1626

Anisotropic Diffusion Filter for Simultaneous Combination and Denoising of Multiple Acquisitions in DWI of the Spinal Cord
Sevgi Gokce Kafali1,2, Cagri Aydinkarahaliloglu1, Tolga Çukur1,2, and Emine Ulku Saritas1,2

1Electrical and Electronics Engineering, Bilkent University, Ankara, Turkey, 2National Magnetic Resonance Research Center (UMRAM), Ankara, Turkey

Synopsis

In diffusion weighted imaging (DWI), multiple acquisitions are acquired and averaged to attain a reasonable SNR level, especially for high spatial resolution or high b-value imaging. However, bulk or involuntary physiological motion during diffusion-sensitizing gradients alters the k-space, creating unpredictable global and/or local phases across multiple acquisitions. Therefore, direct complex averaging of these multiple acquisitions is prohibited. Here, we propose a reconstruction scheme based on modified anisotropic diffusion filtering, which starts with complex-valued acquisitions and corrects the phase issues while improving the SNR. The proposed reconstruction is demonstrated with in vivo DWI of the cervical spinal cord at 1.5T.

Introduction

In diffusion weighted imaging (DWI), multiple acquisitions have to be averaged to overcome low signal-to-noise ratio (SNR), especially in regions that require high-resolution imaging. However, motion during diffusion-sensitizing gradients generates k-space shifts and yields unpredictable global and/or local phases in multiple acquisitions, prohibiting direct complex averaging 1. Here, we propose a reconstruction scheme based on anisotropic diffusion filtering (ADF), which simultaneously combines and denoises multiple acquisitions, while correcting for phase issues.

Methods

Standard ADF: ADF is a popular denoising technique that smooths homogeneous regions while preserving edges, using the following formulation 2,3:$$I(x ̅,t+Δt)≃I(x ̅,t)+Δt.\frac{∂}{∂t}I(x ̅,t)\qquad(1)$$Here, $$$I(x ̅,t)$$$ is the image intensity at pixel location $$$x ̅$$$ at iteration $$$t$$$, and $$$Δt$$$ denotes the integration step. $$$\frac{∂}{∂t}I(x ̅,t)$$$ is updated iteratively as follows:$$\frac{∂}{∂t}I(x ̅,t)=div(c(x ̅,t).∇I(x ̅,t))\qquad(2)$$An edge detector function is typically chosen as$$c(x ̅,t)=\frac{1}{1+\left(\frac{|∇I(x ̅,t)|}{\kappa}\right)^{2}}\qquad(3)$$where $$$\kappa$$$ adjusts the noise tolerance. Larger values of $$$\kappa$$$ cause more effective denoising, at the expense of reduced edge preservation.

Proposed Reconstruction: As outlined in Fig. 1, each of the N acquisitions is first phase corrected by a refocusing reconstruction using the central 6% of k-space data 4. Acquisitions are then individually processed with projection onto convex sets (POCS) partial k-space reconstruction 5. Next, multiple acquisitions are processed with a new modified combination ADF (MC-ADF) method (Fig. 2). In contrast to ADF, MC-ADF benefits from structural information shared among acquisitions. To denoise a given acquisition, MC-ADF forms $$$\left(\begin{array}{c}N-1\\2\end{array}\right)$$$ distinct sets of three acquisitions that contain a given acquisition. Each set is stacked to form a 3D volume, and then processed with a complex-valued ADF. The denoised outputs in the middle layer are complex averaged across sets to compute the updated version of the given acquisition. These steps are also completed for all other acquisitions, and the entire procedure is iteratively repeated.

For MC-ADF, a conservative $$$Δt$$$ of $$$\frac{1}{2n}$$$ is chosen to increase the accuracy of the filter, where $$$n$$$ is the number of neighboring pixels (i.e., $$$n=3^3-1=26$$$ for 3D volumes) 6. $$$\kappa$$$ is calculated automatically at each iteration, using the 90th percentile value of $$$|∇I(x ̅,t)|$$$ throughout the image 7.$$$\kappa_t=0.5\kappa_0$$$ is used as the stopping criterion, where $$$\kappa_0$$$ is the initial $$$\kappa$$$. Once the stopping criterion is reached, filtered versions of the acquisitions are magnitude averaged.

In vivo DWI experiments: MRI experiments were performed on a 1.5T GE Scanner with an 8-channel cervico-thoracic-lumbar (CTL) coil. In vivo DWI images of the cervical spine were acquired on a healthy subject, in the sagittal plane. A reduced-FOV single-shot echo planar imaging sequence 8 was employed with a FOV of 18x4.5 cm2, 0.94x0.94 mm2 in-plane resolution, 192x48 matrix with 62.5% partial k-space acquisition, TE = 69 ms, 4 mm slice thickness, 16 image acquisitions (NEX), TR = 3.6 s, and b = 500 s/mm2 .9

Alternative Reconstructions: For all techniques, each acquisition was processed with a refocusing reconstruction followed by the POCS algorithm. Then, the following steps were performed:

1) COMP: Complex averaging of the multiple acquisitions

2) COMP-ADF: COMP followed by standard ADF

3) MAGN: Magnitude averaging of the multiple acquisitions

4) MAGN-ADF: MAGN followed by standard ADF All alternative reconstructions utilized the same number of iterations as the proposed reconstruction.

Results and Discussion

Figure 3a displays the results of proposed reconstruction across iterations. The stopping criterion is reached at the iteration, providing a denoised image with well-preserved edges. Figure 3b depicts the change in with iteration count.

