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Mäkinen H, Suhonen H, Siiskonen T, David C, Huotari S. Optimization of contrast and dose in x-ray phase-contrast tomography with a Talbot-Lau interferometer. Biomed Phys Eng Express 2024; 10:045045. [PMID: 38815565 DOI: 10.1088/2057-1976/ad5206] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 02/02/2024] [Accepted: 05/30/2024] [Indexed: 06/01/2024]
Abstract
X-ray phase-contrast imaging has become a valuable tool for biomedical research due to its improved contrast abilities over regular attenuation-based imaging. The recently emerged Talbot-Lau interferometer can provide quantitative attenuation, phase-contrast and dark-field image data, even with low-brilliance x-ray tube sources. Thus, it has become a valid option for clinical environments. In this study, we analyze the effects of x-ray tube voltage and total number of images on the contrast-to-noise ratio (CNR) and dose-weighted CNR (CNRD) calculated from tomographic transmission and phase-contrast data of a phantom sample. Constant counting statistics regardless of the voltage was ensured by adjusting the image exposure time for each voltage setting. The results indicate that the x-ray tube voltage has a clear effect on both image contrast and noise. This effect is amplified in the case of phase-contrast images, which is explained by the polychromatic x-ray spectrum and the dependence of interferometer visibility on the spectrum. CNRD is additionally affected by the total imaging time. While submerging the sample into a water container effectively reduces image artefacts and improves the CNR, the additional attenuation of the water must be compensated with a longer exposure time. This reduces dose efficiency. Both the CNR and CNRD are higher in the phase-contrast images compared to transmission images. For transmission images, and phase-contrast images without the water container, CNRD can be increased by using higher tube voltages (in combination with a lower exposure time). For phase-contrast images with the water container, CNRD is increased with lower tube voltages. In general, the CNRD does not strongly depend on the number of tomographic angles or phase steps used.
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Affiliation(s)
- Henrik Mäkinen
- Department of Physics, PO Box 64, FI-00014 University of Helsinki, Finland
| | - Heikki Suhonen
- Department of Physics, PO Box 64, FI-00014 University of Helsinki, Finland
| | - Teemu Siiskonen
- Department of Physics, PO Box 64, FI-00014 University of Helsinki, Finland
- Measurements and Environmental Monitoring, Radiation and Nuclear Safety Authority (STUK), Jokiniemenkuja 1, FI-01370 Vantaa, Finland
| | - Christian David
- Paul Scherrer Institute, Forschungsstrasse 111, CH-5232 Villigen, Switzerland
| | - Simo Huotari
- Department of Physics, PO Box 64, FI-00014 University of Helsinki, Finland
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De Marco F, Andrejewski J, Urban T, Willer K, Gromann L, Koehler T, Maack HI, Herzen J, Pfeiffer F. X-Ray Dark-Field Signal Reduction Due to Hardening of the Visibility Spectrum. IEEE TRANSACTIONS ON MEDICAL IMAGING 2024; 43:1422-1433. [PMID: 38032773 DOI: 10.1109/tmi.2023.3337994] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 12/02/2023]
Abstract
X-ray dark-field imaging enables a spatially-resolved visualization of ultra-small-angle X-ray scattering. Using phantom measurements, we demonstrate that a material's effective dark-field signal may be reduced by modification of the visibility spectrum by other dark-field-active objects in the beam. This is the dark-field equivalent of conventional beam-hardening, and is distinct from related, known effects, where the dark-field signal is modified by attenuation or phase shifts. We present a theoretical model for this group of effects and verify it by comparison to the measurements. These findings have significant implications for the interpretation of dark-field signal strength in polychromatic measurements.
