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Accuracy of spectral curves at different phantom sizes and iodine concentrations using dual-source dual-energy computed tomography.
Sato, Kazuhiro; Kageyama, Ryota; Sawatani, Yuta; Takano, Hirokazu; Kayano, Shingo; Takane, Yumi; Saito, Haruo.
Affiliation
  • Sato K; Health Sciences, Tohoku University Graduate School of Medicine, 2-1 Seiryo-machi, Aoba-ku, Sendai, Miyagi, 980-8575, Japan. satok@med.tohoku.ac.jp.
  • Kageyama R; Health Sciences, Tohoku University Graduate School of Medicine, 2-1 Seiryo-machi, Aoba-ku, Sendai, Miyagi, 980-8575, Japan.
  • Sawatani Y; Department of Radiology, Sendai City Hospital, 1-1-1 Asuto-Nagamachi, Taihaku-ku, Sendai, Miyagi, 982-8502, Japan.
  • Takano H; Department of Radiology, Tohoku University Hospital, 1-1 Seiryo-machi, Aoba-ku, Sendai, Miyagi, 980-8574, Japan.
  • Kayano S; Department of Radiology, Tohoku University Hospital, 1-1 Seiryo-machi, Aoba-ku, Sendai, Miyagi, 980-8574, Japan.
  • Takane Y; Department of Radiology, Tohoku University Hospital, 1-1 Seiryo-machi, Aoba-ku, Sendai, Miyagi, 980-8574, Japan.
  • Saito H; Health Sciences, Tohoku University Graduate School of Medicine, 2-1 Seiryo-machi, Aoba-ku, Sendai, Miyagi, 980-8575, Japan.
Phys Eng Sci Med ; 44(1): 103-116, 2021 Mar.
Article de En | MEDLINE | ID: mdl-33528785
To validate the accuracy of spectral curves obtained by an image-data-based algorithm and clarify the error factors that reduce accuracy. Iodine rods of known composition and different concentrations were inserted into a cylinder or elliptic-cylinder phantom and scanned according to the dual-energy protocol. Spectral curves were obtained by (i) theoretical calculation, (ii) image-data-based 2-material decomposition, and (iii) using a dedicated workstation. Accuracy was verified by comparing the spectral curve obtained by theoretical calculations with those obtained by the image-data-based algorithms or the dedicated workstations. For a quantitative evaluation, the error and relative error (RE) were calculated. In the image-data-based calculation, the errors with respect to the theoretical CT number ranged from - 8.3 to 71.1 HU. For all 192 combinations, 80.7% of the errors were under ± 15 HU, and 97.9% of the REs were under 10%. In the dedicated workstation, the errors ranged from - 94.7 to 26.8 HU. For all combinations, 68.8% of the errors were under ± 15 HU, and 68.2% of the REs were under 10%. By appropriately setting the effective energy corresponding to the CT number of the basis materials, an accurate spectral curve can be obtained. The beam-hardening effect is canceled by the 2-material decomposition process even without beam-hardening correction. Accuracy is primarily reduced by scattered radiation rather than the beam-hardening effect.
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Texte intégral: 1 Collection: 01-internacional Base de données: MEDLINE Sujet principal: Iode Langue: En Journal: Phys Eng Sci Med Année: 2021 Type de document: Article Pays d'affiliation: Japon Pays de publication: Suisse

Texte intégral: 1 Collection: 01-internacional Base de données: MEDLINE Sujet principal: Iode Langue: En Journal: Phys Eng Sci Med Année: 2021 Type de document: Article Pays d'affiliation: Japon Pays de publication: Suisse