2024
DOI: 10.1109/tgrs.2023.3340037
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Multiorder Sequential Joint Inversion of Gravity Data With Inhomogeneous Depth Weighting: From Near Surface to Basin Modeling Applications

Luigi Bianco,
Mojtaba Tavakoli,
Andrea Vitale
et al.

Abstract: We have established a workflow for a multi-order sequential joint inversion (MOSJI) of gravity and gravity gradients, that aims at modelling of vertically-stacked sources in various geological scenarios. We consider the joint inversion of the gravity data and one of the h th order derivative of the gravity data. The first step involves separate inversions, which are fundamental to fully exploit the different wavelength-content of the two quantities to invert. The joint inversion is warranted by using the schem… Show more

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Cited by 6 publications
(2 citation statements)
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“…For the magnetic field T, the DEXP transformation is given by where Ω r, z i is the DEXP-scaled field at each altitude z i ; r is the position vector at points in the harmonic region; T r, z i is the upward continued field at power-law of altitudes; q is the order of differentiation of is the structural index, which is a parameter characterizing the type of source (Bianco et al 2024;Fedi 2016), namely, ranging from 0 to 3, for simple sources such as contact, sheet, line and sphere, respectively. When dealing with real sources, this parameter is not constant versus the altitude and assumes fractional values (Bianco et al 2023) and intermediate versus those of the aforementioned sources (Fedi, Florio, and Paoletti 2012).…”
Section: Magnetic Surveymentioning
confidence: 99%
“…For the magnetic field T, the DEXP transformation is given by where Ω r, z i is the DEXP-scaled field at each altitude z i ; r is the position vector at points in the harmonic region; T r, z i is the upward continued field at power-law of altitudes; q is the order of differentiation of is the structural index, which is a parameter characterizing the type of source (Bianco et al 2024;Fedi 2016), namely, ranging from 0 to 3, for simple sources such as contact, sheet, line and sphere, respectively. When dealing with real sources, this parameter is not constant versus the altitude and assumes fractional values (Bianco et al 2023) and intermediate versus those of the aforementioned sources (Fedi, Florio, and Paoletti 2012).…”
Section: Magnetic Surveymentioning
confidence: 99%
“…We will here use a model-weighting function W z , based on the depth weighting function. Such function, originally proposed by [8][9][10] , has its elements at a given depth z in the 3D model defined as: So, the weighting function (Eq. 4) becomes:…”
Section: Source Atomizationmentioning
confidence: 99%