Jae-Kyun Ryu1,2 and Jang-Yeon Park2,3,4
1Biomedical Institute for Convergence at SKKU, Sungkyunkwan University, Suwon, Korea, Republic of, 2Center for Neuroscience Imaging Research, Institute for Basic Science, Suwon, Korea, Republic of, 3Department of Biomedical Engineering, Sungkyunkwan University, Suwon, Korea, Republic of, 4Department of Intelligent Precision Healthcare Convergence, Sungkyunkwan University, Suwon, Korea, Republic of
Synopsis
Recently
we proposed an ultrafast 3D gradient-echo
imaging sequence using spatiotemporal-encoding (SPEN), called ERASE (Equal-TE Rapid Acquisition with Sequential
Excitation), which has
high tolerance to B0 inhomogeneities. Here, we investigated the noise characteristics, SNR, and tSNR of
ERASE with rat brain imaging at 9.4T at high spatial resolution, in comparison
with 2D and 3D gradient-echo EPI. While ERASE provided better tSNR than both of them, it
provided intermediate SNR between them. The ratio of physiological and thermal
noise (σP/σ0) and lambda (λ) were smaller in ERASE than 2D and 3D-EPI mainly due to its
robustness against B0 inhomogeneity.
Introduction
We recently proposed an
ultrafast 3D gradient-echo imaging sequence using spatiotemporal encoding
(SPEN) with constant TE, called ERASE (Equal-TE Rapid Acquisition and
Sequential Excitation)1, which has high immunity to B0
inhomogeneities. We previously reported that ERASE provides higher SNR, tSNR
and t-score maps than multislice 2D gradient-echo EPI (GE-EPI) when
thermal noise is more dominant than physiological noise,1 e.g., in
high spatial resolution. In this work, we examined the noise characteristics
such as the ratio of physiological and thermal noise (σP/σ0), lambda (λ), SNR and tSNR of ERASE in in
vivo rat brain imaging at 9.4T, in comparison with 2D-EPI and 3D-EPI.Method
Sequence:
Figure1 illustrates the ERASE sequence diagram (A) and schematic representation of its sequential and local
excitation and rephasing mechanism in the SPEN direction (B). ERASE provides a constant TE across slices via the insertion of
a rephasing gradient between spin excitation and acquisition processes along
the SPEN direction.1
Experiment: In vivo rat brain imaging was performed
at 9.4T (BioSpec, Bruker). Four male Sprague Dawley (SD) rats (280–310 g, 8–9
weeks of age) were used with
the approval of the Institutional Animal Care and Use Committee (IACUC)
at Sungkyunkwan University. Three
imaging sequences of ERASE, 2D-EPI and 3D-EPI were simultaneously applied to
each rat and 30 volumes were acquired with each sequence. Scan parameters are summarized in
Table 1. ERASE was
reconstructed offline with MATLAB (ver.8.2.0;
R2013b) using
the superresolution(SR) algorithm by Chen et. al.3 in the SPEN
direction.
Data
analysis: To reduce the effect of head
motion, image registration in each time series was performed with a reference
to the first image using SPM8 motion-correction software. Noise characteristics
were analyzed based on evaluation of SNR and tSNR. The ratio of physiological
thermal noise (sP/s0) was evaluated to assess the relative contribution of
physiological and thermal processes to each imaging technique by the following
equation:
$$\frac{\sigma_{p}}{\sigma_{o}}=\sqrt{(\frac{SNR_{o}}{tSNR})^{2} - 1} .[1]$$
Here, SNR0 was calculated pixelwise
by dividing each pixel value by the standard deviation of background noise (s0). tSNR was also calculated pixelwise by
dividing the mean pixel value across the 30 time-series images by the temporal fluctuations
(sF), where σF2 = σP2 + σ02. On
the other hand, σP is
commonly expressed as λ×S (λ, constant; S, the temporal mean signal)4,
where λ represents a measure of SNR degradation by
signal-dependent fluctuations and can be determined by the relationship between tSNR and SNR0:4,5
$$tSNR=\frac{SNR_{0}}{\sqrt{1+\lambda^{2}SNR_{0}^{2}}} .[2]$$ Results
Fgiure 2A shows presents
the tSNR and SNR maps of three center slices selected from rat brain images
obtained using 2D GE-EPI, 3D GE-EPI and ERASE. Image intensities were scaled
within a range of 0–60 in the SNR map, and 0–30 in the tSNR map. For better representation, the scatter plots of
all tSNR and SNR values in the whole brain were also presented (Fig.2B). Overall, ERASE provided better tSNR
than 2D and 3D GE-EPI, whereas it provided intermediate SNR between them. In
Fig.3A, the mean SNR and tSNR values were plotted in a bar graph
by averaging all the results over the whole brain, as obtained from four rats. σP/σ0 and l
were also presented in a bar graph (Figs. 3B, C). The σP/σ0 and l
values of ERASE were lower than 2D and 3D GE-EPI. Discussion & Conclusion
Here, we compared ERASE with
2D and 3D GE-EPI in terms of noise characteristics, SNR and tSNR ERASE provided
better tSNR than both of them and intermediate SNR between them, and showed
lower σP/σ0
and l values, which closely relate to
physiological noise, than both 2D and 3D GE-EPI. It is interesting to note that the physiological noise contribution to
ERASE is less than 2D GE-EPI because 3D GE-EPI is generally known to have more
physiological noise than 2D GE-EPI.5 In addition, from the fact that
l showed a similar value
in 2D and 3D GE-EPI, it is inferred that thermal noise was dominant over
physiological noise due to high spatial resolution in this study.
The reason why ERASE had less
physiological noise contribution might be
understood in the following respects: 1) Less sensitivity to the
breathing-induced B0 modulation over the whole brain owing to its
robustness against B0 inhomogeneity. 2) Less sensitivity to EPI artifacts such as Nyquist ghosting and image
distortion, which are the main sources of signal fluctuations. A further study
is needed to investigate the dependence on a field strength and spatial
resolution. Acknowledgements
This work was supported by NRF-2019M3C7A1031993 and IBS-R015-D1.References
[1] Ryu J-K et al. An equal-TE ultrafast
3D gradient-echo imaging method with high tolerance to magnetic susceptibility
artifacts: Application to BOLD functional MRI. Magnetic resonance in medicine.
2020; DOI: 10.1002/mrm.28564.
[2] Ryu J-K et al. A new ultrafast 3D gradient
echo-based imaging method using quadratic-phase encoding. Magnetic resonance in
medicine. 2019;82(1):237-250.
[3] Chen Y et al. Partial fourier
transform reconstruction for single-shot MRI linear frequency-swept excitation.
Magnetic resonance in medicine. 2013;69:1326-1336.
[4] Kruger G and Glover GH, Physiological
noise in oxygenation-sensitive magnetic resonance imaging. Magnetic resonance
in medicine. 2001;46:631-637.
[5] van der Zwaag W et al.
Temporal SNR Characteristics in Segmented 3D-EPI at 7T. Magnetic resonance in
medicine. 2012;67:344-352.
[6] Wald LL et al. Impacting the effect of
fMRI noise through hardware and acquisition choices – Implications for
controlling false positive rates. Neuroimage 2017;154:15-22.