TH-D-ValA-05: Effect of Measured Cone-Beam CT-Density Calibration On Dose Calculations

2006 ◽  
Vol 33 (6Part23) ◽  
pp. 2286-2286 ◽  
Author(s):  
P Lindsay ◽  
X Zhu ◽  
L Zhang ◽  
R Wu ◽  
R Kudchadker ◽  
...  
Keyword(s):  
Cone Beam Ct ◽  
Cone Beam ◽  
Dose Calculations ◽  
Ct Density

scholarly journals Pseudo-CT generation from multiple MR images for small animal irradiation

2014 ◽  
Author(s):  
Shandra Gutierrez Diaz ◽  
Roel Van Holen ◽  
Benedicte Descamps ◽  
Christian Vanhove
Keyword(s):  
Soft Tissue ◽  
Cone Beam Ct ◽  
Small Animal ◽  
Cone Beam ◽  
Dose Calculations ◽  
Mr Images ◽  
Dice Coefficient ◽  
Membership Probability ◽  
Echo Time ◽  
Short Echo Time

Introduction. Computed tomography (CT) is the standard imaging modality for radiation therapy treatment planning (RTTP) because of its ability to provide information on electron density. However, magnetic resonance (MR) imaging provides superior soft tissue contrast, especially in small animal imaging, facilitating the precise selection of the target volume. This makes the technique interesting for irradiation of brain tumors. The aim of this study was to present an MR-only based workflow for RTTP on a small animal radiation research platform (SARRP) by investigating the potential of probabilistic classification of voxels using multiple MR sequences. Methods. Six female Fisher rats were anesthetized using isoflurane and individually fixed on an in-house made multimodality bed before starting MR and CT acquisitions. MR measurements were performed on a 7-Tesla system using a rat brain volume coil. Four different MR sequences were acquired for each animal, including a T1-weighted (MDEFT) sequence, a T2-weighted (RARE) sequence, an ultra-short echo time sequence with 20 μs echo time (UTE1) and an ultra- short echo time sequence with 2 ms echo time (UTE2). UTE offers the opportunity to acquire images from proton-poor structures with very short transverse relaxation times, such as bone, by using a rapid readout of the fast decaying signal. Following MR, the animals were moved to the SARRP to start a cone-beam CT (CB-CT) by acquiring 720 projections over 360°. Cone-beam CT projection data were reconstructed by filtered back-projection to obtain the standard-CT for RTTP. Then the images were bias field corrected and manually co-registered to the CB-CT. After that, images were segmented in three tissue classes (air, soft tissue and bone) with k-means for the CB-CT and fuzzy c-means segmentation algorithm (FCM) for the MR images with multiple MR images as input. The membership probability can be between 0 and 1, with one indicating 100% probability and zero indicating 0% probability to belong to a specific tissue class. To obtain a pseudo-CT image, voxels were assigned to the tissue class having the highest membership probability. The dice coefficient was used to evaluate the correctness of the segmentation for soft-tissue and bone. The pseudo-CT images with the highest similarity index were used for further radiotherapy treatment planning (RTTP), in addition, to the standard UTE1-UTE2. The target of the RTTP that was selected in the primary cortex (M1) and three different beam arrangements were investigated to compare CB-CT and MR-based dose calculations. The dose plans were a single static beam of 3x3 mm, using a single arc (3x3 mm beam size, 120° arc, couch at 0°), and three non-coplanar arcs (3x3 mm beam size, 120° arc, couch at 0°, 45° and 90°). Dose distributions were calculated using the TPS of the SARRP and cumulative dose volume histograms (DVHs) of the target and normal brain tissue were obtained for the three dose plans. Results The highest dice coefficient was obtained for the T1-UTE1-T2 combination, which was used for further RTTP. The contribution of bone to the total dice coefficient did not exceed 27%. However, bone accounts for only 2% of the image, therefore a misclassified bone pixel has a bigger effect in the dice coefficient than a misclassified soft tissue pixel. Using only 1 beam, both MR combinations underestimate the dose to be delivered to the target. When more complex beam configurations were used to irradiate the target, very small differences were observed between CB-CT and MR based dose calculations.

Accuracy of dose calculations on kV cone beam CT images of lung cancer patients

2016 ◽  
Vol 43 (11) ◽  
pp. 5934-5941 ◽  
Author(s):  
Mariska de Smet ◽  
Danny Schuring ◽  
Sebastiaan Nijsten ◽  
Frank Verhaegen
Keyword(s):  
Lung Cancer ◽  
Cancer Patients ◽  
Cone Beam Ct ◽  
Ct Images ◽  
Cone Beam ◽  
Dose Calculations ◽  
Lung Cancer Patients

Calibration of megavoltage cone-beam CT for radiotherapy dose calculations: Correction of cupping artifacts and conversion of CT numbers to electron density

2008 ◽  
Vol 35 (3) ◽  
pp. 849-865 ◽  
Author(s):  
Steven F. Petit ◽  
Wouter J. C. van Elmpt ◽  
Sebastiaan M. J. J. G. Nijsten ◽  
Philippe Lambin ◽  
André L. A. J. Dekker
Keyword(s):  
Electron Density ◽  
Cone Beam Ct ◽  
Cone Beam ◽  
Dose Calculations ◽  
Cupping Artifacts ◽  
Radiotherapy Dose ◽  
Megavoltage Cone Beam Ct

SU-E-T-416: VMAT Dose Calculations Using Cone Beam CT Images: A Preliminary Study

2014 ◽  
Vol 41 (6Part18) ◽  
pp. 321-321
Author(s):  
S Yu ◽  
V Sehgal ◽  
J kuo ◽  
P Daroui ◽  
N Ramsinghani ◽  
...  
Keyword(s):  
Cone Beam Ct ◽  
Ct Images ◽  
Cone Beam ◽  
Dose Calculations ◽  
Preliminary Study
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