Ulrich Katscher1, Bjoern Steinhorst1, Jakob Meineke1, and Jochen Keupp1
1Philips Research, Hamburg, Germany
Synopsis
Double-echo steady-state (DESS) sequences are a promising candidate for diffusion weighted imaging (DWI) free of geometric distortions. The design of diffusion-weighted DESS (dwDESS) sequences allows waveform variations for the diffusion weighting gradient GD. While dwDESS sequences were originally introduced with unipolar GD, also bipolar or higher order GD are possible. A balanced GD (i.e., with nulling zeroth momentum) typically necessitates a spoiler gradient to suppress banding artefacts, which additionally increases the degrees of freedom in the design of dwDESS sequences. This study explores different dwDESS sequence variants according to predefined optimization criteria.
Introduction
Double-echo steady-state (DESS) sequences are a promising candidate for diffusion weighted imaging (DWI) free of geometric distortions1. The design of diffusion-weighted DESS (dwDESS) sequences allows waveform variations for the diffusion weighting gradient GD. While dwDESS sequences were originally introduced with unipolar GD2, also bipolar or higher order GD are possible3. A balanced GD (i.e., with nulling zeroth momentum) typically necessitates a spoiler gradient GS to suppress banding artefacts4, which additionally increases the degrees of freedom in the design of dwDESS sequences.
This study explores different dwDESS sequence variants, with the following optimization criteria:
(a) the functional form of signal versus strength of GD reflecting the ability to fit the Apparent Diffusion Coefficient (ADC) from the signal,
(b) the sensitivity of signal versus strength of GD reflecting the reliability of the fitted ADC,
(c) the obtained signal strength reflecting the expected SNR of diffusion weighted images and fitted ADC map.Methods
Different variants of dwDESS sequences were investigated in the framework of Extended Phase Graphs (EPG)5. All signals given below were calculated after applying 50 RF pulses to guarantee that steady state was reached in the sequence. The signals S- and S+ of the echoes directly before and after an RF pulse as well as their ratio ΔS = S-/S+ (corresponding to the diffusion weighted signal) were calculated.
Ten different sequence variants were investigated (Fig.1). Sequence 0 is the unipolar variant2. In Sequences 1-5, GD comprised n=1 to n=5 bipolar gradient pairs, each consisting of a negative and positive lobe of identical size. While Sequence 0 did not need an explicit GS, GS was added between the end of GD and S- for Sequences 1-54,6. Sequence 6 differed from Sequence 2 (n=2) by inverting the polarization of the second gradient pair. Sequences 7/8 differed from Sequence 1 by shifting GS before S+ / after S-. Sequence 9 differed from Sequence 6 by shifting GS to TR/2 and the two bipolar GD before S+ and after S-. All sequences shared the same TR=76 ms, same total length τD=74.1 ms of GD, and same length τS=1.9 ms of GS. (i.e., τS/τD=2.5%).
Each sequence simulation was repeated 7 times with p=40/50/…/90/100% of maximum gradient strength gmax=13 mT/m of GD, yielding current gradient strength g=pgmax. The definition of an effective b-value (and thus, the determination of ADC) was possible if ΔS(g²) showed a mono-exponential shape (see above criterium (a))7. To investigate the sensitivity of ΔS versus g² (see criterium (b)), a “Comparative Diffusion Coefficient” (CDC) was defined via DS(g²) ~ exp(-CDC g²). The higher the obtained CDC, the higher the sensitivity of ΔS versus g², and thus the expected reliability of the ADC map. Sequence variants yielding no impact of g on ΔS (i.e. CDC=0) were excluded from this study beforehand.
Diffusivities D=1mm²/s and D=2mm²/s were applied throughout the study. Corresponding tests confirmed that T1 and T2 (within physiologic range) did not impact ΔS (as required for determination of ADC) but did impact S±. To enable comparison of S± from different sequence variants, T1=350ms, T2=250ms, and α=25° was assumed for all simulations in order to investigate criterium (c) defined above.Results
The desired mono-exponential behavior of ΔS(g²) was found for all investigated sequences except for Sequence 0, which was thus not further examined. For Sequences 1-5, a double logarithmic plot (Fig.2) of CDC versus n showed a functional behavior with CDC~n-1.75, independent of D assumed in the simulation. CDC versus S± is shown for all sequences in Fig.3. Highest S± was found for Sequences 7/8, and highest CDC was found for Sequence 1.Discussion
The following ranking of the investigated dwDESS sequence variants was obtained:
- Criterium (a) (mono-exponential behavior) is fulfilled by all sequence variants except Sequence 0 (unipolar GD),
- Criterium (b) (reliability of fitting ADC, reflected by maximum CDC) is optimally fulfilled for Sequence 1 (bipolar GD, GS inside echoes),
- Criterium (c) (SNR of diffusion weighted images and ADC map, reflected by maximum S±) is optimally fulfilled for Sequences 7 and 8 (bipolar GD, GS outside echoes).
Thus, there is no dedicated, single sequence which optimally fulfills all criteria. Sequences with different n (Sequences 1-5) show a systematic trade-off between criteria (b) and (c). However, comparing Sequence 1 with Sequence 5, the gain in signal strength of S- is less than a factor of 3, while the loss in CDC is almost a factor of 20. More promising are Sequences 7/8, where the gain in signal strength of S- is around a factor of 6 compared with Sequence 1, while the loss in CDC is only a factor of 2-3.Conclusion
According to this simulation study, it is expected that the design of GD and GS in dwDESS has a significant impact on the quality of the resulting diffusion weighted images and ADC map. The optimal design of GD and GS depends on the specific requirements of the targeted application.Acknowledgements
No acknowledgement found.References
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