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Local electrical impedance tomography via projections

A. Jääskeläinen, A. Vavilov, J. Toivanen, A. Hänninen, V. Kolehmainen, N. Hyvönen

TL;DR

This work presents a projection-based framework for local electrical impedance tomography (EIT) that suppresses effects from conductivity changes outside a region of interest (ROI). By partitioning the domain into ROI and rest-of-domain (RONI) and constructing projections from a weighted nuisance Jacobian via left singular vectors, the method enables ROI-focused reconstructions from difference data. The approach integrates into a Bayesian linearized EIT solver with a smoothened total variation prior through a lagged diffusivity iteration, and is validated on three tank experiments including a head-shaped phantom to mimic stroke monitoring. Results show that partial projections onto the RONI can substantially reduce non-ROI artifacts and improve ROI localization, with performance depending on the chosen nuisance subspace and projection strategy. The framework offers a practical pathway to local EIT in clinical and industrial settings, while highlighting open issues in nuisance-subspace selection and nonlinear extensions.

Abstract

This paper introduces a method for approximately eliminating the effect that conductivity changes outside the region of interest have in electrical impedance tomography, allowing to form a local reconstruction in the region of interest only. The method considers the Jacobian matrix of the forward map, i.e., of the map that sends the discretized conductivity to the electrode measurements, at an initial guess for the conductivity. The Jacobian matrix is divided columnwise into two parts: one corresponding to the region of interest and a nuisance Jacobian corresponding to the rest of the domain. The leading idea is to project both the electrode measurements and the forward map onto the orthogonal complement of the span of a number of left-hand singular vectors for a suitably weighted nuisance Jacobian. The weighting can, e.g., account for the element sizes in a finite element discretization or to prior information on the conductivity outside the region of interest. The inverse problem is then solved by considering the projected relation between the measurements and the forward map, only reconstructing the conductivity in the region of interest. The functionality of the method is demonstrated by applying a reconstruction algorithm that combines lagged diffusivity iteration and total variation regularization to experimental data. In particular, data from a head-shaped water tank is considered, with the conductivity change in the region of interest mimicking growth of a hemorrhagic stroke and the changes outside the region of interest imitating physiological variations in the conductivity of the scalp.

Local electrical impedance tomography via projections

TL;DR

This work presents a projection-based framework for local electrical impedance tomography (EIT) that suppresses effects from conductivity changes outside a region of interest (ROI). By partitioning the domain into ROI and rest-of-domain (RONI) and constructing projections from a weighted nuisance Jacobian via left singular vectors, the method enables ROI-focused reconstructions from difference data. The approach integrates into a Bayesian linearized EIT solver with a smoothened total variation prior through a lagged diffusivity iteration, and is validated on three tank experiments including a head-shaped phantom to mimic stroke monitoring. Results show that partial projections onto the RONI can substantially reduce non-ROI artifacts and improve ROI localization, with performance depending on the chosen nuisance subspace and projection strategy. The framework offers a practical pathway to local EIT in clinical and industrial settings, while highlighting open issues in nuisance-subspace selection and nonlinear extensions.

Abstract

This paper introduces a method for approximately eliminating the effect that conductivity changes outside the region of interest have in electrical impedance tomography, allowing to form a local reconstruction in the region of interest only. The method considers the Jacobian matrix of the forward map, i.e., of the map that sends the discretized conductivity to the electrode measurements, at an initial guess for the conductivity. The Jacobian matrix is divided columnwise into two parts: one corresponding to the region of interest and a nuisance Jacobian corresponding to the rest of the domain. The leading idea is to project both the electrode measurements and the forward map onto the orthogonal complement of the span of a number of left-hand singular vectors for a suitably weighted nuisance Jacobian. The weighting can, e.g., account for the element sizes in a finite element discretization or to prior information on the conductivity outside the region of interest. The inverse problem is then solved by considering the projected relation between the measurements and the forward map, only reconstructing the conductivity in the region of interest. The functionality of the method is demonstrated by applying a reconstruction algorithm that combines lagged diffusivity iteration and total variation regularization to experimental data. In particular, data from a head-shaped water tank is considered, with the conductivity change in the region of interest mimicking growth of a hemorrhagic stroke and the changes outside the region of interest imitating physiological variations in the conductivity of the scalp.
Paper Structure (14 sections, 22 equations, 9 figures)

This paper contains 14 sections, 22 equations, 9 figures.

Figures (9)

  • Figure 3.1: Left: The first water tank with two embedded cylindrical inclusions made of conductive plastic. Right: The second water tank with one embedded cylindrical inclusion made of conductive plastic and sweet potato slices placed between a resistive collar and the boundary of the tank.
  • Figure 3.2: The current patterns used for different water tanks. The vertical axes correspond to electrode numbers and the horizontal axes to different current patterns. Red color indicates the source and blue color the sink of the 1 mA current injection. Left: The first cylindrical tank. Middle: The second cylindrical tank. Right: The head-shaped tank.
  • Figure 3.3: Top left: The head-shaped water tank with a cylindrical embedded inclusion made of conductive plastic inside a 3D-printed skull. Top right: The head-shaped water tank with an embedded inclusion made of conductive plastic and sweet potato slices placed between the skull and the boundary of the tank. Bottom: The FE head model used in the numerical computations.
  • Figure 6.1: First experiment: Horizontal cross-sections of reconstructions at heights 1 cm, 2 cm, 2.5 cm and 3.5 cm for the setup in the left image of Figure \ref{['fig:cylindrical_tanks']}. The unit of conductivity is S/m. Top: Reconstruction without projections in the whole domain. Middle: Reconstruction when ROI and RONI are, respectively, the top and bottom halves of the tank, and a projection with respect to the RONI is utilized. Bottom: Reconstruction computed only in the top half of the tank without any projections.
  • Figure 6.2: Second experiment: Horizontal cross-sections of reconstructions at heights 1 cm, 2 cm, 2.5 cm and 3.5 cm for the setup in the right image of Figure \ref{['fig:cylindrical_tanks']}. The unit of conductivity is S/m. Top: Reconstruction without projections in the whole domain. Bottom: Reconstruction when ROI is a concentric cylinder of radius 10 cm, the RONI is its complement, and a projection with respect to the RONI is utilized.
  • ...and 4 more figures

Theorems & Definitions (1)

  • Remark 5.1