2023
DOI: 10.1029/2023je007796
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Lithospheric Elastic Thickness Beneath the Caloris Basin: Implications for the Thermal Structure of Mercury

Abstract: The basin interior is covered by the Caloris interior plains (CIP) that have been deformed by complex tectonic features (Denevi et al., 2018), including concentric ridges and tensional grabens that exhibit both radial and tangential strikes (Byrne et al., 2018). Both the northern and southern parts of the basin floor have been significantly uplifted to heights that exceed the basin rim (Figure 1c), and the two mountain belts have a trend that is more-or-less parallel to the east-northeast to west-southwest dir… Show more

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Cited by 1 publication
(14 citation statements)
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References 98 publications
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“…Within the circular region delineated by the red dashed lines in the basin, Figures 8b–8d illustrate that a positive load ratio corresponds to a negative transverse density anomaly. This finding is in line with previous studies (Belleguic et al., 2005; Deng, Xiao, et al., 2023; Deng, Zhong, et al., 2023; Zhong et al., 2022). Moreover, the absolute value of the density anomaly gradually increases with the increase in the load ratio, which reduces the initial positive net load from topography plus mantle plug and mare basalt.…”
Section: Methodssupporting
confidence: 93%
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“…Within the circular region delineated by the red dashed lines in the basin, Figures 8b–8d illustrate that a positive load ratio corresponds to a negative transverse density anomaly. This finding is in line with previous studies (Belleguic et al., 2005; Deng, Xiao, et al., 2023; Deng, Zhong, et al., 2023; Zhong et al., 2022). Moreover, the absolute value of the density anomaly gradually increases with the increase in the load ratio, which reduces the initial positive net load from topography plus mantle plug and mare basalt.…”
Section: Methodssupporting
confidence: 93%
“…In this study, we utilize the approach proposed by Deng, Xiao, et al. (2023) and Deng, Zhong, et al. (2023) to quantify the model uncertainties as follows: σ(Te,f)=1lmaxlwin+1l=lwinlmax[]Z(l)Zmodel(l)κz(l)2 $\sigma (Te,f)=\frac{1}{{l}_{\max }-{l}_{\text{win}}+1}{\sum\limits _{l={l}_{\text{win}}}^{{l}_{\max }}\left[\frac{Z(l)-{Z}^{\text{model}}(l)}{\kappa z(l)}\right]}^{2}$ where l max represents the highest degree of fit between gravity and topography.…”
Section: Methodsmentioning
confidence: 99%
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