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  • 1
    In: Medical Image Analysis, Elsevier BV, Vol. 71 ( 2021-07), p. 102061-
    Type of Medium: Online Resource
    ISSN: 1361-8415
    Language: English
    Publisher: Elsevier BV
    Publication Date: 2021
    detail.hit.zdb_id: 1497450-2
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  • 2
    In: Composites Part A: Applied Science and Manufacturing, Elsevier BV, Vol. 107 ( 2018-04), p. 354-365
    Type of Medium: Online Resource
    ISSN: 1359-835X
    Language: English
    Publisher: Elsevier BV
    Publication Date: 2018
    detail.hit.zdb_id: 1294545-6
    detail.hit.zdb_id: 2012223-8
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  • 3
    Online Resource
    Online Resource
    IOP Publishing ; 2002
    In:  Nanotechnology Vol. 13, No. 1 ( 2002-02-01), p. 23-28
    In: Nanotechnology, IOP Publishing, Vol. 13, No. 1 ( 2002-02-01), p. 23-28
    Type of Medium: Online Resource
    ISSN: 0957-4484 , 1361-6528
    Language: Unknown
    Publisher: IOP Publishing
    Publication Date: 2002
    detail.hit.zdb_id: 1362365-5
    SSG: 11
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  • 4
    In: AIDS Care, Informa UK Limited, Vol. 26, No. 3 ( 2014-03-04), p. 379-386
    Type of Medium: Online Resource
    ISSN: 0954-0121 , 1360-0451
    Language: English
    Publisher: Informa UK Limited
    Publication Date: 2014
    detail.hit.zdb_id: 2003080-0
    SSG: 5,2
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  • 5
    In: Acta Radiologica, SAGE Publications, Vol. 55, No. 1 ( 2014-02), p. 62-70
    Abstract: Three-dimensional (3D) roadmap is a recently developed imaging technique used to guide diagnostic and interventional catheter-directed procedures and mainly evaluated for neurovascular procedures. Few data with regard to efficacy and radiation dose are currently available in literature. Purpose To evaluate the use of 3D roadmap technique as compared with the conventional two-dimensional (2D) roadmap for uterine artery catheterization and embolization during uterine fibroid embolization and assess the potential impact on radiation dose, contrast load, and total procedure time. Material and Methods In this prospective study, 40 patients were randomly assigned to the 2D or 3D roadmap technique for uterine artery catheterization. Demographic data, specifically the patient’s age, weight, height, pelvic circumference, and total uterine and fibroid volume were recorded. Exposure parameters, contrast load, and procedure time were recorded and organ doses for ovaries and uterus were calculated. Results Demographic data did not differ between the groups. Catheterization and embolization of both uterine arteries were feasible in all patients, although in one patient in the 3D group, a focal dissection of the proximal uterine artery occurred. No significant difference in estimated ovarian dose was found in the 3D versus 2D group ( P = 0.07). Total procedure time was shorter in the 2D group ( P = 0.01) and no difference in total contrast load was seen ( P = 0.17). Conclusion Both roadmap techniques are effective imaging-guided tools for uterine artery catheterization, without difference in terms of radiation exposure or contrast load. The total procedure time is shorter in the 2D group.
    Type of Medium: Online Resource
    ISSN: 0284-1851 , 1600-0455
    RVK:
    Language: English
    Publisher: SAGE Publications
    Publication Date: 2014
    detail.hit.zdb_id: 2024579-8
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  • 6
    In: Medical Physics, Wiley, Vol. 50, No. 5 ( 2023-05), p. 2928-2938
    Abstract: Modelling of the 3D breast shape under compression is of interest when optimizing image processing and reconstruction algorithms for mammography and digital breast tomosynthesis (DBT). Since these imaging techniques require the mechanical compression of the breast to obtain appropriate image quality, many such algorithms make use of breast‐like phantoms. However, if phantoms do not have a realistic breast shape, this can impact the validity of such algorithms. Purpose To develop a point distribution model of the breast shape obtained through principal component analysis (PCA) of structured light (SL) scans from patient compressed breasts. Methods SL scans were acquired at our institution during routine craniocaudal‐view DBT imaging of 236 patients, creating a dataset containing DBT and SL scans with matching information. Thereafter, the SL scans were cleaned, merged, simplified, and set to a regular grid across all cases. A comparison between the initial SL scans after cleaning and the gridded SL scans was performed to determine the absolute difference between them. The scans with points in a regular grid were then used for PCA. Additionally, the correspondence between SL scans and DBT scans was assessed by comparing features such as the chest‐to‐nipple distance (CND), the projected breast area (PBA) and the length along the chest‐wall (LCW). These features were compared using a paired t‐test or the Wilcoxon signed rank sum test. Thereafter, the PCA shape prediction and SL scans were evaluated by calculating the mean absolute error to determine whether the model had adequately captured the information in the dataset. The coefficients obtained from the PCA could then parameterize a given breast shape as an offset from the sample means. We also explored correlations of the PCA breast shape model parameters with certain patient characteristics: age, glandular volume, glandular density by mass, total breast volume, compressed breast thickness, compression force, nipple location, and centre of the chest‐wall. Results The median value across cases for the 90 th and 99 th percentiles of the interpolation error between the initial SL scans after cleaning and the gridded SL scans was 0.50 and 1.16 mm, respectively. The comparison between SL and DBT scans resulted in small, but statistically significant, mean differences of 1.6 mm, 1.6 mm, and 2.2 cm 2 for the LCW, CND, and PBA, respectively. The final model achieved a median mean absolute error of 0.68 mm compared to the scanned breast shapes and a perfect correlation between the first PCA coefficient and the patient breast compressed thickness, making it possible to use it to generate new model‐based breast shapes with a specific breast thickness. Conclusion There is a good agreement between the breast shape coverage obtained with SL scans used to construct our model and the DBT projection images, and we could therefore create a generative model based on this data that is available for download on Github.
