TY - JOUR
T1 - Principles and applications of multienergy CT
T2 - Report of AAPM Task Group 291
AU - McCollough, Cynthia H.
AU - Boedeker, Kirsten
AU - Cody, Dianna
AU - Duan, Xinhui
AU - Flohr, Thomas
AU - Halliburton, Sandra S.
AU - Hsieh, Jiang
AU - Layman, Rick R.
AU - Pelc, Norbert J.
N1 - Funding Information:
Cynthia McCollough is the recipient of a research grant from Siemens Healthcare. Dianna Cody is an ACR CT Accreditation Program Reviewer and has a research agreement with Gammex, Inc. Xinhui Duan receives research funding from Cancer Prevention Research Institute of Texas. Jiang Hsieh is an employee of GE Healthcare Technologies. Sandra Hallburton is an employee of Philips Healthcare. Thomas Flohr is an employee of Siemens Healthcare. Kirsten Boedeker is an employee of Canon Medical Systems. The authors thank Ms. Kristina Nunez of the Mayo Clinic for expert assistance in the preparation and submission of this manuscript and Dr. Shuai Leng, also of the Mayo Clinic, for many insightful discussions.
Funding Information:
Cynthia McCollough is the recipient of a research grant from Siemens Healthcare. Dianna Cody is an ACR CT Accreditation Program Reviewer and has a research agreement with Gammex, Inc. Xinhui Duan receives research funding from Cancer Prevention Research Institute of Texas. Jiang Hsieh is an employee of GE Healthcare Technologies. Sandra Hallburton is an employee of Philips Healthcare. Thomas Flohr is an employee of Siemens Healthcare. Kirsten Boedeker is an employee of Canon Medical Systems.
Publisher Copyright:
© 2020 American Association of Physicists in Medicine
PY - 2020/7/1
Y1 - 2020/7/1
N2 - In x-ray computed tomography (CT), materials with different elemental compositions can have identical CT number values, depending on the mass density of each material and the energy of the detected x-ray beam. Differentiating and classifying different tissue types and contrast agents can thus be extremely challenging. In multienergy CT, one or more additional attenuation measurements are obtained at a second, third or more energy. This allows the differentiation of at least two materials. Commercial dual-energy CT systems (only two energy measurements) are now available either using sequential acquisitions of low- and high-tube potential scans, fast tube-potential switching, beam filtration combined with spiral scanning, dual-source, or dual-layer detector approaches. The use of energy-resolving, photon-counting detectors is now being evaluated on research systems. Irrespective of the technological approach to data acquisition, all commercial multienergy CT systems circa 2020 provide dual-energy data. Material decomposition algorithms are then used to identify specific materials according to their effective atomic number and/or to quantitate mass density. These algorithms are applied to either projection or image data. Since 2006, a number of clinical applications have been developed for commercial release, including those that automatically (a) remove the calcium signal from bony anatomy and/or calcified plaque; (b) create iodine concentration maps from contrast-enhanced CT data and/or quantify absolute iodine concentration; (c) create virtual non-contrast-enhanced images from contrast-enhanced scans; (d) identify perfused blood volume in lung parenchyma or the myocardium; and (e) characterize materials according to their elemental compositions, which can allow in vivo differentiation between uric acid and non-uric acid urinary stones or uric acid (gout) or non-uric acid (calcium pyrophosphate) deposits in articulating joints and surrounding tissues. In this report, the underlying physical principles of multienergy CT are reviewed and each of the current technical approaches are described. In addition, current and evolving clinical applications are introduced. Finally, the impact of multienergy CT technology on patient radiation dose is summarized.
AB - In x-ray computed tomography (CT), materials with different elemental compositions can have identical CT number values, depending on the mass density of each material and the energy of the detected x-ray beam. Differentiating and classifying different tissue types and contrast agents can thus be extremely challenging. In multienergy CT, one or more additional attenuation measurements are obtained at a second, third or more energy. This allows the differentiation of at least two materials. Commercial dual-energy CT systems (only two energy measurements) are now available either using sequential acquisitions of low- and high-tube potential scans, fast tube-potential switching, beam filtration combined with spiral scanning, dual-source, or dual-layer detector approaches. The use of energy-resolving, photon-counting detectors is now being evaluated on research systems. Irrespective of the technological approach to data acquisition, all commercial multienergy CT systems circa 2020 provide dual-energy data. Material decomposition algorithms are then used to identify specific materials according to their effective atomic number and/or to quantitate mass density. These algorithms are applied to either projection or image data. Since 2006, a number of clinical applications have been developed for commercial release, including those that automatically (a) remove the calcium signal from bony anatomy and/or calcified plaque; (b) create iodine concentration maps from contrast-enhanced CT data and/or quantify absolute iodine concentration; (c) create virtual non-contrast-enhanced images from contrast-enhanced scans; (d) identify perfused blood volume in lung parenchyma or the myocardium; and (e) characterize materials according to their elemental compositions, which can allow in vivo differentiation between uric acid and non-uric acid urinary stones or uric acid (gout) or non-uric acid (calcium pyrophosphate) deposits in articulating joints and surrounding tissues. In this report, the underlying physical principles of multienergy CT are reviewed and each of the current technical approaches are described. In addition, current and evolving clinical applications are introduced. Finally, the impact of multienergy CT technology on patient radiation dose is summarized.
KW - dual-energy CT
KW - material decomposition
KW - material selective
KW - multienergy CT
KW - virtual monoenergetic
KW - virtual noncontrast
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U2 - 10.1002/mp.14157
DO - 10.1002/mp.14157
M3 - Comment/debate
C2 - 32215937
AN - SCOPUS:85085487595
SN - 0094-2405
VL - 47
SP - e881-e912
JO - Medical Physics
JF - Medical Physics
IS - 7
ER -