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Leatham TA, Paganin DM, Morgan KS. X-ray phase and dark-field computed tomography without optical elements. OPTICS EXPRESS 2024; 32:4588-4602. [PMID: 38297656 DOI: 10.1364/oe.509604] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/17/2023] [Accepted: 12/07/2023] [Indexed: 02/02/2024]
Abstract
X-ray diffusive dark-field imaging, which allows spatially unresolved microstructure to be mapped across a sample, is an increasingly popular tool in an array of settings. Here, we present a new algorithm for phase and dark-field computed tomography based on the x-ray Fokker-Planck equation. Needing only a coherent x-ray source, sample, and detector, our propagation-based algorithm can map the sample density and dark-field/diffusion properties of the sample in 3D. Importantly, incorporating dark-field information in the density reconstruction process enables a higher spatial resolution reconstruction than possible with previous propagation-based approaches. Two sample exposures at each projection angle are sufficient for the successful reconstruction of both the sample density and dark-field Fokker-Planck diffusion coefficients. We anticipate that the proposed algorithm may be of benefit in biomedical imaging and industrial settings.
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Pfeiffer F, Willer K, Viermetz M, Pfeiffer D. [Dark-field imaging and computed tomography : Novel X-ray-based contrast imaging modality with great promise for pulmonary imaging]. RADIOLOGIE (HEIDELBERG, GERMANY) 2023:10.1007/s00117-023-01161-4. [PMID: 37341743 DOI: 10.1007/s00117-023-01161-4] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Subscribe] [Scholar Register] [Accepted: 05/03/2023] [Indexed: 06/22/2023]
Abstract
INTRODUCTION The spatial and contrast resolution of conventional planar or computed tomographic X‑ray techniques is not sufficient to investigate microstructures of tissues. Dark-field imaging with X‑rays is an emerging technology that recently provided the first clinical results and makes diagnostic use of interactions of the beams with tissue due to their wave character. APPLICATION Dark-field imaging can provide information about the microscopic structure or porosity of the tissue under investigation that is otherwise inaccessible. This makes it a valuable complement to conventional X‑ray imaging, which can only account for attenuation. Our results demonstrate that X‑ray dark-field imaging provides pictorial information about the underlying microstructure of the lung in humans. Given the close relationship between alveolar structure and the functional state of the lung, this is of great importance for diagnosis and therapy monitoring and may contribute to a better understanding of lung diseases in the future. In the early detection of chronic obstructive pulmonary disease, which is usually associated with structural impairment of the lung, this novel technique could help to facilitate its diagnosis. PERSPECTIVE The application of dark-field imaging to computed tomography is still under development because it is technically difficult. Meanwhile, a prototype for experimental application has been developed and is currently being tested on a variety of materials. Use in humans is conceivable especially for tissues whose microstructure favors characteristic interactions due to the wave nature of the X‑rays.
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Affiliation(s)
- Franz Pfeiffer
- Chair of Biomedical Physics, Department of Physics, School of Natural Sciences, Technical University of Munich, 85748, Garching, Deutschland.
- Munich Institute of Biomedical Engineering, Technical University of Munich, 85748, Garching, Deutschland.
- Department of Diagnostic and Interventional Radiology, School of Medicine, Klinikum rechts der Isar, Technical University of Munich, 81675, München, Deutschland.
| | - Konstantin Willer
- Chair of Biomedical Physics, Department of Physics, School of Natural Sciences, Technical University of Munich, 85748, Garching, Deutschland
- Munich Institute of Biomedical Engineering, Technical University of Munich, 85748, Garching, Deutschland
| | - Manuel Viermetz
- Chair of Biomedical Physics, Department of Physics, School of Natural Sciences, Technical University of Munich, 85748, Garching, Deutschland
- Munich Institute of Biomedical Engineering, Technical University of Munich, 85748, Garching, Deutschland
| | - Daniela Pfeiffer
- Department of Diagnostic and Interventional Radiology, School of Medicine, Klinikum rechts der Isar, Technical University of Munich, 81675, München, Deutschland
- Institute for Advanced Study, Technical University of Munich, 85748, Garching, Deutschland
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