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Optimization of Flip Angle Design for Reduced T2 Blurring of 3D Arterial Spin Labeling
Li Zhao1 and David Alsop1

1Radiology, Beth Israel Deaconess Medical Center and Harvard Medical School, Boston, MA, United States

Synopsis

Conventional 3D arterial spin labeling images suffer from pronounced T2 blurring. In this work, new variable flip angle schemes, which can provide a Hann or Fermi window response across the slice direction, or which can be easily corrected to the designed window response and provide optimal SNR, were evaluated. Volunteers’ results show reduced blurring, improved SNR and contrast with the proposed methods.

Purpose

Arterial spin labeling acquisition using 3D spin echo train based sequences (e.g. stack-of-spiral [1] or GRASE [2]) is desirable because background suppression is more optimal, the post-labeling delay is constant across slices, and the signal-to-noise ration is high. These acquisitions suffer, however, from blurring due to the T2 decay during the echo train. Since the slice encoding is conventionally performed during the echo train, quite poor slice profiles can result leading to errors such as erroneously high flow white matter. Previous work has explored correcting T2 blurring by image post-processing [3], reduced echo train length with parallel imaging [4], and using a particular variable flip angle train design [5]. Since ASL is usually a SNR challenged acquisition, careful optimization of the acquisition SNR and point spread function is essential. In this work, the combination of variable flip angle trains and post processing filters were evaluated to determine optimal SNR for prespecified point-spread-function, such as Hann and Fermi. The performance of proposed methods was evaluated with ASL perfusion imaging on healthy volunteers.

Method

Since an algorithm for simultaneous global optimization of flip angle train and filter based correction was not available, optimization was divided into two sections. First, variable flip angle trains were designed to achieve signal amplitudes, including T2 decay, matched to a number of different window functions. The extended phase map algorithm [6] was used. Echo trains were iteratively calculated as the first echo amplitude was gradually increased from zero until the target shape of response could not be achieved. Standard constant asymptotic flip angle schemes were also implemented as a benchmark. The second stage of the optimization was selection of the echo train with optimal SNR for the desired window response. In general, the optimal echo train doesn’t need to be the one that exactly produces the window response. Instead, a different echo train in combination with a correction filter may achieve a better SNR.

Five volunteers were imaged by 3D pseudo continuous ASL on a 3T GE scanner. 32 slices with slice thickness 4mm covered the majority of the brain. Five interleaved spirals with 4.1ms readout provided 4.5x4.5mm in-plane resolution for a 24cm FOV. Other parameters were labeling duration 2s, post labeling delay 1.8s, 6 repetitions, TR 4.5s, TE 9.8ms and echo spacing 9.8ms.

ASL images were processed in MATLAB. To quantify the SNR of ASL more accurately, the noise was measured by the difference from the first and last three pairs of ASL images [7]. Image quality was measured by a non-reference blurring metric [8], where large value indicated more blurred image. The contrast between grey and white matters was measured with 3D mask generated by segmenting the T1 weighted images with a probability map in SPM12. Nonparametric Friedman's test was used to compare each method with the standard flip angle scheme without correction.

Result and Discussion

The flip angle designs and resulted echo signal are shown in Figure 1. Variable trains and filter corrections were able to achieve clear improvements in image resolution. Figure 2 shows results from one selected volunteer. With optimal flip angle and filter correction, the sharpness of ASL images was improved at the expense of SNR.

Quantitative results, Figure 3, show fairly equivalent performance for different optimization strategies: (1) The original standard constant asymptotic flip angle method resulted in the highest SNR (9.3±1.9), but also the most blurred images (33.2±1.5) and the lowest contrast (2.1±0.2). (2) When corrected to Hann window, the standard sequence resulted in significantly higher contrast (2.3±0.2 p<0.05). The optimized constant asymptotic flip angle for Hann windows provided the highest SNR as expected. The sequence designed for direct Hann response provided the least blurred images. (3) When corrected to Fermi window, the constant flip angle optimized for Fermi window provided the highest SNR, but generally the SNR of corrected image was lower than the original ones (the standard method with Fermi window correction 4.9±0.7 p<0.005 and direct Fermi response 4.4±0.9, p<0.01). When corrected to Fermi window, all methods showed reduced blurring (standard 27.3±1.3 p<0.001, optimal constant for Fermi 28.4±0.8 p<0.01 and direct Fermi 28.1±1.9 p<0.01) and standard method (2.4±0.2 p<0.05) and the constant flip angle optimal for Fermi (2.4±0.2 p<0.05) showed improved contrast.

