Magnetic Resonance Electrical Impedance Tomography (MREIT) is a lately developed medical imaging modality visualizing static conductivity images of an electrically conducting object. MREIT was motivated to deal with the well-known ill-posedness of the image reconstruction problem of Electrical Impedance Tomography (EIT).

Numerous experiences have shown that practically measurable data sets in EIT system are insufficient for a robust reconstruction of a high-resolution static conductivity image due to its ill-posed nature and formidable influences of errors in forward modeling. To overcome the inherent ill-posed characteristics in EIT, MREIT system has been proposed in the early 1990s to use the internal data of magnetic flux density B=(B_x,B_y,B_z) which is induced by an externally injected current

MREIT uses an MRI scanner as a tool to measure the z-component B_z of the magnetic flux density where z is the axial magnetization direction of the MRI scanner. In 2001, Seo-Woo-Kwon-Yoon developed the first constructive B_z-based MREIT algorithm called the harmonic B_z algorithm and its numerical simulations showed that high-resolution conductivity image reconstructions are possible. This novel algorithm is based on the key observation that the Laplacian of B_z probes changes in log of the conductivity distribution along any equipotential curve having its tangent to the transversal projection of the induced current vector field (J_x,J_y,J_z). Since then, imaging techniques in MREIT have been advanced rapidly and now reached the stage of in vivo animal and human experiments.

Numerous experiences have shown that practically measurable data sets in EIT system are insufficient for a robust reconstruction of a high-resolution static conductivity image due to its ill-posed nature and formidable influences of errors in forward modeling. To overcome the inherent ill-posed characteristics in EIT, MREIT system has been proposed in the early 1990s to use the internal data of magnetic flux density B=(B_x,B_y,B_z) which is induced by an externally injected current

MREIT uses an MRI scanner as a tool to measure the z-component B_z of the magnetic flux density where z is the axial magnetization direction of the MRI scanner. In 2001, Seo-Woo-Kwon-Yoon developed the first constructive B_z-based MREIT algorithm called the harmonic B_z algorithm and its numerical simulations showed that high-resolution conductivity image reconstructions are possible. This novel algorithm is based on the key observation that the Laplacian of B_z probes changes in log of the conductivity distribution along any equipotential curve having its tangent to the transversal projection of the induced current vector field (J_x,J_y,J_z). Since then, imaging techniques in MREIT have been advanced rapidly and now reached the stage of in vivo animal and human experiments.

**Frequency-derivative electrical impedance tomography (fdEIT) **

Seo-EJ Woo proposed fdEIT to deal with technical difficulties of a conventional static EIT imaging method caused by unknown boundary geometry, uncertainty in electrode positions and other systematic measurement artifacts. In fdEIT, we try to produce images showing changes of a complex conductivity distribution with respect to frequency. Simultaneously injecting currents with at least two frequencies, we find differences of measured boundary voltages between those frequencies. In most previous studies, real parts of frequency-difference voltage data were used to reconstruct conductivity changes and imaginary parts to reconstruct permittivity changes.

This conventional approach is neglecting the interplay of conductivity and permittivity upon measured boundary voltage data. Our group proposed an improved fdEIT image reconstruction algorithm that properly handles the interaction. It uses weighted frequency differences of complex voltage data and a complex sensitivity matrix to reconstruct frequency-difference images of conductivity and permittivity. We found that there were two major sources of image contrast in fdEIT. The first is a contrast in conductivity and permittivity values between an anomaly and background. The second is a frequency-dependency of conductivity and permittivity distributions to be imaged. We note that even for the case where conductivity and permittivity do not change with frequency, the fdEIT algorithm may show a contrast in frequency-difference images of conductivity and permittivity distributions. On the other hand, even if conductivity and permittivity values significantly change with frequency, there is an example where we cannot find any contrast.

last update 2012.9.25 by Song Yizhuang

Research Topics

Introduction

Electrical Impedance Tomography

Magnetic Resonance EIT

Electrical Property Imaging

Elastography

LV contours in Ultrasound

Dental CT : Metal Artifacts Reduction

Bioimpedance spectroscopy

Quantitative susceptibility mapping

Image processing

Micro EIT

Surveillance

Lecture Notes

Algorithm

Electrical Impedance Tomography

Magnetic Resonance EIT

Electrical Property Imaging

Elastography

LV contours in Ultrasound

Dental CT : Metal Artifacts Reduction

Bioimpedance spectroscopy

Quantitative susceptibility mapping

Image processing

Micro EIT

Surveillance

Lecture Notes

Algorithm