研究目的
To investigate the use of k-t BLAST in monitoring tumor motion for radiotherapy and examine the trade-off between increased sparsification and potential loss of information.
研究成果
Sparse-sampling-based dynamic MRI with k-t BLAST can achieve high acquisition speeds (up to 20 Hz) with minimal information loss (RMS error <1 mm), making it suitable for radiotherapy guidance. It enables monitoring of respiratory variability over multiple cycles, complementing 4DCT by providing better temporal resolution and soft-tissue contrast. Future work should focus on 3D dynamic imaging and multimodality integration.
研究不足
The study is limited to 2D imaging in a single coronal plane, not capturing motion in other directions. MRI cannot measure electron density for dose calculation. Memory constraints of the MRI scanner limit the number of images acquired, and reconstruction time is significant. The deformable phantom may not fully mimic biological tissue properties.
1:Experimental Design and Method Selection:
The study used a 2D balanced fast field echo (bFFE) sequence with k-t BLAST for dynamic MRI to monitor tumor motion. The methodology involved comparing different k-t acceleration factors (1, 2, 5, 16) to assess spatial accuracy and information loss.
2:Sample Selection and Data Sources:
Lung tumor motion data from ten patients were used, replayed using an MRI-compatible motion phantom. Two human subjects (one with kidney tumor, one with lung tumor) were also studied.
3:List of Experimental Equipment and Materials:
MRI scanner (3T Philips Ingenia), MRI-compatible motion platform, Eppendorf test tubes filled with water as fiducial markers, torso RF receiver coil.
4:Experimental Procedures and Operational Workflow:
For phantom studies, motion was replicated and imaged in coronal slices with varying k-t factors. For human studies, dynamic MRI was performed during free breathing. Data were analyzed using affine and deformable image registration.
5:Data Analysis Methods:
Root mean square (RMS) error was used to compare measured trajectories with ground truth. Frequency spectra were analyzed using Fourier transform. Statistical analysis included mean and standard deviation calculations.
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