Mihir Pendse1 and Brian Rutt1
1Stanford University, Stanford, CA, United States
Synopsis
We describe an extension of the IMPULSE pTx design algorithm
to enable simultaneous multislice (SMS) excitation. We introduce a strategy for integrating the optimal control
method for reducing peak power in SMS with the optimization of pTx channel
weightings. Desirable features of IMPULSE, including the ability to optimize spoke locations and to design pulses without SAR compression, are retained in this extension. We demonstrate that, even for large multiband acceleration factors,
our approach enables design of pTx pulses that minimize local SAR while
achieving acceptable in-slice homogeneity under strict peak power constraints. Purpose
Simultaneous multislice (SMS) has been recently described as
a method for significantly reducing acquisition time, decreasing TR or
increasing slice coverage. The major challenge in SMS pulse design is to reduce
peak power to abide by hardware limitations. At high field strengths, in-slice
flip angle inhomogeneity (FAI) and local SAR hotspots are additional criteria
that must be considered in the pulse design. Prior efforts to develop SAR-aware
SMS-pTx pulse design algorithms [1] only focused on optimizing channel weightings. The composite
RF waveform for the SMS-pTx pulse was formed through summation of a
conventional slice-selective subpulse modulated by appropriate slice
frequencies, which results in high peak power especially for large multiband
acceleration factors. Here we introduce two related approaches for SMS-pTx
based on an extension of the SAR-aware pulse design algorithm, IMPULSE [2], and
describe a strategy for using the two methods to design optimal SMS-pTx pulses
even for large number of slices with demanding peak power constraints.
Methods
We propose two methods, termed IMPULSE-SMS1 and IMPULSE-SMS2, that are each formulated to maximize pulse performance depending on whether the FAI tolerance or peak power limit is the more demanding constraint.
Both variations
extend the IMPULSE algorithm which finds the minimum SAR pTx pulse that
satisfies a tolerance on FAI by splitting the pTx
pulse design problem into two subproblems, a SAR-update and an FAI-update, each
of which can be solved efficiently. Two major benefits of IMPULSE, which are
retained here, include elimination of the need for SAR
compression (eg. VOPs [3]) and the ability to optimize k-space trajectory (eg.
spokes locations).
IMPULSE-SMS1 (Figure 1) involves first
using SLR design to find the RF waveform for the pTx sub-pulse, $$${\beta_{sub,1}(t)}$$$, that achieves the desired single-slice
profile (1a). Then IMPULSE is used to optimize the C*K*N channel weightings, $$${b_{c,k}^{(n)}}$$$, corresponding to a different set of channel weightings for each
slice (1b). The composite SMS-pTx pulse is then formed as: $$${\beta_{SMS,1}^{(c,k)}(t)=\sum_{n=1}^N{b_{c,k}^{(n)}\beta_{sub,1}(t)e^{-\gamma G_z z_n t}}}$$$ (1c).
IMPULSE-SMS2 (Figure 2) involves first designing
a single subpulse, $$${\beta_{sub,2}(t)}$$$, to
excite all slices in a way that limits peak power (2a). We chose to use
the optimal control approach for accomplishing this [4]. Then IMPULSE is
used to optimize the C*K channel weightings, $$${b_{c,k}}$$$, corresponding to a single set of channel weightings for all
slices (2b). The composite SMS-pTx pulse is then formed as: $$${\beta_{SMS,2}^{(c,k)}(t)={b_{c,k}\beta_{sub,2}(t)}}$$$ (2c).
We use both methods to optimize pTx pulses for two different design cases. For the first case, representing an
FAI-limited problem, we seek to excite 2 slices spaced 6 cm apart with FAI≤5%. For the second
case, representing a peak power-limited problem, we seek to excite 6 slices spaced 2
cm apart with FAI≤10%. We simulated B1+ and E fields using an 8-channel loop array (SEMCAD,
ZMT, Zurich) operating at 298 MHz (7T) and the Duke head model (IT’IS
Foundation, Zurich) to design SMS pulses to minimize SAR subject to a 600W peak
power constraint.
Results
For the case with 2 slices and a 5% FAI tolerance (Fig 3),
IMPULSE-SMS1 is able to achieve a peak local SAR of 1.24 W/kg which is better
than IMPULSE-SMS2 (2.13 W/kg). However, for 6 slices and a 10% FAI
tolerance (Fig 4), IMPULSE-SMS2 performs better with a peak local SAR of 8.47 W/kg
compared to 9.92 W/kg for IMPULSE-SMS1.
Discussion
For
low acceleration factors where peak power is of less concern, IMPULSE-SMS1 is
better able to achieve in-slice homogeneity because of the fact that there are
more degrees of freedom in the optimization since the channel weightings for
each slice are determined separately. However, for higher acceleration factors,
IMPULSE-SMS1 proves to be inadequate as it results in undesirable high SAR. A
significantly novel contribution of this work is IMPULSE-SMS2 which is an
effective method for addressing the problem of high peak power that results
from summation of the waveforms corresponding to each slice. By intelligently designing
the RF waveform upfront to excite all slices in a way that limits peak power,
the composite SMS-pTx pulse will be less likely to violate the hardware power
constraint. The results for the acceleration factor of 6 indicate that this
benefit outweighs the limited degrees of freedom in the IMPULSE-SMS2 optimization.
Conclusion
We have presented a general pulse design strategy, composed
of two extensions of the IMPULSE pTx design algorithm, that
enables combined SMS-pTx to achieve acceptable flip angle homogeneity over
multiple simultaneous slices. This method can be used to perform significantly accelerated high field imaging without sacrificing in plane flip angle homogeneity while abiding by SAR and peak power constraints.
Acknowledgements
No acknowledgement found.References
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