R.F. Remis
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1
This thesis systematically investigates the application of several model compression methods, such as low-rank factorization, knowledge distillation, and quantization, to enhance the efficiency of a baseline MR reconstruction neural network. By exploring multiple variations within each compression technique, this study evaluates their impact on key performance metrics such as inference speed, model size reduction, and reconstruction accuracy. Extensive tests show significant trade-offs between image fidelity and computational efficiency, providing insights into the practical feasibility of deploying compressed models in clinical workflows.
Among the techniques tested, low-rank factorization implemented via Tucker decomposition emerged as the most effective approach. This method achieved a threefold reduction in inference time while maintaining high reconstruction quality, highlighting its potential to improve MRI processing times in real-world applications significantly. ...
This thesis systematically investigates the application of several model compression methods, such as low-rank factorization, knowledge distillation, and quantization, to enhance the efficiency of a baseline MR reconstruction neural network. By exploring multiple variations within each compression technique, this study evaluates their impact on key performance metrics such as inference speed, model size reduction, and reconstruction accuracy. Extensive tests show significant trade-offs between image fidelity and computational efficiency, providing insights into the practical feasibility of deploying compressed models in clinical workflows.
Among the techniques tested, low-rank factorization implemented via Tucker decomposition emerged as the most effective approach. This method achieved a threefold reduction in inference time while maintaining high reconstruction quality, highlighting its potential to improve MRI processing times in real-world applications significantly.
re reconstructed using two-dimensional contrast source inversion, due to a significant complexity reduction in comparison to its three-dimensional counterpart, allowing for reconstructions in a reasonable amount of time. Data acquisition is usually performed using a shielded
irdcage coil. Current methods, however, disregard the presence of this shielding, only accounting for it using a rough first-order approximation, as properly accounting for it would lead to an intractable computational load. This thesis shows a method of analytically describing this
hielding in the Greens functions and its efficient implementation in the corresponding Greens operators for CSI-EPT, exploiting the Greens functions being degenerate. This results in a significant increase in the reconstruction performance both qualitatively and quantitatively, at the cost of a slight increase of the computational load. The inversion problem being ill-posed leads to poor reconstruction performance on noisy data. This thesis presents a method for quantization of the tissue parameters, by enforcing a multi-modal distribution for these parameters.
through simulation, the quantization method shows a significant increase in performance for noisy data, at the cost of losing smaller details in the image. This improved model was tested on synthetic E-polarized data, and realistic three-dimensional data, showing a more robust, and
accurate reconstruction of the electrical properties for both. ...
re reconstructed using two-dimensional contrast source inversion, due to a significant complexity reduction in comparison to its three-dimensional counterpart, allowing for reconstructions in a reasonable amount of time. Data acquisition is usually performed using a shielded
irdcage coil. Current methods, however, disregard the presence of this shielding, only accounting for it using a rough first-order approximation, as properly accounting for it would lead to an intractable computational load. This thesis shows a method of analytically describing this
hielding in the Greens functions and its efficient implementation in the corresponding Greens operators for CSI-EPT, exploiting the Greens functions being degenerate. This results in a significant increase in the reconstruction performance both qualitatively and quantitatively, at the cost of a slight increase of the computational load. The inversion problem being ill-posed leads to poor reconstruction performance on noisy data. This thesis presents a method for quantization of the tissue parameters, by enforcing a multi-modal distribution for these parameters.
through simulation, the quantization method shows a significant increase in performance for noisy data, at the cost of losing smaller details in the image. This improved model was tested on synthetic E-polarized data, and realistic three-dimensional data, showing a more robust, and
accurate reconstruction of the electrical properties for both.
Background: Chronic kidney disease (CKD) affects over one in ten individuals worldwide and has a high mortality rate. As renal microvascular dysfunction plays a key role in CKD progression, accurate and non-invasive quantification of renal perfusion is valuable. ASL magnetic resonance imaging (MRI) enables the measurement of renal perfusion without exogenous contrast agents and has been validated at 1.5 T and 3 T. However, its feasibility at 0.6 T has not yet been investigated.