    Type of Medium: Online Resource
    ISSN: 0094-2405 , 2473-4209
    URL: Issue
    Language: English
    Publisher: Wiley
    Publication Date: 2023
    detail.hit.zdb_id: 1466421-5
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  • 7
    In: Medical Physics, Wiley, Vol. 50, No. 8 ( 2023-08), p. 4744-4757
    Abstract: Digital breast tomosynthesis (DBT) has gained popularity as breast imaging modality due to its pseudo‐3D reconstruction and improved accuracy compared to digital mammography. However, DBT faces challenges in image quality and quantitative accuracy due to scatter radiation. Recent advancements in deep learning (DL) have shown promise in using fast convolutional neural networks for scatter correction, achieving comparable results to Monte Carlo (MC) simulations. Purpose To predict the scatter radiation signal in DBT projections within clinically‐acceptable times and using only clinically‐available data, such as compressed breast thickness and acquisition angle. Methods MC simulations to obtain scatter estimates were generated from two types of digital breast phantoms. One set consisted of 600 realistically‐shaped homogeneous breast phantoms for initial DL training. The other set was composed of 80 anthropomorphic phantoms, containing realistic internal tissue texture, aimed at fine tuning the DL model for clinical applications. The MC simulations generated scatter and primary maps per projection angle for a wide‐angle DBT system. Both datasets were used to train (using 7680 projections from homogeneous phantoms), validate (using 960 and 192 projections from the homogeneous and anthropomorphic phantoms, respectively), and test (using 960 and 48 projections from the homogeneous and anthropomorphic phantoms, respectively) the DL model. The DL output was compared to the corresponding MC ground truth using both quantitative and qualitative metrics, such as mean relative and mean absolute relative differences (MRD and MARD), and to previously‐published scatter‐to‐primary (SPR) ratios for similar breast phantoms. The scatter corrected DBT reconstructions were evaluated by analyzing the obtained linear attenuation values and by visual assessment of corrected projections in a clinical dataset. The time required for training and prediction per projection, as well as the time it takes to produce scatter‐corrected projection images, were also tracked. Results The quantitative comparison between DL scatter predictions and MC simulations showed a median MRD of 0.05% (interquartile range (IQR), −0.04% to 0.13%) and a median MARD of 1.32% (IQR, 0.98% to 1.85%) for homogeneous phantom projections and a median MRD of −0.21% (IQR, −0.35% to −0.07%) and a median MARD of 1.43% (IQR, 1.32% to 1.66%) for the anthropomorphic phantoms. The SPRs for different breast thicknesses and at different projection angles were within ± 15% of the previously‐published ranges. The visual assessment showed good prediction capabilities of the DL model with a close match between MC and DL scatter estimates, as well as between DL‐based scatter corrected and anti‐scatter grid corrected cases. The scatter correction improved the accuracy of the reconstructed linear attenuation of adipose tissue, reducing the error from −16% and −11% to −2.3% and 4.4% for an anthropomorphic digital phantom and clinical case with similar breast thickness, respectively. The DL model training took 40 min and prediction of a single projection took less than 0.01 s. Generating scatter corrected images took 0.03 s per projection for clinical exams and 0.16 s for one entire projection set. Conclusions This DL‐based method for estimating the scatter signal in DBT projections is fast and accurate, paving the way for future quantitative applications.
