2022
DOI: 10.1190/geo2021-0626.1
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3D controlled-source electromagnetic inversion in the radio-frequency band

Abstract: The classical radio-magnetotelluric (RMT) method is nowadays routinely applied to various environmental, engineering, and exploration problems. The technique uses radio transmitters broadcasting in the frequency range of 10 kHz to 1 MHz, and the measurements are carried out in the far field. The well-known disadvantages of RMT are a lack of robust radio transmitters in remote areas; the absence of transmitters broadcasting below 10 kHz, which limits the penetration depth; and a possible low signal-to-noise rat… Show more

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Cited by 5 publications
(8 citation statements)
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“…Nevertheless, this is not valid for near-field and transition zones (Smirnova et al, 2023). In an ideal condition where signals are being received orthogonal, E-and B-polarizations are completely independent and only E-polarization or TE mode contains tipper information.…”
Section: Transfer Function Calculationsmentioning
confidence: 99%
See 1 more Smart Citation
“…Nevertheless, this is not valid for near-field and transition zones (Smirnova et al, 2023). In an ideal condition where signals are being received orthogonal, E-and B-polarizations are completely independent and only E-polarization or TE mode contains tipper information.…”
Section: Transfer Function Calculationsmentioning
confidence: 99%
“…The following study focuses only on far-field zone results. The results for transition zone are available in Smirnova et al (2023).…”
Section: Introductionmentioning
confidence: 99%
“…Moreover, the convergence behaviour of normalized EM field component inversion can be severely impaired if a heterogeneous sensitivity distribution is generated by a single distant source setup (Bretaudeau & Coppo, 2016) that is a combination of two transmitter aerials employed to provide two independent source polarizations. When inverting transfer functions (TF) in the form of CSEM impedance tensors and vertical magnetic transfer functions (e.g., Bretaudeau & Coppo, 2016; Smirnova et al., 2023), also known as tensor controlled‐source audio‐magnetotellurics (CSAMT) (Zonge & Hughes, 1991), the source currents do not need to be known as they cancel out in this formulation of the CSEM data. This may reduce the footprint of the source in the resistivity models (Bretaudeau & Coppo, 2016).…”
Section: Introductionmentioning
confidence: 99%
“…This may reduce the footprint of the source in the resistivity models (Bretaudeau & Coppo, 2016). However, it is suspected that resolution properties of transfer function data are worse compared to using field components (Sasaki et al., 2015; Smirnova et al., 2023).…”
Section: Introductionmentioning
confidence: 99%
“…Along with the soundings in the far-field zone, the techniques and software tools were elaborated to use the HED source in the transition zone. Examples of the bimodal inversion of field data using the tensor variant of the CSRMT method in the transition zone have been reported in articles [19,24].…”
mentioning
confidence: 99%