은 것으로 확인되었다. 따라서 치과임상에서 OCT를 활용하면 초기우식병소의 탐지 및 모니터링 그리고 초기우식병소의 심도 파악이 가능할 것으로 여겨진다.

• Korean Journal of Ophthalmology
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• 제32권6호
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• pp.506-516
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• 2018

Purpose: We measured the thicknesses of the ganglion cell and inner plexiform layer (GCIPL), the macula, and the retinal nerve fiber layer (RNFL) using spectral-domain optical coherence tomography in patients with idiopathic macula holes to analyze the repeatability of these measurements and compare them with those of the fellow eye. Methods: We evaluated 85 patients who visited our retinal clinic. The patients were divided into two groups according to their macular hole size: group A had a size of $<400{\mu}m$, while group B had a size of ${\geq}400{\mu}m$. Repeatability was determined by comparing the thicknesses of the GCIPL, macula, and RNFL with those of the normal fellow eye. Results: The average central macular thickness in patients with macular holes was significantly thicker than that in the normal fellow eye ($343.8{\pm}78.6$ vs. $252.6{\pm}62.3{\mu}m$, p < 0.001). The average thickness of the GCIPL in patients with macular holes was significantly thinner than that in the normal fellow eye ($56.1{\pm}23.4$ vs. $77.1{\pm}12.8{\mu}m$, p < 0.001). There was no significant difference in the average RNFL thickness between eyes with macular holes and fellow eyes ($92.4{\pm}10.0$ vs. $95.5{\pm}10.7{\mu}m$, p = 0.070). There were also no significant differences in the thicknesses of the GCIPL and RNFL among the two groups (p = 0.786 and p = 0.516). The intraclass correlation coefficients for the macula and RNFL were 0.994 and 0.974, respectively, in patients with macular holes, while that for the GCIPL was 0.700. Conclusions: Macular contour change with macular hole results in low repeatability and a tendency of thinner measurement regarding GCIPL thickness determined via spectral-domain optical coherence tomography. The impact of changes in the macular shape caused by macular holes should be taken into consideration when measuring the GCIPL thickness in patients with various eye diseases such as glaucoma and in those with neuro-ophthalmic disorders.

• Journal of the Optical Society of Korea
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• 제15권4호
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• pp.386-393
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• 2011

In this study, we report an effective k-domain linearization method with a pre-calibrated indexed look-up table. The method minimizes k-domain nonlinear characteristics of a swept source optical coherence tomography (SS-OCT) system by using two arrays, a sample position shift index and an intensity compensation array. Two arrays are generated from an interference pattern acquired by connecting a Fabry-Perot interferometer (FPI) and an optical spectrum analyzer (OSA) to the system. At real time imaging, the sample position is modified by location movement and intensity compensation with two arrays for linearity of wavenumber. As a result of evaluating point spread functions (PSFs), the signal to noise ratio (SNR) is increased by 9.7 dB. When applied to infrared (IR) sensing card imaging, the SNR is increased by 1.29 dB and the contrast noise ratio (CNR) value is increased by 1.44. The time required for the linearization and intensity compensation is 30 ms for a multi thread method using a central processing unit (CPU) compared to 0.8 ms for compute unified device architecture (CUDA) processing using a graphics processing unit (GPU). We verified that our linearization method is appropriate for applying real time imaging of SS-OCT.