Conclusion

Numerical optimization of multiple spin echo acquisitions suggests a combination of flip angle modulation and filter correction provides the best SNR for a desired window response. In-vivo results confirmed the resolution and contrast enhancement of the correction methods. Control of the point spread function in 3D ASL spin echo acquisitions can be achieved with a modest SNR penalty.

Acknowledgements

This work is partly supported by National Institute of Mental Health; Grant number: R01-MH080729.

References

[1] W. Dai, D. Garcia, C. de Bazelaire, and D. C. Alsop, “Continuous Flow-Driven Inversion for Arterial Spin Labeling Using Pulsed Radio Frequency and Gradient Fields,” Magn. Reson. Med., vol. 60, no. 6, pp. 1488–1497, Dec. 2008.

[2] D. J. Wang, J. R. Alger, J. X. Qiao, M. Gunther, W. B. Pope, J. L. Saver, N. Salamon, and D. S. Liebeskind, “Multi-Delay Multi-Parametric Arterial Spin-Labeled Perfusion MRI in Acute Ischemic Stroke – Comparison with Dynamic Susceptibility Contrast Enhanced Perfusion Imaging,” NeuroImage Clin., vol. 3, pp. 1–7, 2013.

[3] I. B. Galazzo, M. A. Chappell, D. L. Thomas, X. Golay, P. Manganotti, and E. De Vita, “Reducing blurring artifacts in 3D-GRASE ASL by integrating new acquisition and analysis strategies,” Proc. Intl. Soc. Mag. Reson. Med., vol. 22, p. 2704, 2014.

[4] M. Vidorreta, Y. V. Chang, M. A. Fernández-Seara, and J. A. Detre, “Single-Shot Whole-Brain Background-Suppressed pCASL MRI with 1D Accelerated 3D RARE Stack-Of-Spirals Readout,” Proc. Int. Soc. Magn. Reson. Med., vol. 23, p. 269, 2015.

[5] X. Liang, A. Connelly, J. D. Tournier, and F. Calamante, “A variable flip angle-based method for reducing blurring in 3D GRASE ASL,” Phys Med Biol, vol. 59, no. 18, pp. 5559–5573, 2014.

[6] M. Weigel, “Extended phase graphs: Dephasing, RF pulses, and echoes - Pure and simple,” J. Magn. Reson. Imaging, vol. 41, no. 2, pp. 266–295, 2015.

[7] O. Dietrich, J. G. Raya, S. B. Reeder, M. F. Reiser, and S. O. Schoenberg, “Measurement of signal-to-noise ratios in MR images: Influence of multichannel coils, parallel imaging, and reconstruction filters,” J. Magn. Reson. Imaging, vol. 26, no. 2, pp. 375–385, 2007.

[8] T. Dolmiere, P. Ladret, and M. Nicolas, “The Blur Effect?: Perception and Estimation with a New No-Reference Perceptual Blur Metric Fr ´ To cite this version?: The Blur Effect?: Perception and Estimation with a New No-Reference Perceptual Blur Metric,” vol. 6492, pp. 1–11, 2008.

Figures

Figure 1 variable flip angle and resulted response signal. Standard: the standard sequence with constant asymptotic flip angle. C-Hann/Fermi: the constant asymptotic flip angle sequence with optimal SNR for Hann/Fermi post correction. D-Hann/Fermi: the variable flip angle designed to provide Hann/Fermi window response directly without filter correction.

Figure 2 Reduced T2 blurring with variable flip angle and/or filter correction. (a) standard constant asymptotic flip angle scheme. (b) standard method filter corrected to Hann window. (c) standard method filter corrected to Fermi window. (d) optimal constant flip angle for Hann with post correction. (e) optimal constant flip angle for Fermi with post correction. (f) variable flip angle with Hann response. (g) variable flip angle with Fermi response.

Figure 3 Quantification of SNR, blurring and contrast in five volunteers. The labels of x-axis indicate the correction method. The error bars show the standard deviation across subjects. C-Hann/Fermi: the constant asymptotic flip angle sequence with optimal SNR for Hann/Fermi post correction. D-Hann/Fermi: the variable flip angle designed to provide Hann/Fermi window response directly without filter correction.

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