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Novel application of the reversed gradient method in Diffusion Weighted-MRI for tumor response assessment in head and neck squamous cell carcinoma patient undergoing radiation therapy.
David Aramburu Nuñez1,2,3, Jose Luis del Olmo Claudio3, Silvia Reigosa Montes3, Antonio López Medina3, Moises Mera Iglesias4, Francisco Salvador Gómez 3, Íñigo Nieto5, Alfonso Calzado2, Amita Shukla-Dave6, and Victor M Muñoz5

1Medical Physics, Memorial Sloan-Kettering Cancer Center, NEW YORK, NY, United States, 2Department of Radiology, Complutense University, MADRID, Spain, 3Department of Medical Physics and Radiological protection, Galaria - Hospital do Meixoeiro – Complexo Hospitalario Universitario de Vigo, VIGO, Spain, 4Medical Physics, Oncoserv, Santiago de los Caballeros – Dominican Republic, Dominican Republic, 5Department of Radiation Oncology, Galaria - Hospital do Meixoeiro – Complexo Hospitalario Universitario de Vigo, Spain, 6Departments of Medical Physics & Radiology, Memorial Sloan-Kettering Cancer Center, NY, United States

Synopsis

Reversed gradient method can reduce geometric distortion leading to accurate measurement of ADC. We designed a new phantom for distortion assessment and tested the reversed gradient method in both phantom and head and neck cancer patients, obtaining a relevant increase in mutual information values (phantom: 13% – 35%; patients: 6% - 100%). The voxel-wise analysis of the tumor showing variation of ADC with treatment exhibits significant difference (p<0.01) in calculated ADC between corrected and raw images. In future studies, the reverse gradient method may be included as part of clinical DW-MRI that focus on tumor response assessment.

Purpose

The most challenging issue in radiation therapy is the non-invasive, accurate assessment of tumor response during treatment. Apparent diffusion coefficient (ADC)1, derived from DW-MRI has shown promise in tumor characterization and assessment of treatment response2. However, geometric distortions associated with the DW-MRI data collected in clinical setting needs to be corrected prior to the calculation of ADC. One of the options for this correction is to use reversed gradient method3,4. This pilot study investigates the use of the reversed gradient correction method in DW-MRI for reduction in geometric distortion and accurate measurement of ADC in treatment response assessment.

Methods

MRI data acquisition: We developed a new phantom for distortion assessment (DA) in DW-MRI (Figure 1). It consists of a 17 x 17 x 17 cm³ polyethylene HD 500 cube, which contains 10 rows and 5 columns of cylindrical tubes (diameter: 14 mm) filled with water and capped at the ends. After phantom studies were performed at room temperature, three head and neck squamous cell carcinoma patients (stage IV) were enrolled for in vivo feasibility study and was approved by local institutional review board. The patients had 4 MRIs (1pre-, 2 intra- treatment [2nd and 3rd week] and 1 post- chemoradiation therapy). All MRI examinations were performed on a 1.5-T scanner (Achieva; Philips Healthcare) with a Philips Sense Flex Medium coil. Standard MR images for localization and T2w Turbo Spin Echo images were obtained followed by DW-MRI acquisition using a single-shot echo planar imaging (TE/TR (ms) = 77/5270; NEX=4, FOV (cm): 23, slice thickness (mm)= 6) with 3 b values of b=0, 600 and 1000 s/mm², respectively. For the reversed gradient correction method3,4, a 2nd DW-MRI acquisition was performed under exactly the same conditions, supposing that the spatial shifting of the signal occurred in the opposite direction along the y axis. MRI data analysis: Regions of interest (ROIs) were delineated in the cylindrical tubes filled with water in the phantom-DA, using ImageJ (http://imagej.nih.gov/ij/.). For the patient MRI studies, the radiation oncologist contoured the ROIs on the tumor using treatment planning vendor system (FocalSim). We used the 2 sets of DW-MRI images collected for each b values (b= 0, 600 and 1000 s/mm²) and analyzed the data with the open source SPM8 software (http://www.fil.ion.ucl.ac.uk/spm/software/spm8/) selecting the HySCO options to apply the reversed gradient method3,4. We used the standard settings for the method: dimension of phase encoding y (Antero-Posterior Direction), maximal data resolution full; smoothing of spline-interpolation 0.1, weight for "diffusion" regularizer 50; weight for "Jacobian" regularizer105. The corrected set of DW-MRI images were used to calculate ADC (mono-exponential fitting of the data) on a voxel-wise basis. ADC was also calculated from the 2 raw DW-MRI datasets. Geometric distortion correction was assessed using mutual information metrics6,7 via registration of the raw and corrected DW-MRI images with T2-weighted MR images using a in-home software ( ARTFIBio 0.6.2) 8.

Results

Phantom study: No significant difference was observed in ADC values of water derived from the raw ((2.13 ± 0.19) × 10-3 mm²/s) and corrected ((2.19 ± 0.05) × 10-3 mm² /s) DW-MRI data at room temperature. The mutual information metric values reflect their dependence on the b-value (13% for b=0, 23% for b=600 and 36% for b=1000s/mm2) [Table 1]. Patients study: The mutual information metric values for the pre- MRIs in three different patients for different b-values obtaining an average registration improvement of 21% [Table 2]. In one of the three patients tumor response was evaluated by measuring the difference in ADC values during treatment for raw and corrected datasets. The voxel-wise analysis of the tumor showing variation of ADC with treatment is closely clustered for corrected datasets rather than raw datasets and exhibits significant difference (p<0.01) in calculated ADC between corrected and raw images. (Figure 3).