Figure 4 compares all reconstruction techniques. COMP suffers from local phase cancellations along the spinal cord (yellow arrows), which can be confused with increased diffusion. COMP-ADF improves image SNR, but is not able to alleviate phase cancellations. While MAGN is inherently devoid of phase cancellations, it suffers from noise accumulation in the background. MAGN-ADF slightly denoises the image, but noise accumulation persists. In contrast, the proposed reconstruction successfully denoises the image while preserving the edges. Furthermore, the final image is not affected by phase cancellations. Table 1 lists measurements of a no-reference image quality metric for all reconstruction methods 10. Larger values of this anisotropy metric, $$$\sigma_{anisotropy}$$$ indicate higher image quality. The proposed MC-ADF results in the highest $$$\sigma_{anisotropy}$$$ among all techniques, suggesting superior image quality.

Conclusion

We proposed an iterative image reconstruction algorithm for DWI based on anisotropic diffusion filtering, to simultaneously suppress noise and combine multiple acquisitions. In vivo spinal cord DWI results demonstrate that the proposed reconstruction significantly enhances image quality while overcoming local phase cancellations.

Acknowledgements

SG Kafali and AC Aydinkarahaliloglu contributed equally to this work. This work was supported by the European Commission through FP7 Marie Curie Career Integration Grant (PCIG13GA618834, PCIG13GA618101), by a European Molecular Biology Organization Installation Grant (IG 3028), by the Turkish Academy of Sciences through TUBA-GEBIP 2015 program, and by the BAGEP Award of the Science Academy.

References

1. Anderson AW, Gore JC. Analysis and correction of motion artifacts in diffusion weighted imaging. Magnetic Resonance in Medicine. 1994;32:379–387.

2. Perona P, Malik J. Scale-space and edge detection using anisotropic diffusion. IEEE Transactions on Pattern Analysis and Machine Intelligence. 1990;12(7):629–639.

3. Gerig G, Kubler O, Kikinis R, Jolesz F a. Nonlinear anisotrophic filtering of MRI data. IEEE Transactions on Medical Imaging. 1992;11(2):221–232.

4. Miller KL, Pauly JM. Nonlinear phase correction for navigated diffusion imaging. Magnetic Resonance in Medicine. 2003;50(2):343–353.

5. Haacke EM, Lindskogj ED, Lin W. A fast, iterative, partial-fourier technique capable of local phase recovery. Journal of Magnetic Resonance. 1991;92(1):126–145.

6. Weickert J, Romeny B, Viergever M. Efficient and reliable scheme for nonlinear diffusion filtering. IEEE Transactions on Image Processing. 1998;7(3):398–410.

7. Canny J. A computational approach to edge detection. IEEE transactions on pattern analysis and machine intelligence. 1986;8(6):679–698.

8. Saritas EU, Cunningham CH, Lee JH, Han ET, Nishimura DG. DWI of the spinal cord with reduced FOV single-shot EPI. Magnetic Resonance in Medicine. 2008;60(2):468–473.

9. Saritas EU, Lee JH, Nishimura DG. SNR dependence of optimal parameters for apparent diffusion coefficient measurements. Medical Imaging, IEEE Transactions on. 2011;30(2):424–437.

10. Gabarda S, Cristóbal G. Blind image quality assessment through anisotropy. Journal of the Optical Society of America. A, Optics, image science, and vision. 2007;24(12):B42–B51.

Figures

Figure 1. Multiple acquisitions are first phase corrected with a refocusing reconstruction, utilizing the central 6% portion of the k-space. The resulting data are processed by the POCS algorithm for partial k-space reconstruction. MC-ADF filter denoises each acquisition iteratively while leveraging the structural information shared among multiple acquisitions. $$$\left(\begin{array}{c}N-1\\ 2\end{array}\right)$$$ sets of three acquisitions that contain a given acquisition are filtered, and the filtered versions are then complex averaged at the end of each iteration. Once iterations are complete, the resulting acquisitions are magnitude averaged.

Figure 2. The schematic of MC-ADF for one iteration. Three-combinations of acquisitions are formed, by keeping the middle layer as the specific acquisition to denoise, and stacking $$$\left(\begin{array}{c}N-1\\ 2\end{array}\right)$$$ possibly different acquisitions to the top and bottom. Each of these 3D volumes is processed by a complex-valued ADF. The resulting “denoised” versions of middle layers are then complex averaged. As a result, each acquisition is filtered and averaged, yielding denoised images at the end of an iteration.

Figure 3. a) The results of the proposed MC-ADF at selected iterations for in vivo DWI of the cervical spine. The proposed stopping criterion occurs at the iteration for this subject. Earlier iterations are not able to suppress the noise, whereas later iterations cause over-smoothing of the edges. b) Normalized $$$\kappa$$$ values versus iteration count. Normalization was performed with respect to $$$\kappa_0$$$. The stopping criterion of $$$\kappa_t=0.5\kappa_0$$$ was reached at the 8th iteration, marked with the red rhombus.

Figure 4. The results of the cervical spinal cord for the alternative and the proposed reconstructions. COMP suffers from local phase cancellations (yellow arrows). COMP-ADF is not able to alleviate these cancellations. Although MAGN and MAGN-ADF do not suffer from local phase cancellations, noise accumulation in the background results in a faded appearance. In contrast, the proposed MC-ADF reconstruction provides visibly increased SNR without any local phase cancellations.

Table 1. No-reference image quality assessment for alternative reconstructions and the proposed MC-ADF. Higher $$$\sigma_{anisotropy}$$$ with MC-ADF indicates superior image quality.

Proc. Intl. Soc. Mag. Reson. Med. 26 (2018)
1626