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Fast Magnetization-Prepared Gradient Echo Sequences for 3D-T1rho Mapping of the Knee Joint Using Optimized Variable Flip-Angles
Marcelo V. W. Zibetti1, Hector L. De Moura1, Mahesh B. Keerthivasan2, and Ravinder R. Regatte1
1Radiology, NYU Grossman School of Medicine, New York, NY, United States, 2Siemens Medical Solutions, Malvern, PA, United States

Synopsis

Keywords: Pulse Sequence Design, Quantitative Imaging

We proposed an efficient magnetization-prepared gradient echo (MP-GRE) sequence that uses optimized variable flip-angles (OVFA) to reduce acquisition time by 4x while increasing SNR when compared to magnetization-prepared angle-modulated partitioned k-space spoiled GRE snapshots (MAPSS), typically used for T1rho mapping. The proposed OVFA based sequence can improve the spatial resolution of T1rho mapping by 4x, with nearly same SNR and scan time as MAPSS.

Introduction:

T1rho mapping can be accelerated by using undersampling or fast pulse sequences. In this work, we demonstrate the potential of magnetization-prepared gradient echo (MP-GRE) sequences (1–3) with optimized variable flip-angles (OVFA) for accelerated T1rho mapping. We compare the proposed modified sequence against one of the most used sequences for T1rho mapping, the magnetization-prepared angle-modulated partitioned k-space spoiled GRE snapshots (MAPSS) (1,4). The proposed new sequence based on OVFA can provide 4X more data per unit of time, and also achieve better SNR than MAPSS, allowing to acquire T1rho data faster and with higher spatial resolutions.

Methods:

