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  <channel rdf:about="https://scholar.dgist.ac.kr/handle/20.500.11750/11758">
    <title>Repository Community: null</title>
    <link>https://scholar.dgist.ac.kr/handle/20.500.11750/11758</link>
    <description />
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        <rdf:li rdf:resource="https://scholar.dgist.ac.kr/handle/20.500.11750/60548" />
        <rdf:li rdf:resource="https://scholar.dgist.ac.kr/handle/20.500.11750/60243" />
        <rdf:li rdf:resource="https://scholar.dgist.ac.kr/handle/20.500.11750/59938" />
        <rdf:li rdf:resource="https://scholar.dgist.ac.kr/handle/20.500.11750/59239" />
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    <dc:date>2026-08-10T14:29:02Z</dc:date>
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  <item rdf:about="https://scholar.dgist.ac.kr/handle/20.500.11750/60548">
    <title>Approximate Cramér-Rao lower bound analyses for semi-optimal energy thresholds selection in photon counting CT</title>
    <link>https://scholar.dgist.ac.kr/handle/20.500.11750/60548</link>
    <description>Title: Approximate Cramér-Rao lower bound analyses for semi-optimal energy thresholds selection in photon counting CT
Author(s): Lee, Okkyun
Abstract: Background Selecting energy thresholds in photon counting CT (PCCT) is crucial for reducing noise in material decomposition. Theoretically, it can be determined by analyzing the Cram &amp; eacute;r-Rao lower bound (CRLB). However, the CRLB analysis is challenging in practice without complete knowledge of system models.Purpose This study aims to develop a practical method for selecting semi-optimal energy thresholds in PCCT without the system models.Methods We proposed approximate CRLB approaches, linear and nonlinear. It only needs to generate look-up tables of measured counts using a threshold scan for reference slab phantoms, which roughly model the largest basis line integrals in the object. We also introduced total noise, which summarizes the noise in the basis line integrals and can be calculated from the look-up table; one can select energy thresholds that yield the minimum total noise. The proposed methods were validated using the PcTK toolbox in simulation studies for two- and three-material decomposition for various numbers of energy thresholds. The proposed methods were compared to the theoretically optimal CRLB analysis and the condition of equally distributed counts (EDC). It was also validated using a bench-top PCCT system for two-material decomposition with two energy thresholds.Results In simulation studies, all methods showed similar total noises for two-material decomposition. For the three-material decomposition, the proposed methods showed lower or similar noise levels compared to the EDC condition. All methods showed higher noise than the optimal one, except the proposed nonlinear approach, which exhibited the optimal noise level at four energy bins. In experiments, the proposed linear method achieved a near-optimal performance in a two-material decomposition, while the EDC condition increased noise levels by 15% and 18% for epoxy resin and CaHA, respectively.Conclusions The proposed energy threshold selection methods are practical and effective: they require only a threshold scan of the reference phantoms and are computationally efficient. It outperformed the existing EDC condition in both simulation and experimental studies. It also showed a near-optimal noise level across various conditions, except in the three-material with three-energy-bin case.</description>
    <dc:date>2026-06-30T15:00:00Z</dc:date>
  </item>
  <item rdf:about="https://scholar.dgist.ac.kr/handle/20.500.11750/60243">
    <title>포톤카운팅 CT 기반의 물질 분리에서의 이웃간 우도를 활용한 노이즈 제거 장치 및 그 방법</title>
    <link>https://scholar.dgist.ac.kr/handle/20.500.11750/60243</link>
    <description>Title: 포톤카운팅 CT 기반의 물질 분리에서의 이웃간 우도를 활용한 노이즈 제거 장치 및 그 방법
Author(s): 이옥균