    Type of Medium: Online Resource
    ISSN: 0094-2405 , 2473-4209
    URL: Issue
    Language: English
    Publisher: Wiley
    Publication Date: 2023
    detail.hit.zdb_id: 1466421-5
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  • 8
    In: Journal of Applied Clinical Medical Physics, Wiley, Vol. 12, No. 4 ( 2011-09), p. 245-260
    Abstract: Cone‐beam CT (CBCT) has shown to be a useful imaging modality for various dentomaxillofacial applications. However, optimization and quality control of dental CBCT devices is hampered due to the lack of an appropriate tool for image quality assessment. To investigate the application of different image quality parameters for CBCT, a prototype polymethyl methacrylate (PMMA) cylindrical phantom with inserts for image quality analysis was developed. Applicability and reproducibility of the phantom were assessed using seven CBCT devices with different scanning protocols. Image quality parameters evaluated were: CT number correlation, contrast resolution, image homogeneity and uniformity, point spread function, and metal artifacts. Deviations of repeated measurements were between 0.0% and 3.3%. Correlation coefficients of CBCT voxel values with CT numbers ranged between 0.68 and 1.00. Contrast‐to‐noise ratio (CNR) values were much lower for hydroxyapatite than for air and aluminum . Noise values ranged between 35 and 419. The uniformity index was between 3.3% and 11.9%. Full width at half maximum (FWHM) measurements varied between 0.43 mm and 1.07 mm. The increase of mean voxel values surrounding metal objects ranged between 6.7% and 43.0%. Results from preliminary analyses of the prototype quality control phantom showed its potential for routine quality assurance on CBCT. Large differences in image quality performance were seen between CBCT devices. Based on the initial evaluations, the phantom can be optimized and validated. PACS numbers: 87.57.C‐, 87.57.N‐, 87.57.Q‐
    Type of Medium: Online Resource
    ISSN: 1526-9914 , 1526-9914
    Language: English
    Publisher: Wiley
    Publication Date: 2011
    detail.hit.zdb_id: 2010347-5
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  • 9
    Online Resource
    Online Resource
    Wiley ; 2015
    In:  Medical Physics Vol. 42, No. 11 ( 2015-11), p. 6537-6548
    In: Medical Physics, Wiley, Vol. 42, No. 11 ( 2015-11), p. 6537-6548
    Abstract: The authors wish to evaluate the possible advantages of using a multigrid approach to maximum‐ a‐posteriori reconstruction in digital breast tomosynthesis together with block‐iterative updates in the form of either plane‐by‐plane updates or ordered subsets. Methods: The authors previously developed a penalized maximum likelihood reconstruction algorithm with resolution model dedicated to breast tomosynthesis [K. Michielsen et al. , “Patchwork reconstruction with resolution modeling for digital breast tomosynthesis,” Med. Phys. 40 , 031105 (10pp.) (2013)]. This algorithm was extended with ordered subsets and multigrid updates, and the effects on the convergence and on limited angle artifact appearance were evaluated on a mathematical phantom and patient data. To ensure a fair comparison, the analysis was performed at the same computational cost for all methods. To assess convergence and artifact creation in the phantom reconstructions, the authors looked at posterior likelihood, sum of squared residuals, contrast of identical calcifications at different positions, and the standard deviation between the contrasts of these calcifications. For the patient cases, the authors calculated posterior likelihood, measured the signal difference to noise ratio of subtle microcalcifications, and visually evaluated the reconstructions. Results: The authors selected multigrid sequences scoring in the best 10% of the four evaluated parameters, except for the reconstructions with subsets where a low standard deviation of the contrast was incompatible with the three other parameters. In further evaluation of phantom reconstructions from noisy data and patient data, the authors found improved convergence and a reduction in artifacts for our chosen multigrid reconstructions compared to the single grid reconstructions with equivalent computational cost, although there was a diminishing return for an increasing number of subsets. Conclusions: Multigrid reconstruction improves upon reconstruction with a fixed grid when evaluated at a fixed computational cost. For multigrid reconstruction, using plane‐by‐plane updates or applying ordered subsets resulted in similar performance.
    Type of Medium: Online Resource
    ISSN: 0094-2405 , 2473-4209
    Language: English
    Publisher: Wiley
    Publication Date: 2015
    detail.hit.zdb_id: 1466421-5
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  • 10
    In: Medical Physics, Wiley, Vol. 43, No. 12 ( 2016-12), p. 6577-6587
    Abstract: In this work, the authors design and validate a model observer that can detect groups of microcalcifications in a four‐alternative forced choice experiment and use it to optimize a smoothing prior for detectability of microcalcifications. Methods: A channelized Hotelling observer (CHO) with eight Laguerre–Gauss channels was designed to detect groups of five microcalcifications in a background of acrylic spheres by adding the CHO log‐likelihood ratios calculated at the expected locations of the five calcifications. This model observer is then applied to optimize the detectability of the microcalcifications as a function of the smoothing prior. The authors examine the quadratic and total variation (TV) priors, and a combination of both. A selection of these reconstructions was then evaluated by human observers to validate the correct working of the model observer. Results: The authors found a clear maximum for the detectability of microcalcification when using the total variation prior with weight β TV = 35. Detectability only varied over a small range for the quadratic and combined quadratic‐TV priors when weight β Q of the quadratic prior was changed by two orders of magnitude. Spearman correlation with human observers was good except for the highest value of β for the quadratic and TV priors. Excluding those, the authors found ρ = 0.93 when comparing detection fractions, and ρ = 0.86 for the fitted detection threshold diameter. Conclusions: The authors successfully designed a model observer that was able to predict human performance over a large range of settings of the smoothing prior, except for the highest values of β which were outside the useful range for good image quality. Since detectability only depends weakly on the strength of the combined prior, it is not possible to pick an optimal smoothness based only on this criterion. On the other hand, such choice can now be made based on other criteria without worrying about calcification detectability.
    Type of Medium: Online Resource
    ISSN: 0094-2405 , 2473-4209
    Language: English
    Publisher: Wiley
    Publication Date: 2016
    detail.hit.zdb_id: 1466421-5
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