MAPSS (4) and MP-GRE (5) sequences for T1rho mapping are shown in Figure 1(a) and 1(b) respectively, with their total time ($$$T_{tot}$$$). MAPSS used a Mz reset pulse at each shot, followed by Mz recovery time (Trec), T1rho preparation, and an imaging echo train that acquires several k-space lines. The number of lines collected, or views-per-segment (VPS), and its center-out ordering (6) are shown in Figure 1(c) and (d). Fully sampled or undersampled patterns may be used (6). MP-GRE does not use the Mz reset pulse, which allows for much smaller Trec. Because of it, MP-GRE requires some dummy segments (where no data is acquired) to reach a steady-state. MAPSS uses optimized flip-angles (FA) to reduce filtering effects (4). MP-GRE typically uses constant FA (CFA) (5). Here, we propose an optimization framework, that generalizes the optimization of MAPSS, considering not only reducing the filtering effects (7) but also improving SNR and T1rho accuracy.
The signal evolution (SE) model for MP-GRE sequences is given by (see (1) for SE of MAPSS):
$$M_{xy}(s,n)=A(n)M_{prep}(s)+B(n),$$
where $$$n$$$ represents the echo index and $$$s$$$ represents the shot position, and
$$A(n)=e_{\tau}\left[\prod_{i=1}^{n-1}e_1cos(\alpha_i)\right]e_2sin(\alpha_n)$$
and
$$B(n)=M_0\left\{(1-e_{\tau})\left[\prod_{i=1}^{n-1}e_1cos(\alpha_i)\right]+(1-e_{1})\left[1+\sum_{p=2}^{n-1}\left(\prod_{i=p}^{n-1}e_1cos(\alpha_i)\right)\right]\right\}e_2sin(\alpha_n)$$
where $$$e_{\tau}=e^{-\frac{\tau}{T_{1}}}$$$, $$$e_{1}=e^{-\frac{TR}{T_{1}}}$$$, $$$e_{2}=e^{-\frac{TE}{T2}}$$$, and
$$M_{prep}(s)=\left[M_z(s-1,VPS)e^{-\frac{T_{rec}}{T_{1}}}+M_0(1-e^{-\frac{T_{rec}}{T_{1}}})\right]e^{-\frac{TSL}{T_{1\rho}}}$$
where $$$1\leq n\leq VPS$$$, and:
$$M_{z}(s,n)=C(n)M_{prep}(s)+D(n),$$
With
$$C(n)=e_{\tau}\left[\prod_{i=1}^{n}e_1cos(\alpha_i)\right],$$ $$D(n)=M_0\left\{(1-e_{\tau})\left[\prod_{i=1}^{n}e_1cos(\alpha_i)\right]+(1-e_{1})\left[1+\sum_{p=2}^{n}\left(\prod_{i=p}^{n}e_1cos(\alpha_i)\right)\right]\right\}$$
being $$$M_{prep}(1)=M_0e^{-\frac{TSL}{T_{1\rho}}}$$$.
We optimize the FA using:
$${\bf \hat{\alpha}}=\arg\min_{\alpha}\left[\sum_{k=1}^K\omega_k\left(\lambda_A||{\bf Am}_k(\alpha)||_2^2+\lambda_F||{\bf Fm}_k(\alpha)||_2^2+\lambda_S||{\bf S}({\bf m}_k(\alpha)-{\bf m}_{ref}||_2^2 \right)\right]$$
where $$${\bf m}_k(\alpha)$$$ in the normalized SE, $$${\bf m}_k(\alpha)=[M_{xy}(k,t_1,1,1)/e^{-\frac{t_1}{T_{1\rho}(k)}}...M_{xy}(k,t_T,S+D,VPS)/e^{-\frac{t_T}{T_{1\rho}(k)}}]$$$, being $$$M_{xy}(k,t,s,n)$$$ the SE with relaxation set $$$1\leq k\leq K$$$, where $$$K$$$ is the number of relaxation sets, considering $$$T_{1}(k),T_{2}(k),T_{1\rho}(k)$$$, for $$$1\leq t\leq T$$$, where $$$T$$$ is the number of TSLs, on the segment $$$1\leq s\leq S+D$$$, after the flip-angle pulse $$$1\leq n\leq VPS$$$.
We used $$$\omega_k=|T_{1\rho}(k)|^2/\sum_{i=1}^{K}|T_{1\rho}(i)|^2$$$. The first term targets accuracy, with the matrix $$$\bf A$$$ computes the finite difference between all pairs of $$$M_{xy}(k,t_p,s,1)/e^{-\frac{t_T}{T_{1\rho}(k)}}$$$ and $$$M_{xy}(k,t_q,s,1)/e^{-\frac{t_T}{T_{1\rho}(k)}}$$$, being $$$t_p$$$ and $$$t_q$$$ two different TSLs. The second term reduces the filtering effects, where the matrix $$$\bf F$$$ computes the finite difference on the SE inside the segment, and it is repeated for all TSLs. The third term targets a better SNR, where $$${\bf m}_{ref}$$$ is the reference signal, and the matrix $$${\bf S}$$$ has ones in the positions we want to be close to $$${\bf m}_{ref}$$$, and zeros on the others. The non-linear least squared problem is minimized with the TRCG method (8).
The optimization is weighted primarily to improve $$$T_{1\rho}$$$ accuracy first, secondarily to improve SNR, and thirdly to reduce filtering effects in MP-GRE sequences in configurations that make it faster than MAPSS. Note we also apply this framework to MAPSS itself (denoted by MAPSS-OVFA), to improve SNR.

Results and Discussion:

We compare the results visually and with SNR and the mean of the normalized absolute deviation (MNAD) (see (9) for details on how to compute them). In Figure 2, we show the results with MAPSS and MAPSS-OVFA, to illustrate the improvement that OVFA can obtain in MAPSS. Because MAPSS-OVFA obtained the best quality it was chosen as the reference. In Figure 3, we compared the MAPSS-OVFA to our proposed sequence, named MP-GRE-OVFA, which is 4X faster than MAPSS. In Figure 4, we illustrate a comparison of MAPSS-OVFA with MP-GRE-OVFA with spatial resolution improved by 4X. In Table 1 we see the numerical results of the approaches compared to MAPSS-OVFA, including an evaluation with synthetic data, where ground truth is known.