Methodology: Data from the NEO-2 study acquired at 3 T was analyzed using a pipeline that included image registration, segmentation, and quantitative perfusion mapping. Midfield scanners have a lower signal-to-noise ratio and altered relaxation times. Therefore, the existing renal ASL sequence used in 3 T was adjusted. The sequence parameters that were modified included the repetition time (TR), the number of control–label pairs, voxel size, post-label delay (PLD), and background suppression (BGS) pulse timings. After choosing the optimal parameters, a healthy volunteer was scanned back-to-back at both field strengths for direct comparison.
Results: At 3~T, cortical perfusion values ranged between 180 and 286 mL/100g/min, consistent with literature. Optimal parameters at 0.6 T were: TR = 4000 ms, 25 control–label pairs, in-plane resolution of 4×4 mm^2, slice thickness of 10 mm, and PLD = 1400 ms with BGS pulses at 700 & 1100 ms. With these settings applied at 0.6 T, the cortical perfusion values were 215.34 ± 67.92 and 236.80 ± 66.33 mL/100 g/min in the left and right cortex, respectively. Using the 3 T acquisition protocol, the corresponding values were 241.89 ± 76.55 and 250.75 ± 70.82 mL/100g/min, respectively. Values at 3 T were approximately 5–10% higher.
Conclusion: The results show that renal ASL at 0.6~T can produce quantitative perfusion estimates that are similar to those at 3 T.
...
Background: Chronic kidney disease (CKD) affects over one in ten individuals worldwide and has a high mortality rate. As renal microvascular dysfunction plays a key role in CKD progression, accurate and non-invasive quantification of renal perfusion is valuable. ASL magnetic resonance imaging (MRI) enables the measurement of renal perfusion without exogenous contrast agents and has been validated at 1.5 T and 3 T. However, its feasibility at 0.6 T has not yet been investigated.
Methodology: Data from the NEO-2 study acquired at 3 T was analyzed using a pipeline that included image registration, segmentation, and quantitative perfusion mapping. Midfield scanners have a lower signal-to-noise ratio and altered relaxation times. Therefore, the existing renal ASL sequence used in 3 T was adjusted. The sequence parameters that were modified included the repetition time (TR), the number of control–label pairs, voxel size, post-label delay (PLD), and background suppression (BGS) pulse timings. After choosing the optimal parameters, a healthy volunteer was scanned back-to-back at both field strengths for direct comparison.
Results: At 3~T, cortical perfusion values ranged between 180 and 286 mL/100g/min, consistent with literature. Optimal parameters at 0.6 T were: TR = 4000 ms, 25 control–label pairs, in-plane resolution of 4×4 mm^2, slice thickness of 10 mm, and PLD = 1400 ms with BGS pulses at 700 & 1100 ms. With these settings applied at 0.6 T, the cortical perfusion values were 215.34 ± 67.92 and 236.80 ± 66.33 mL/100 g/min in the left and right cortex, respectively. Using the 3 T acquisition protocol, the corresponding values were 241.89 ± 76.55 and 250.75 ± 70.82 mL/100g/min, respectively. Values at 3 T were approximately 5–10% higher.
Conclusion: The results show that renal ASL at 0.6~T can produce quantitative perfusion estimates that are similar to those at 3 T.
Contrast Source Inversion Electrical Property Tomography
Is the two-dimensional CSI algorithm feasible on realistic three-dimensional data?
This 2D-CSI algorithm is significantly faster than its three-dimensional (3D) counterpart. However, reconstruction artefacts may appear since the 2D field description is not always applicable. In this thesis, these artefacts are identified and it is investigated if the 2D-CSI algorithm can be improved to handle them. In particular, the proposed updates are, first, implementing the early stopping principle, then adding a positivity constraint to the conductivity and relative permittivity, and lastly, initialising with Helmholtz electrical property tomography (HEPT). The first two enhancements create a more robust algorithm, while the third update could be useful only in specific cases (with no fine structures and low noise levels).
After achieving a more robust algorithm, the 2D-CSI algorithm is applied to the realistic 3D dataset ”A Database for MR-based Electrical Properties Tomography” (ADEPT). The first and foremost challenge is accurately simulating the incident field, as the reconstructions depend a lot on the incident fields. If the incident fields do not match perfectly, the algorithm can only produce satisfactory reconstruction results in a part of the reconstruction domain. The reconstructions are only partly accurate because the reconstructed electric fields converge to a line creating line artefacts. It is shown that small changes in the incident fields produce small changes in the position of the artefacts. Based on this observation, a reconstruction strategy has been developed in which a reconstruction without artefacts is produced by combining reconstruction results of multiple incident fields. Integrating all modifications of the 2D-CSI
algorithm in one single framework shows that the conductivity and relative permittivity of the brain in the middle of the birdcage coil can be reconstructed accurately ...
