4.2 Article

Toward robust deconvolution of pass-through paleomagnetic measurements: new tool to estimate magnetometer sensor response and laser interferometry of sample positioning accuracy

Journal

EARTH PLANETS AND SPACE
Volume 68, Issue -, Pages -

Publisher

SPRINGER HEIDELBERG
DOI: 10.1186/s40623-016-0493-2

Keywords

Superconducting rock magnetometer; Pass-through measurement; Sensor response; Deconvolution; Laser interferometry; Geomagnetic excursion; U-channel; Sediment long-core sample

Funding

  1. JSPS [25247082, 25247073, PE14034]
  2. University of Southampton
  3. Grants-in-Aid for Scientific Research [25247082, 25247073] Funding Source: KAKEN

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Pass-through superconducting rock magnetometers (SRM) offer rapid and high-precision remanence measurements for continuous samples that are essential for modern paleomagnetism studies. However, continuous SRM measurements are inevitably smoothed and distorted due to the convolution effect of SRM sensor response. Deconvolution is necessary to restore accurate magnetization from pass-through SRM data, and robust deconvolution requires reliable estimate of SRM sensor response as well as understanding of uncertainties associated with the SRM measurement system. In this paper, we use the SRM at Kochi Core Center (KCC), Japan, as an example to introduce new tool and procedure for accurate and efficient estimate of SRM sensor response. To quantify uncertainties associated with the SRM measurement due to track positioning errors and test their effects on deconvolution, we employed laser interferometry for precise monitoring of track positions both with and without placing a u-channel sample on the SRM tray. The acquired KCC SRM sensor response shows significant cross-term of Z-axis magnetization on the X-axis pick-up coil and full widths of similar to 46-54 mm at half-maximum response for the three pick-up coils, which are significantly narrower than those (similar to 73-80 mm) for the liquid He-free SRM at Oregon State University. Laser interferometry measurements on the KCC SRM tracking system indicate positioning uncertainties of similar to 0.1-0.2 and similar to 0.5 mm for tracking with and without u-channel sample on the tray, respectively. Positioning errors appear to have reproducible components of up to similar to 0.5 mm possibly due to patterns or damages on tray surface or rope used for the tracking system. Deconvolution of 50,000 simulated measurement data with realistic error introduced based on the position uncertainties indicates that although the SRM tracking system has recognizable positioning uncertainties, they do not significantly debilitate the use of deconvolution to accurately restore high-resolution signal. The simulated excursion event associated with a significant magnetization intensity drop was clearly recovered in the deconvolved measurements with a maximum error of similar to 3 degrees in inclination.

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