Conclusion:

The proposed optimization framework was able to produce a modified MP-GRE sequence that can be 4X faster and achieve more SNR than MAPSS for T1rho mapping. With this sequence, we can improve the spatial resolution by 4X with a similar scan time and SNR as compared to MAPSS.

Acknowledgements

This study was supported by NIH grants, R21-AR075259-01A1, R01-AR068966, R01-AR076328-01A1, R01-AR076985-01A1, and R01-AR078308-01A1 and was performed under the rubric of the Center of Advanced Imaging Innovation and Research (CAI2R), an NIBIB Biomedical Technology Resource Center (NIH P41-EB017183).

References

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6. Zibetti MVW, Sharafi A, Keerthivasan MB, Regatte RR. Prospective Accelerated Cartesian 3D-T1rho Mapping of Knee Joint using Data-Driven Optimized Sampling Patterns and Compressed Sensing. In: Proceedings of the Annual Meeting of ISMRM 2021. ; 2021.

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Figures

Fig. 1: Illustration of the pulse sequences for (a) MAPSS and (b) MP-GRE. Including the expression for the time taken by each sequence. Note that MAPSS uses phase cycling, which doubles the acquisition time when the other parameters are the same. In (c) we observe that the 3D data collection is controlled by the sampling pattern (fully or undersampled) and in (d) the ordering is illustrated.

Fig. 2: Results comparing MAPSS with MAPSS-OVFA. Histograms of (a) a phantom and (b) a healthy volunteer are shown. The improvement in SNR was very significant and easily seen in phantom, (c) against (d), and humans, (e) against (f). Because of it, we decided to use MAPSS-OVFA as a reference to compute MNAD against other methods (MAPSS-OVFA was compared against a repetition of itself). Note that the peaks in the phantom histograms in (a) are sharper with MAPSS-OVFA, indicating better precision.

Fig.3: Results comparing the reference (MAPSS-OVFA) against MP-GRE-OVFA. Histograms of (a) a phantom and (b) a healthy volunteer are shown. Note that MP-GRE is a faster sequence, since it does not use phase cycling and can produce good SNR with short Trec because it does not use Mz reset. The MP-GRE-OVFA has improved accuracy (see histograms) compared to MP-GRE-CFA, very close to MAPSS-OVFA. The quality of MP-GRE-OVFA is very close to MAPSS-OVFA (note that MAPSS-OVFA is already better than MAPSS), but with a 4X shorter scan time.

Fig. 4: The combination of speed and good SNR makes the MP-GRE-OVFA an excellent sequence for high-resolution T1rho mapping. In this example, we illustrate the T1rho mapping with 4X better spatial in-plane resolution (2X horizontal and 2X vertical) in phantoms, (a) against (b), and human volunteers (c) against (d). The smaller voxel size of the HR sequence caused an expected reduction in SNR (SNR=4.7) in (d), but still close to what the standard MAPSS obtained in Fig 1(e) (SNR=5.5) with a voxel size 4X larger.

Table 1: Tested sequences, parameters, and results. Common parameters are 2 TSLs (1ms, 35ms), freq.=500Hz, and TR of 6ms (except MP-GRE-OVFA HR which uses TR of 8.6 ms), $$$\tau=TR/2$$$, FOV=200mmx200mmx128mm, volume of 256x256x64. For each sequence, it is specified views per segment (VPS), the number of acquired segments or shots (S), T1 recovery time (Trec), dummy shots (D), the time for each TSL (Time), which does not include phase cycling (PC) time, and the total time of the acquisition (Total time), which include all TSLs and phase cycling acquired.

Proc. Intl. Soc. Mag. Reson. Med. 31 (2023)
2377
DOI: https://doi.org/10.58530/2023/2377