Abstract: 본 발명은 포톤카운팅 CT 기반의 물질 분리에서의 이웃간 우도를 활용한 노이즈 제거 장치 및 그 방법에 관한 것이다. 본 발명에 따르면, 노이즈 제거 장치는 최대 우도(Maximum Likelihood)를 기반으로 물질 분리가 완료된 물질별 사이노그램 영상을 획득하는 영상 획득부, 상기 물질별 사이노그램 영상에 포함된 복수의 픽셀 중에서 노이즈 제거를 하고자 하는 특정 픽셀을 선택하고, 광자 계수 검출기(PCD)로부터 상기 특정 픽셀에 대응되는 기준 측정값을 획득하는 측정값 획득부, 상기 특정 픽셀을 중심으로 인접하는 제1 픽셀 및 제2 픽셀을 추출하고, 상기 획득한 기준 측정값을 이용하여 제1 픽셀 및 제2 픽셀에 대응되는 각각의 우도를 계산한 다음, 계산된 우도를 이용하여 특정 픽셀, 제1 픽셀 및 제2 픽셀에 각각의 가중치를 부여하는 분석부, 상기 산출된 가중치를 우도 기반의 양방향 필터(Likelihood-based Bilateral Filter, LBF)에 적용하여 노이즈를 제거하는 필터링부, 그리고 노이즈가 제거된 물질별 사이노그램 영상을 획득하고, 획득한 물질별 사이노그램 영상에 역투영(Filtered Backprojection, FBP) 알고리즘을 적용하여 최종 물질별 영상을 획득하는 제어부를 포함한다.</description>
  </item>
  <item rdf:about="https://scholar.dgist.ac.kr/handle/20.500.11750/59938">
    <title>Single-Exposure Material Decomposition in Chest Tomosynthesis with a CdTe Photon-Counting Detector</title>
    <link>https://scholar.dgist.ac.kr/handle/20.500.11750/59938</link>
    <description>Title: Single-Exposure Material Decomposition in Chest Tomosynthesis with a CdTe Photon-Counting Detector
Author(s): Lee, Soohyun; Lim, Younghwan; Park, Sungmin; Lee, Okkyun; Cha, Bo Kyung; Cho, Hyosung
Abstract: Dual-energy material decomposition enables differentiation of soft tissue and bone in X-ray imaging; however, conventional methods require two sequential exposures, increasing radiation dose, acquisition time, and the risk of misregistration. This study presents a single-exposure material decomposition method using a cadmium telluride (CdTe)-based photon-counting detector (PCD) integrated with digital tomosynthesis (DTS). The proposed framework consists of three key steps: 1) simultaneous acquisition of low- and high-energy projections with dual thresholds (25 and 65 keV), 2) calibration-based decomposition using a PMMA–Al wedge phantom, and 3) projection-domain material separation followed by DTS reconstruction. Validation through both simulation and experimental studies demonstrated accurate separation of soft-tissue and bone components, high projection-level decomposition precision (RMSE: 0.052 for PMMA; 0.012 for Al), and improved perceptual image quality (SSIM: 0.979 and 0.974; PSNR: 37.6 and 38.6 dB). Compared with conventional energy-integrating detector (EID)-based dual-energy methods, the proposed PCD-based approach achieved superior structural preservation, contrast uniformity, and image interpretability. Beyond chest imaging, this single-exposure PCD framework is also applicable to non-medical X-ray applications, such as industrial nondestructive testing, security screening, and material characterization.</description>
    <dc:date>2026-04-30T15:00:00Z</dc:date>
  </item>
  <item rdf:about="https://scholar.dgist.ac.kr/handle/20.500.11750/59239">
    <title>Material decomposition-based improved normalized metal artifact reduction method (MD-NMAR) in photon counting CT</title>
    <link>https://scholar.dgist.ac.kr/handle/20.500.11750/59239</link>
    <description>Title: Material decomposition-based improved normalized metal artifact reduction method (MD-NMAR) in photon counting CT
Author(s): Nam, Jeonghyeon; Kim, Joonbeom; Ye, Dong Hye; Lee, Okkyun
Abstract: Photon counting computed tomography (PCCT) acquires multiple images of different energy ranges from a single computed tomography (CT) scan. It provides us with spatial and spectral information not available from conventional CT, making it possible for further analysis in the metal artifacts reduction (MAR). This study aims to develop a method to reduce metal artifacts in PCCT using material decomposition. We use the normalized MAR (NMAR) method and calibration data to obtain the initial basis material images. We correct the image of soft tissue using the NMAR and then correct the image of hard tissue by performing least squares fitting with virtual monochromatic images (VMIs). The artifact-reduced material images are reverted to the bin-wise images (CT images for each energy bin) and then employed as the improved prior images for the NMAR method to obtain the final MAR results: The metal artifact-reduced bin-wise CT images. In simulation results, the proposed method showed promising results, reducing metal artifacts compared to the original NMAR method applied to bin-wise images. For example, it reduced the root mean squared error values by an average of 6.3% for a dual-energy case. The proposed method also reproduced noticeable improvements in the table-top PCCT experiments compared to the conventional NMAR.</description>
    <dc:date>2025-08-31T15:00:00Z</dc:date>
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