This 2D-CSI algorithm is significantly faster than its three-dimensional (3D) counterpart. However, reconstruction artefacts may appear since the 2D field description is not always applicable. In this thesis, these artefacts are identified and it is investigated if the 2D-CSI algorithm can be improved to handle them. In particular, the proposed updates are, first, implementing the early stopping principle, then adding a positivity constraint to the conductivity and relative permittivity, and lastly, initialising with Helmholtz electrical property tomography (HEPT). The first two enhancements create a more robust algorithm, while the third update could be useful only in specific cases (with no fine structures and low noise levels).
After achieving a more robust algorithm, the 2D-CSI algorithm is applied to the realistic 3D dataset ”A Database for MR-based Electrical Properties Tomography” (ADEPT). The first and foremost challenge is accurately simulating the incident field, as the reconstructions depend a lot on the incident fields. If the incident fields do not match perfectly, the algorithm can only produce satisfactory reconstruction results in a part of the reconstruction domain. The reconstructions are only partly accurate because the reconstructed electric fields converge to a line creating line artefacts. It is shown that small changes in the incident fields produce small changes in the position of the artefacts. Based on this observation, a reconstruction strategy has been developed in which a reconstruction without artefacts is produced by combining reconstruction results of multiple incident fields. Integrating all modifications of the 2D-CSI
algorithm in one single framework shows that the conductivity and relative permittivity of the brain in the middle of the birdcage coil can be reconstructed accurately
Total variation (TV) regularization has been shown to perform noise reduction in the iterative Contrast Source Inversion EPT (CSI-EPT) method. The Jacobi matrix inversion regularization, an alternative to the known conjugate gradient formulation, is elaborated and applied to an E-polarized MRI fields scenario such that this thesis presents the Jacobi step regularized CSI-EPT.
The alternative regularization method outperforms the known regularization method in the reconstruction qualities of noise-suppression and edge-preservation in the simulated MRI experiments using a virtual body model. Further advancements are also described, such as multiple inner-iterations Jacobi regularization and an anatomical prior initialization of the contrast function. Important future research topics are the incorporation and evaluation of the Jacobi step regularization into more advanced CSI-EPT versions, which are the three-dimensional and transceive phase based algorithms to correct realistic MRI data. ...
Total variation (TV) regularization has been shown to perform noise reduction in the iterative Contrast Source Inversion EPT (CSI-EPT) method. The Jacobi matrix inversion regularization, an alternative to the known conjugate gradient formulation, is elaborated and applied to an E-polarized MRI fields scenario such that this thesis presents the Jacobi step regularized CSI-EPT.
The alternative regularization method outperforms the known regularization method in the reconstruction qualities of noise-suppression and edge-preservation in the simulated MRI experiments using a virtual body model. Further advancements are also described, such as multiple inner-iterations Jacobi regularization and an anatomical prior initialization of the contrast function. Important future research topics are the incorporation and evaluation of the Jacobi step regularization into more advanced CSI-EPT versions, which are the three-dimensional and transceive phase based algorithms to correct realistic MRI data.
VoNA The Visualisation of Neuronal Activation
To observe and shape electrode-generated outputs for electrical stimulation in the brain using a Finite Element Model
A straightforward, effective, and computationally fast backprojection imaging method is proposed that provides an indication of the regions in a given volume of cardiac tissue that exhibit prominent irregular atrial activity. The chosen volume is subdivided into non-overlapping voxels, and the standard electrogram signal model is discretized to a matrix multiplication form. The inverse problem of reconstructing the transmembrane current distribution in the volume is solved using the epicardial electrogram readings obtained from the surface and the inverse distances matrix containing the inverse of the distances from each electrode to each voxel within the volume domain. The generated backprojection images are visualized to estimate the location (x and y coordinate information) and depth of irregular atrial activity in the volume. To improve the accuracy of localization while maintaining the computationally fast nature of the proposed solution, Singular Value decomposition (SVD) of the inverse distances matrix is proposed for the transmembrane current reconstruction. The obtained visual estimates can guide ablation procedures, making them more targeted, and reducing the need for repeat ablation procedures due to AF recurrence.
