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Geophysical Journal International· 2026Q1

A Cramér–Rao resolution limit for structural-parameter estimation in electrical resistivity tomography: interface dip, data noise and model error

Junghoon Choi

Short summary

A new Cramér–Rao bound (CRB) quantifies the noise-dependent resolution limit for estimating geological interface dip in electrical resistivity tomography (ERT), showing that improving geometric constraints is more impactful than reducing data noise.

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Key points

  • A Cramér–Rao bound (CRB) is derived to set a noise-dependent resolution limit for interface dip estimation in ERT.
  • The derived dip standard error is $\sigma _\theta \ge \sigma /\left\Vert \partial g_0/\partial \theta \right\Vert _{P_{\mathrm{ C}_0}}$ after profiling out background resistivity.
  • At 3% noise, the single-parameter resolution floor is 0.14–0.50°, and the geometry-marginalized floor is 0.33–0.72°.
  • Model misspecification (incorrect geometry) causes a 3–5° dip bias, 6–25 times larger than the formal resolution floor.
  • Improving independent geometric constraints is more beneficial than reducing data noise for the tested cases.

AI-generated from the title and abstract; the full text is not read.

Abstract

SUMMARY Dip is often read from a regularized electrical resistivity tomography image without a parameter-specific uncertainty. Image-resolution measures describe how an inversion blurs the resistivity field, but they do not give a noise-dependent limit for the dip of a geological interface. We derive that limit from the 2.5-D forward operator using Fisher information and a Cramér–Rao bound (CRB). The background resistivity is profiled out in log-data space. For a specified structural family, the dip standard error satisfies $\sigma _\theta \ge \sigma /\left\Vert \partial g_0/\partial \theta \right\Vert _{P_{\mathrm{ C}_0}}$. We also derive a marginal bound for unknown geometry and a first-order bias caused by structural misspecification. Tests with a 30-electrode dipole–dipole array show that the maximum-likelihood estimate attains the CRB when the fitted family is correct. At 3 per cent noise, the single-parameter floor is 0.14–$0.50{}^{\circ }$ and the geometry-marginalized floor is 0.33–$0.72{}^{\circ }$. Holding a coupled geometry parameter one cell away from its true value instead produces a 3–$5{}^{\circ }$ dip bias. This is 6–25 times the formal floor. An ablation attributes most of the bias to thickness, width or depth rather than resistivity contrast. The result is conditional on the chosen model family: The CRB measures noise-limited precision within that family, whereas the bias measures the cost of using the wrong geometry. For the cases tested here, improving an independent geometric constraint is therefore more useful than further reducing data noise.

The authors' abstract, as published at the source. Geophysical Journal International, 2026 · DOI ↗

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GeophysicsEarth and Planetary Sciences