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An Optimal Design Method for MRI Teardrop Gradient Waveforms
Tingting Ren Joint work with Christopher Anand and Tamás Terlaky
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Overview Introduction Original Optimization Model
Improved Optimization Model Conclusion Future work 11/14/2018
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Introduction Radio Frequency (RF) pulses excite the spins
Field gradients spatial encode the spins Large uniform static RF coil receives a signal Large uniform static external magnetic field Signal: Amplified Digitized Fourier-Transformed 11/14/2018
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The Conventional Spatial Frequency Patterns and 2D Imaging Methods
Echo Planar Imaging Projection Reconstruction 2DFT Imaging 11/14/2018
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Fast Imaging : acquire a greater portion of k-space per signal
Interleaved spiral Square spiral Spiral Resample Inverse FT Fast Imaging : acquire a greater portion of k-space per signal readout. The gradient system must be able to generate the trajectory. 11/14/2018
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The Theory of Teardrop Steady State Free Precession imaging (i.e. SSFP) requires balanced gradient waveforms. Conventionally, this is done by adding read, slice and phase rewinders. waste time generate high dB/dt By using a non-raster trajectory beginning and ending in the center of k-space, a teardrop readout requires neither read nor phase dephase/rephase lobes, increasing scan-time efficiency. 11/14/2018
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The Advantages of Teardrop
objective = radius = resolution designed to follow an interleaved spiral like trajectory leaving the center of k-space, and returning on the mirror image trajectory to the center of k-space . Family of waveforms, increasing scan time efficiency. 100% readout ( no rewinders). 11/14/2018
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We acquired ungated, free breathing cardiac images using non optimal teardrop readout sequence. The image displays good blood/septum contrast to noise. We can expect better result with our optimal teardrop readout trajectory. X-section of Dr. Anand 11/14/2018
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Original Optimization Model
The design goal of the teardrop is to maximize resolution when obey the Nyquist sampling condition for the given FOV, and remain within the gradient strength and slew limits of the given system. Parameter Sets: A discrete series of point-by-point gradient amplitudes: A set of points in k-space: From Fourier transform, we know 11/14/2018
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Objective Constraints Gradient System Hardware Limitations
For a fixed FOV, the basic technique for fast imaging is to acquire larger portion on k-space per signal readout. So our objective function is if is an even number if is an odd number Constraints Gradient System Hardware Limitations Objective or Amplitude Limits 11/14/2018
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Slew or Rise Time Limits
Gradient Start and End Amplitudes The beginning and the end of k-space trajectory Constrains to keep a teardrop k-space trajectory 11/14/2018
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The Spiral Constraints
So the constraint is 11/14/2018
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By using atan function, we can simplify this constraint significantly.
Making the readout gradient motion-insensitive requires that we zero the first moment, which is a global constraint First Moment Nulling 11/14/2018
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Model 11/14/2018
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Results We used five nonlinear softwares: IPOPT, LOQO, KNITRO,
SNOPT and FILTER to solve the model with various parameters. We got almost the same optimal results in each case. Here is the optimal trajectory where = 0.04 T/m, = 150 T/m/s, TR = 4ms, and N=50 ( 101 sampling points ). 11/14/2018
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Rotating the associated gradient profiles is equivalent to rotating
the trajectory around the center of k-space. Together the combined views cover k-space, as evidenced by a partial set of views ( three interleaves ). 11/14/2018
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Improved Optimization Model
Add a new set of points in k-space as design variables: Replace the spiral constraints by two new constraints: (1) (2) Recalculate the quadratic constraints, solve the optimization problem again. 11/14/2018
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How to calculate at each step
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Model Repeat { Recalculate } until obj < ( previous_obj + tolerance) 11/14/2018
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Results Objective Function = 52490 25 31 30 11/14/2018
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Objective Function = 93481 31 32 25 11/14/2018
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Objective Function = 32 33 25 11/14/2018
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Objective Function = 25 33 32 11/14/2018
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Objective Function = 33 32 25 11/14/2018
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Objective Function = 25 32 33 11/14/2018
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Conclusions We have modeled 2D teardrop design using nonlinear and second order cone methods including Global constraints ( moment nulling ) Commercial solves can solve both models quickly Good foundation for 3D model. 11/14/2018
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Future Work Generalize 2D model to 3D model.
We may add other constraints to the model, like second moment nulling, which would reduce image artifacts caused by pulsatile flow, just as first moment nulling reduces the effect of constant flow. Test on MRI machine. 11/14/2018
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Thank you! 11/14/2018
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