Cory R. Wyatt1 and Alexander R. Guimaraes2
1Oregon Health and Science University, Portland, OR, United States, 2Diagnostic Radiology, Oregon Health and Science University, Portland, OR, United States
Synopsis
3D magnetic resonance
fingerprinting (MRF) techniques have been developed to efficiently acquire 3D
volumes of quantitative parameters. Most techniques are based on applications
of 2D trajectories rotated or stacked in 3D k-space. By acquiring data across all of 3D k-space
each TR, we believe that efficient imaging and quantification can
be obtained. In this study, seiffert spirals are used to acquire 3D k-space in
an MRF acquisition of an isotropic 3D volume for the quantification
of T1 and T2 relaxation times. High resolution T1
and T2 maps of a human brain were acquired in less than 3
minutes.
Introduction
Previous work with MR
fingerprinting (MRF) has demonstrated the ability to acquire 3D quantitative
parameters, mainly with the use of 2D spirals rearranged in 3D k-space1-6. Recent work by Speidel et al.7 has demonstrated the use of Seiffert spirals
for efficient acquisition of 3D k-space. By utilizing these 3D trajectories, we
hypothesize that 3D MRF acquisitions can be designed for more time-efficient
acquisition compared to conventional techniques. In this study, we evaluate the
use of seiffert spirals for the acquisition of T1 and T2 relaxation times using MRF techniques.Methods
Seiffert spiral design: Similar to Speidel et al., a seiffert spiral
was calculated using equation 1, where sn and cn are Jacobi’s elliptical
functions and m determines the velocity of the spiral. For our implementation, a longer seiffert
spiral was generated and then separated into 8 individual spirals (m=0.15) with
a 4.51ms readout duration and isotropic resolution. All eight spirals are shown in Figure 1a and 1b. These
8 spirals were
acquired consecutively every 8 TRs, and then rotated around the origin by the
golden angle. For all acquisitions/simulations in this study, 12,000 TRs were
acquired for a total of 1,500 rotations. A sampling of every 100 rotated
spirals is shown in Figure 1c. To induce signal changes, flip angle variations
(shown in Figure 1d) are repeated every 800 TRs, for a total of 15 repetitions,
similar to the work of Gomez, et al.1. Before each
repetition, an adiabatic inversion pulse was applied to induce T1 recovery.
$$ρ = sn(s|m), z = cn(s|m), Φ = κs, κ=√m$$
Simulation Comparison: To determine sampling efficiency, the
diaphony8 of 40 interleaves was compared between the
proposed sequence and a 2D spiral with the same resolution, acquisition time, and
rotations as the seiffert spiral acquisition. Additionally, simulated brain
data was created using high resolution brain segmentations obtained from the
Brainweb project9. For each tissue (gray
matter, etc.), simulated signal curves were generated using Bloch equations and
then sampled in k-space by the two trajectories. The simulated k-space data for
both trajectories was then reconstructed using a subspace constrained FISTA reconstruction
in the Berkeley Advanced Reconstruction Toolbox10. A dictionary was
simulated using Bloch equations with 69 T1 values from
[100:50:3000,3200:200:5000] and 64 T2 values from [3:3:150,175:25:500] over 12,000
TRs. The reconstructed subspace images were then fit for T1 and T2
values using the dictionaries entries with the highest inner product and
compared to the true T1 and T2 brain images using
normalized root mean square error (NRMSE).
Phantom Validation: To demonstrate the feasibility of the proposed
technique, agarose phantoms of various concentrations were scanned with the
proposed test sequence. Sixteen phantoms (1/2/3/4% agarose with 2/6/12/20mg/kg
of ferumoytol) were scanned in a 20-channel head coil on a Siemens 3T Prisma
system. Conventional T1 images were acquired with a variable flip
angle VIBE sequence and conventional T2 images were acquired with a
multi-echo spin echo sequence. The proposed 3D MRF sequence acquired and
reconstructed as described previously. Mean values were obtained using the
center 3x3 section of each phantom and ICC values were calculated between the
3D MRF and conventional sequences.
In Vivo: Lastly, to demonstrate in vivo feasibility, a
healthy volunteer (28 year old male) was recruited under an OHSU IRB approved
protocol and scanned on a 3T Siemens Prisma scanner with a 20-channel head
coil. The proposed 3D MRF sequence was then acquired in the head of the
volunteer and T1/T2 relaxation maps were reconstructed. Results
The
diaphony of the two sampling schemes are shown in Figure 2, showing decreased diaphony
for the proposed seiffert sequence. Example images of the simulated data are
shown in Figure 3, in which the 2D trajectory had a NRMSE of 21.9 and 12.2 for
T1 and T2, respectively. For the seiffert spiral
trajectory, the NRMSE was 17.9 and 7.6 for T1 and T2,
demonstrating approximately 40% improvement in the error. For the phantom
validation, the ICC values between the 3D MRF and conventional sequences were
0.967 and 0.915 for T1 and T2 respectively. The acquired 3D relaxation maps are shown in a
few of the slices of the brain in Figure 4, demonstrating good image quality in
3 minutes using a TR=15ms.Discussion
As seen in the simulation
results, the error was substantially lower using the proposed seiffert trajectory
compared to the 2D spiral trajectory, suggesting more efficient coverage of
k-space. Similarly, the decreased diaphony suggests more evenly distributed 3D
k-space acquisition. The phantom experiment demonstrated good agreement between
conventional sequences and the proposed 3D MRF sequence. Lastly, the relaxation
maps obtained in vivo demonstrate good image quality, especially considering
the low scan time. The results in this study demonstrate the effectiveness of
the use of seiffert spirals for 3D MRF acquisition, allowing for high
resolution acquisition in a short period of time, with less error compared to
conventional techniques. Conclusion
This study
demonstrates the ability of seiffert spiral trajectories to efficiently quantify
T1 and T2 relaxation using MR fingerprinting techniques. Future
work will focus on comparing the seiffert and 2D spiral trajectories in vivo,
as well as comparing them to conventional relaxometry techniques. Acknowledgements
Grant Support: This project was supported in part by a
training fellowship from the Brenden-Colson Center for Pancreatic Care, NIDDK grant
R01DK117459, and a Medical Research Foundation New Investigator grant.References
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