Yuan Zheng1, Yu Ding1, Qing Wei2, Rongxing Zhang2, and Weiguo Zhang1
1UIH America, Houston, TX, United States, 2United Imaging Healthcare, Shanghai, China
Synopsis
In simultaneous multi-slice (SMS) imaging, the multi-band RF pulses have
complicated waveforms and may suffer from distortions, which can cause sideband
excitations and result in image artifacts. We have proposed a simple method for
correcting the RF distortions using a prescan of the RF output, which can be
conveniently integrated in general SMS applications to suppress such artifacts
with a negligible increase of scan time.
Introduction
Simultaneous Multi-Slice (SMS) imaging is a technique that improves the
time efficiency of MRI pulse sequences by exciting and imaging multiple slices
at the same time1. It is closely related to in-plane parallel
imaging in that both techniques need multi-channel coil arrays for data
collection, and aliased images are separated using coil sensitivity variations.
However, unlike in-plane parallel imaging which is achieved by adjusting the
k-space sampling pattern, SMS imaging requires accurately broadcasting of complex multi-band
(MB) RF waveforms for excitation. Distortions caused by the transmit chain
could lead to additional excitation bands, which will show up as image
artifacts. In this abstract, we present a method for eliminating the undesired
sideband excitations by correcting MB RF waveforms using a prescan. Direct
measurement of the RF output showed significantly suppressed sidebands; The SMS
image artifacts were also effectively removed.Methods
We propose the following method for suppressing the excitation
sidebands (Fig.1). After the initial MB RF waveform is prepared according to
user inputs, it is broadcasted and the RF output is sampled, which
typically takes only a few milliseconds. The frequency profile is subsequently
analyzed. Since the intended excitation bands are known, it is straightforward
to extract the sidebands using a mask. The compensation time-domain RF waveform
is calculated by inverse Fourier transform of the inverted sidebands. Finally,
the corrected MB RF waveform is generated by adding the compensation waveform
to the initial MB RF waveform, which can then be used for SMS imaging.
The amount of RF distortion strongly depends on the hardware. Here we chose
an RF transmit chain with relatively large distortions in order to effectively
show this problem and demonstrate the proposed correction technique. An MB RF
pulse was generated by combining 2 identical 90 degree SLR pulses2
24 KHz apart. The time-bandwidth product of the SLR pulse was 6 and the
duration was 4 ms. The RF output before and after correction were directly
sampled by an integrated loop and compared to the input waveform.
We also performed SMS imaging and compared the artifact level with and
without RF correction. Images of a water cylinder phantom were acquired on a 1.5T
uMR 560 scanner (United Imaging Healthcare, Shanghai, China) with a 16 channel
head coil. The same RF transmit chain as used for Fig.2 and 3 was installed for
this test. An SMS gradient-echo EPI sequence was used for data collection.
Images were acquired with: slice thickness = 3.5 mm, FOV = 230 x 230 mm,
resolution = 112 x 112, FA = 90 deg, TE = 61 ms, number of slices = 34, BW = 1910
Hz/pixel, MB factor = 2. For the purpose of this experiment, controlled
aliasing was not applied. Single-band calibration images were acquired
separately, and the slice-GRAPPA algorithm3 was used for image
reconstruction.Results
Fig.2 shows the time domain waveform comparison between the RF input
and output without correction. Distortions can be easily identified. Fig.3
compares the frequency spectra of RF output before and after correction. The 1st
sidebands were about 8% the size of the main bands before correction, and were suppressed
to under 1% using the corrected RF waveform. Fig.4 shows selected slices of
the SMS images. The image artifacts caused by undesired sideband excitations
were largely removed using the proposed RF correction technique.Discussion
MB pulses have complex waveforms (Fig.2) that demand high fidelity of
the RF transmit chain. Hardware that perform well on typical single-band pulses
may show some degrees of distortion that may lead to image artifacts. We have
demonstrated the proposed RF correction method with an MB = 2 waveform.
However, it should be straightforward to extend this technique to correct more complex
RF pulses, such as the ones with higher MB factors, as long as the undesired
excitation bands can be separated from the intended excitation bands. It is
also worth noting that the prescan only directly samples the RF output instead
of MR signals, taking just a few milliseconds. Finally, we would like to point
out that this technique can be used iteratively, i.e., the remaining undesired
excitations in Fig.3 after correction can be further suppressed by adding a
compensation pulse that cancels the residual sidebands.Conclusion
The distortion of MB RF pulses in SMS imaging can lead to sideband
excitations, which may result in image artifacts. We have proposed a simple and
reliable method for correcting the MB RF distortions using a fast prescan,
which can be conveniently integrated in general SMS applications to suppress
such artifacts with a negligible increase of scan time.Acknowledgements
No acknowledgement found.References
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