...
A straightforward, effective, and computationally fast backprojection imaging method is proposed that provides an indication of the regions in a given volume of cardiac tissue that exhibit prominent irregular atrial activity. The chosen volume is subdivided into non-overlapping voxels, and the standard electrogram signal model is discretized to a matrix multiplication form. The inverse problem of reconstructing the transmembrane current distribution in the volume is solved using the epicardial electrogram readings obtained from the surface and the inverse distances matrix containing the inverse of the distances from each electrode to each voxel within the volume domain. The generated backprojection images are visualized to estimate the location (x and y coordinate information) and depth of irregular atrial activity in the volume. To improve the accuracy of localization while maintaining the computationally fast nature of the proposed solution, Singular Value decomposition (SVD) of the inverse distances matrix is proposed for the transmembrane current reconstruction. The obtained visual estimates can guide ablation procedures, making them more targeted, and reducing the need for repeat ablation procedures due to AF recurrence.
Using these algorithms on simulated data, it was shown that promising results can be achieved for both transmembrane current estimations and LAT estimations. Several wavelet support sizes were tested on the simulated data to observe performance changes. These were compared to an already existing LAT estimation algorithm. The results mainly confirm the efficiency of the proposed methods on severely diseased tissue corrupted by conduction blocks and noise. ...
Using these algorithms on simulated data, it was shown that promising results can be achieved for both transmembrane current estimations and LAT estimations. Several wavelet support sizes were tested on the simulated data to observe performance changes. These were compared to an already existing LAT estimation algorithm. The results mainly confirm the efficiency of the proposed methods on severely diseased tissue corrupted by conduction blocks and noise.
Deep Learning Enhanced Contrast Source Inversion And Phase Error Based Conductivity Correction For Electrical Properties Tomography
Exploration Of Physics-Assisted Deep Learning Methodology For Magnetic Resonance Based Electrical Properties Tomography
Evaluation of Direct FID-Based Dielectric Parameter Retrieval in MRI
Generalized Signal Models
tween the two and thus it is concluded that it can be used. Using a single emitting loop, the effect of varying conductivity was simulated for a dielectric sphere placed in free space, with the single emitting loop submerged into the solution. The simulations showed that by increasing the conductivity, the measured voltage at the receiver coil reduces. Note that this simulation was performed twice, for relative
permittivity values εr = 1 and εr = 80. The reason for choosing these two values was to first eliminate the effect of relative permittivity εr = 1 and to simulate a water-based solution εr = 80. Simulations verified that for εr = 1, the measured voltage at the receiver location is lower than εr = 80. After verifying the full-wave model and observing the effect of varying the electrical conductivity, two more simulations were performed to prepare for the experiment. In the first simulation, instead of a single loop, a series of loops was used to simulate the beam excitation of an MRI. As it is shown in the results, there is not a linear correlation between increasing the conductivity and the induced voltage at the receiver coil. Secondly, the experimental setup was simulated. In addition to the previous simulation, a plastic layer was added to the outside of the ball, to model the plastic sphere used during the experiment. In chapter 4, the results of the experiment are introduced. The results from the experiment could not justify the simulations due to reasons that are explained in the conclusions. ...
tween the two and thus it is concluded that it can be used. Using a single emitting loop, the effect of varying conductivity was simulated for a dielectric sphere placed in free space, with the single emitting loop submerged into the solution. The simulations showed that by increasing the conductivity, the measured voltage at the receiver coil reduces. Note that this simulation was performed twice, for relative
permittivity values εr = 1 and εr = 80. The reason for choosing these two values was to first eliminate the effect of relative permittivity εr = 1 and to simulate a water-based solution εr = 80. Simulations verified that for εr = 1, the measured voltage at the receiver location is lower than εr = 80. After verifying the full-wave model and observing the effect of varying the electrical conductivity, two more simulations were performed to prepare for the experiment. In the first simulation, instead of a single loop, a series of loops was used to simulate the beam excitation of an MRI. As it is shown in the results, there is not a linear correlation between increasing the conductivity and the induced voltage at the receiver coil. Secondly, the experimental setup was simulated. In addition to the previous simulation, a plastic layer was added to the outside of the ball, to model the plastic sphere used during the experiment. In chapter 4, the results of the experiment are introduced. The results from the experiment could not justify the simulations due to reasons that are explained in the conclusions.
