The D-bar method is a direct, non-iterative reconstruction algorithm for 2D EIT. It is based on Nachman’s (1996) constructive uniqueness proof (see Reconstruction Algorithms with Guarantees).

Steps (identifying , spectral parameter ):

  1. From the measured DtN map, compute the traces of the Complex Geometrical Optics Solutions on by solving a boundary integral equation.
  2. Compute the non-physical scattering transform
  3. For each , solve the -equation in with as .
  4. Recover .

Regularisation. With noisy data, is only reliable for small . Truncating to , with chosen according to the noise level, gives a provably convergent regularisation strategy (Knudsen et al. 2009). The result is a smoothed (low-pass) conductivity.

Variants. Approximations such as replace step 1 with a Born-type approximation. Deep D-bar (Hamilton & Hauptmann 2018) post-processes the blurry D-bar image with a U-Net to sharpen edges (see Deep Learning for EIT).

References

  1. A. I. Nachman (1996). Global Uniqueness for a Two-Dimensional Inverse Boundary Value Problem. Ann. of Math. 143(1), 71–96. doi:10.2307/2118653
  2. S. Siltanen, J. Mueller, D. Isaacson (2000). An implementation of the reconstruction algorithm of A Nachman for the 2D inverse conductivity problem. Inverse Problems 16(3), 681–699. doi:10.1088/0266-5611/16/3/310
  3. K. Knudsen, M. Lassas, J. L. Mueller, S. Siltanen (2009). Regularized D-bar method for the inverse conductivity problem. Inverse Probl. Imaging 3(4), 599–624. doi:10.3934/ipi.2009.3.599
  4. J. L. Mueller, S. Siltanen (2012). Linear and Nonlinear Inverse Problems with Practical Applications. SIAM. doi:10.1137/1.9781611972344
  5. S. J. Hamilton, A. Hauptmann (2018). Deep D-Bar: Real-Time Electrical Impedance Tomography Imaging With Deep Neural Networks. IEEE Trans. Med. Imaging 37(10), 2367–2377. doi:10.1109/TMI.2018.2828303