WE-D-332-02: X-Ray Spectra Optimization for Dual-Energy Imaging Using Dual-Source CT

2008 ◽  
Vol 35 (6Part24) ◽  
pp. 2948-2948
Author(s):  
J Ramirez Giraldo ◽  
A Primak ◽  
X Liu ◽  
C McCollough
2015 ◽  
Vol 2015 ◽  
pp. 1-8 ◽  
Author(s):  
Kuo Men ◽  
Jian-Rong Dai ◽  
Ming-Hui Li ◽  
Xin-Yuan Chen ◽  
Ke Zhang ◽  
...  

Purpose. To develop a dual energy imaging method to improve the accuracy of electron density measurement with a cone-beam CT (CBCT) device.Materials and Methods. The imaging system is the XVI CBCT system on Elekta Synergy linac. Projection data were acquired with the high and low energy X-ray, respectively, to set up a basis material decomposition model. Virtual phantom simulation and phantoms experiments were carried out for quantitative evaluation of the method. Phantoms were also scanned twice with the high and low energy X-ray, respectively. The data were decomposed into projections of the two basis material coefficients according to the model set up earlier. The two sets of decomposed projections were used to reconstruct CBCT images of the basis material coefficients. Then, the images of electron densities were calculated with these CBCT images.Results. The difference between the calculated and theoretical values was within 2% and the correlation coefficient of them was about 1.0. The dual energy imaging method obtained more accurate electron density values and reduced the beam hardening artifacts obviously.Conclusion. A novel dual energy CBCT imaging method to calculate the electron densities was developed. It can acquire more accurate values and provide a platform potentially for dose calculation.


Radiology ◽  
2009 ◽  
Vol 252 (1) ◽  
pp. 61-70 ◽  
Author(s):  
Long-Jiang Zhang ◽  
Yan-E Zhao ◽  
Sheng-Yong Wu ◽  
Benjamin M. Yeh ◽  
Chang-Sheng Zhou ◽  
...  

Circulation ◽  
2007 ◽  
Vol 116 (suppl_16) ◽  
Author(s):  
Carlos A Van Mieghem ◽  
Annick C Weustink ◽  
Marcel Kofflard ◽  
A. Schreve-Steensma ◽  
Niels A Matheijssen ◽  
...  

Introduction and aim: Dual Source CT (DSCT) scanners, with an increased temporal resolution (83 ms), are becoming widely available. To evaluate the current potential of this scanner in the clinical arena, we performed a head-to-head comparison with conventional coronary angiography (CCA) taking into account the following parameters: radiation exposure, procedure time and contrast load. Methods: During a one-year period (april 2006 to march 2007) we compared a consecutive patient group who underwent DSCT (318 patients, 222 male, mean age 68±11 years) and CCA (352 patients, 258 male, mean age 61±12) respectively. Patients with previous bypass surgery were excluded. In DSCT, the volume of iodinated contrast material was adapted to the scan time. A contrast bolus was injected in an antecubital vein at a flow rate of 5.0 ml/s followed by a saline chaser of 40 ml at 5.0 ml/s. Each tube provided 412 mAs/rot (maximum), and full X-ray tube current was given during 25–70% of the RR-interval. Exposure data were collected using the x-ray dosimetrical reports from DSCT and CCA. Results: The mean procedure time using DSCT and CCA was 16.1±4.7 min and 44.1±25.5 min (p<0.001), respectively. The mean contrast load in DSCT and CCA was 77.9±7.6 ml and 175.3±4.3ml (p<0.001), respectively. The overall radiation exposure for DSCT and CCA was calculated as 15.3±4.0 mSv and 5.7±4.3 mSv, respectively. Radiation exposure with DSCT was significantly lower (p<0.001) in patients with a heart rate of >70 bpm (12.9±3.1 mSv ) as compared with patients with heart rates <70 bpm (16.4±3.8 mSv). Conclusion: In today’s practice currently available DSCT scanners perform favorably as compared with CCA, considering procedure time and patient contrast load. Radiation exposure with DSCT remains higher but should not be considered a major disadvantage taking into account the relatively old age group that generally undergoes coronary angiography and the major benefit of not being exposed to the risks of an invasive procedure.


Circulation ◽  
2007 ◽  
Vol 116 (suppl_16) ◽  
Author(s):  
Sei Komatsu ◽  
Alexander Kuhlmann ◽  
Valentine Campean ◽  
Dieter Ropers ◽  
Ulrike Ropers ◽  
...  

Background In addition to high spatial (0.4 mm) and temporal resolution (83 ms), Dual Source CT (DSCT) allows simultaneous imaging with two different x-ray energies. This may be beneficial for tissue characterization. Objectives. To determine the accuracy of ex vivo atherosclerotic plaque characterization with DSCT and to assess the CT attenuation of various plaque components depending on X-ray energy. Materials and Methods. 18 atherosclerotic vessels of coronary, carotid and iliac arteries obatined from autopsy were analyzed by DSCT. Each lumen of the vessels was filled with contrast media (30X Imeron 350). The collimation was 2X64X0.6 mm, rotation time was 330 msec., temporal resolution was 83 msec. Data sets were obtained using a tube voltage of 80, 100, 120, and 140 kV. The x.-ray attenuation of lipid-rich plaque, fibrous plaque, calcified plaque and contrast-enhanced lumen were determined for all x-ray energies by comparison to histology at 25 sites. In addition, cross-sectional images were reconstructed with 0.75 mm slice thickness and 0.4 mm increment. 26 slices at 10 mm interval were analyzed by comprehensive color-coding according to CT number. Results. There were significant differences among CT attenuations of lipid-rich, fibrous and calcified plaque using 80, 100, 120, and 140 kV (Table , p<0.01), respectively. The averaged ratio of CT attenuation of lipid-rich, fibrous plaque, and calcified plaque to the Contrast-enhanced lumen for 80kV and 140kV were −16%, 11%, 14%, respectively (p<0.05). Lipid-rich plaque was well-differentiated with lumen attenuation in all energies. Conclusions. The relationships between lumen enhancement and each plaque component were different as changing the x-ray energy level. Using of varying x-ray energy, DSCT may able to detect atherosclerotic plaque and characterization of plaque components. The Attenuation on Different Energy


2009 ◽  
Vol 36 (6Part24) ◽  
pp. 2749-2750
Author(s):  
B Schmidt

Sign in / Sign up

Export Citation Format

Share Document