Compressed Sensing in Low-Field MRI
Using Multiplicative Regularization
In this work we rewrite and implement the regularization functions in a multiplicative manner by multiplying the data fidelity term with the regularization terms, thereby eliminating the need to tune the regularization parameters. Moreover, we include a region of support (ROS) mask to further accelerate reconstruction. The performance of different combinations of regularization functions and reconstruction algorithms are validated on a simulation study and various experiments on a low-field MRI scanner. This also shows the capability of CS applied to low-field MRI, which has lower signal-to-noise ratio compared to conventional MRI. Of all proposed methods, a nonlinear conjugate gradient method applied to the fully multiplicatively regularized objective function shows the most robust performance. ...
In this work we rewrite and implement the regularization functions in a multiplicative manner by multiplying the data fidelity term with the regularization terms, thereby eliminating the need to tune the regularization parameters. Moreover, we include a region of support (ROS) mask to further accelerate reconstruction. The performance of different combinations of regularization functions and reconstruction algorithms are validated on a simulation study and various experiments on a low-field MRI scanner. This also shows the capability of CS applied to low-field MRI, which has lower signal-to-noise ratio compared to conventional MRI. Of all proposed methods, a nonlinear conjugate gradient method applied to the fully multiplicatively regularized objective function shows the most robust performance.
Low Field Magnetic Resonance Imaging of the Eye
Inexpensive MRI for Ocular Conditions
Design requirements are a scan time of less than 4 minutes; resolution of 1.0 mm isotropic; Field of View (FOV) large enough to contain the eye and the orbit; contrast sufficient to distinguish the sclera, vitreous, tumour, lens and lipid. The experimental setup consists of a 46 mT Halbach-array based scanner, a volume coil as transmit coil and a custom-built surface coil as receive coil. Images are made of a water phantom to characterise the FOV, and a porcine eye to characterise the contrast.
The FOV is found to meet the requirements, and the contrast is sufficient to distinguish the sclera, vitreous, lens and lipid in porcine eyes. The resolution is too low and the scans take too long (about 5 minutes at a resolution of 1.0 × 1.0 × 7.5 mm). Increasing the resolution and decreasing the scan time will result in a low Contrast to Noise Ratio (CNR), causing the contrast requirement to be violated. Fast, high-resolution three-dimensional imaging is therefore not feasible on the current system.
The CNR can be improved by using a higher field strength, which requires the development of new hardware. Furthermore, in order to develop a clinically useable system, it is necessary to determine tumour contrast, design optimised pulse sequences, and test the method on human subjects. ...
Design requirements are a scan time of less than 4 minutes; resolution of 1.0 mm isotropic; Field of View (FOV) large enough to contain the eye and the orbit; contrast sufficient to distinguish the sclera, vitreous, tumour, lens and lipid. The experimental setup consists of a 46 mT Halbach-array based scanner, a volume coil as transmit coil and a custom-built surface coil as receive coil. Images are made of a water phantom to characterise the FOV, and a porcine eye to characterise the contrast.
The FOV is found to meet the requirements, and the contrast is sufficient to distinguish the sclera, vitreous, lens and lipid in porcine eyes. The resolution is too low and the scans take too long (about 5 minutes at a resolution of 1.0 × 1.0 × 7.5 mm). Increasing the resolution and decreasing the scan time will result in a low Contrast to Noise Ratio (CNR), causing the contrast requirement to be violated. Fast, high-resolution three-dimensional imaging is therefore not feasible on the current system.
The CNR can be improved by using a higher field strength, which requires the development of new hardware. Furthermore, in order to develop a clinically useable system, it is necessary to determine tumour contrast, design optimised pulse sequences, and test the method on human subjects.
Image Reconstruction for Multicoil Low-field MRI
Reconstructing MR images based on incomplete multicoil data and object support information