Discussion

ADC has shown promise for mathematically modeling of the individual tumor response9. The DW-MRI data corrected by the reversed gradient method points out the feasibility of accurately measuring ADC through a voxel-wise approach for tumor response assessment. DW-MRI phantoms have been developed for verifying ADC value mostly of water10, 11, and do not focus on evaluating geometric distortion. Thus, our new phantom-DA provides the DW-MRI imaging community with a new tool to evaluate geometric distortions with mutual information metric.

Conclusion

The reverse gradient method may find wider applicability after validation in a larger cancer patient population for tumor response assessment which needs accurate measurement of ADC.

Acknowledgements

The National Health Institute of Spain is supporting this work by the ISCIII Grant PI11/02035 and DTS14/00188, and BIOCAPS project (FP7/REGPOT-2012-2013.1 under grant agreement n° 316265) that also partially supported this research.

References

1. Stejskal, E. O. and Tanner, J. E., "Spin diffusion measurements: spin echoes in the presence of a time dependent field gradient," J Chem Phys, p. 42:288–292, 1965. 2. Yankeelov, T. E., Lepage, M., Chakravarthy, A., Broome, E. E., Niermann, K. J., Kelley, M. C. Meszoely I, Mayer IA, Herman CR, McManus K, Price RR, and Gore, JC. "Integration of quantitative DCE-MRI and ADC mapping to monitor treatment response in human breast cancer: initial results," Magn Reson Imaging, vol. 25, pp. 1-13, 2007. 3. Chang H and Fitzpatrick M, "A technique for accurate magnetic resonance imaging in the presence of field inhomogeneities," IEEE Transactions on Medical Imaging, vol. 11, no. 3, pp. 319-329, 1992. 4. Morgan PS, Bowtell RW, McIntyre DJO, and Worthington BS, "Correction of spatial distortion in EPI due to inhomogeneous static magnetic fields using the reversed gradient method," J Magn Reson Imaging, vol. 19, pp. 499-507, 2004. 5. Ruthotto L, Kugel, H, Olesch J, Fischer B, Modersitzki J, Burguer M, and Wolters CH, "Diffeomorphic Susceptibility Artifact Correction of Diffusion-Weighted Magnetic Resonance Images," Phys Med Biol, vol. 57, pp. 5715-5731, 2012. 6. J. P. W. Pluim, J. Maintz, and M. Viergever, "Mutual-Information based registration of medical images: A survey," IEEE Transactions on, pp. 986-1004, 2003. 7. D. Mattes, D. R. Haynor, H. Vesselle, T. K. Lewellyn, and W. Eubank, "Non-Rigid Multimodality Image Registration," Proc. SPIE, Medical Imaging: Image Processing, vol. 4322, pp. 1609-1620, 2001. 8. Landesa-Vázquez, I.., Alba-Castro, J.L, Mera-Iglesias, M., Aramburu-Núñez, D., López-Medina, and A. Muñóz-Garzón, V., "ARTFIBio: A Cross-Platform Image Registration Tool for Tumor Response Quantification in Head and Neck Cancer," in 2nd IEEE Int. Conf. on Biomedical and Health Informatics, Valencia (Spain), 2014. 9. Atuegwu, N.C., Gore, J.C., and Yankeelov, T.E., "The integration of quantitative multi-modality imaging data into mathematical models of tumors," Phys Med Biol, vol. 55, pp. 2429-2449, 2010. 10. Lavdas, I., Behan, K. C., Papadaki, A., McRobbie, D. W., and Aboagye, E. O., "A phantom for diffusion-weighted MRI (DW-MRI)," Journal of Magnetic Resonance Imaging, vol. 38, no. 1, pp. 173-179, 2013. 11. Malyarenko, D., Galban, C.G., Londy, F.J., Meyer, C., Johnson, T.D., Rehemtulla, A., Ross, B., and Chenevert, T. L., "Multi-system repeatability and reproducibility of apparent diffusion coefficient measurement using an ice-water phantom," J Magn Reson Imaging, vol. 37(5), pp. 1238-1246, 2013.

Figures

Figure.1. a. Phantom-DA, specifically designed for distortion assessment in DW-MRI. b. CT Axial image of empty Phantom-DA, c. T2w MRI Axial image of Phantom-DA, Cylindrical hollows are filled with water.

Figure.2. The upper figure shows the DW-MRI with b=0 for the Phantom-DA: a. Phase encoding direction: Antero-Posterior, fat shift anterior (AP); b. Phase encoding direction: Antero-Posterior, fat shift posterior (PA); c. Corrected by the reversed gradient method. The lower figure shows the registration of CT and DW-MRI with b=0 for a patient: d. Phase encoding direction: Antero-Posterior, fat shift anterior (AP); e. Phase encoding direction: Antero-Posterior, fat shift posterior (PA); f. Corrected by the reversed gradient method.

Figure.3. ΔADC (10-3 mm2/s) vs Dose (Gy) in the tumor. Each point represents the voxel ΔADC values extracted from a. DW-MRI RAW, b. DW-MRI corrected at the 12th and 16th fractions of Treatment.

Table 1. Mutual Information values for the registration of T2w MRI and DW-MRI with different b-values of the phantom-DA. % difference is calculated with respect to averaged mutual information of raw studies, considering both gradients. Raw AP and raw PA correspond to the reversed gradients applied for phase encoding direction in the AP dimension and different fat shifts.

Table 2. - Mutual information values for different DW-MRI of the three patients with different b-values and T2w MRI. % difference is calculated with respect to averaged mutual information of raw studies, considering both gradients. Raw AP and raw PA correspond to reversed gradients applied for phase encoding direction in the AP dimension and different fat shifts.

Proc. Intl. Soc. Mag. Reson. Med. 25 (2017)
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