Peter B. James

Dr. Peter B. James

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Research Focus & Metrics

Academic Career Length

10Years (2017-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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21 June 2021 in Proceedings of the National Academy of Sciences
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PBPaul K. Byrne
Paul K. Byrne
RGRichard Ghail
Richard Ghail
AŞA. M. Celâl Şengör
A. M. Celâl Şengör
PJPeter B. James
Peter B. James
CKChristian Klimczak
Christian Klimczak
SSSean C. Solomon
Sean C. Solomon
Significance: We have identified a pattern of tectonic deformation on Venus that suggests that many of the planet’s lowlands have fragmented into discrete crustal blocks, and that these blocks have moved relative to each other in the geologically recent past. These motions may be the result of mantle convection and, if so, constitute a style of interior–surface coupling not seen elsewhere in the inner Solar System except for continental interiors on Earth. Venus’ fragmented, mobile lithosphere may offer a framework for understanding how tectonics on Earth operated in the Archean.

27 May 2019 in Geophysical Research Letters
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PJPeter B. James
Peter B. James
DSDavid E. Smith
David E. Smith
PBPaul K. Byrne
Paul K. Byrne
JKJordan D. Kendall
Jordan D. Kendall
HMH. Jay Melosh
H. Jay Melosh
MZMaria T. Zuber
Maria T. Zuber
The South Pole‐Aitken basin is a gigantic impact structure on the far side of the Moon, with an inner rim extending approximately 2,000 km in the long axis dimension. The structure and history of this basin are illuminated by gravity and topography data, which constrain the subsurface distribution of mass. These data point to the existence of a large excess of mass in the Moon's mantle under the South Pole‐Aitken basin. This anomaly has a minimum mass of 2.18 × 1018 kg and likely extends to depths of more than 300 km. Plausible sources for this anomaly include metal from the core of a differentiated impactor or oxides from the last stage of magma ocean crystallization. Although the basin‐forming impact event likely excavated the vast majority of the preexisting crust, the present‐day crust of the basin interior is at least 16 km thick in undisturbed regions.

25 March 2017 in Journal of Geophysical Research: Planets
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EFElizabeth A. Frank
Elizabeth A. Frank
RPRoss W. K. Potter
Ross W. K. Potter
OAOleg Abramov
Oleg Abramov
PJPeter B. James
Peter B. James
RKRachel L. Klima
Rachel L. Klima
LNLarry R. Nittler
Larry R. Nittler

30 August 2021 in Geophysical Research Letters
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TWThomas R. Watters
Thomas R. Watters
PJPeter B. James
Peter B. James
MSMichelle M. Selvans
Michelle M. Selvans
The crust of Mercury has experienced contraction on a global scale. Contractional deformation is expressed by a broadly distributed network of lobate thrust fault scarps. The most likely principal source of stress is global contraction from cooling of Mercury's interior. Global contraction alone would be expected to result in a uniformly distributed population of thrust faults. Mercury's fault scarps, however, often occur in long, linear clusters or bands. An analysis of the contractional strain as a function of crustal thickness, estimated in two crustal thickness models (CT1 and CT2) derived from gravity and topography data obtained during the MESSENGER mission, indicates the greatest contractional strain occurs in crust 50–60 km thick. On Earth, mantle downwelling can thicken and compress overlying crust, regionally concentrating thrust faults. Clusters of lobate scarps collocated with regions of thick crust suggest downward mantle flow contributed to the localization of lithosphere‐penetrating thrust faults.

1 June 2022 in The Planetary Science Journal
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SGSander Goossens
Sander Goossens
Antonio GenovaAntonio Genova
Antonio Genova
PJPeter B. James
Peter B. James
EMErwan Mazarico
Erwan Mazarico
We have analyzed the entire set of radiometric tracking data from the MErcury Surface, Space ENvironment, GEochemistry, and Ranging (MESSENGER) mission. This analysis employed a method where standard Doppler tracking data were transformed into line-of-sight accelerations. These accelerations have greater sensitivity to small-scale features than standard Doppler. We estimated a gravity model expressed in spherical harmonics to degree and order 180 and showed that this model is improved, as it has increased correlations with topography in areas where tracking data were collected when the spacecraft altitude was low. The new model was used in an analysis of the localized admittance between gravity and topography to determine properties of Mercury’s lithosphere. Four areas with high correlations between gravity and topography were selected. These areas represent different terrain types: the high-Mg region, the Strindberg crater plus some lobate scarps, heavily cratered terrain, and smooth plains. We employed a Markov Chain Monte Carlo method to estimate crustal density, load density, crustal thickness, elastic thickness, load depth, and a load parameter that describes the ratio between surface and depth loading. We find densities around 2600 kg m−3 for three of the areas, with the density for the fourth area, the northern rise, being higher. The elastic thickness is generally low, between 11 and 30 km.

7 February 2018 in Journal of Geophysical Research: Planets
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MSMichael M. Sori
Michael M. Sori
PJPeter B. James
Peter B. James
BJBrandon C. Johnson
Brandon C. Johnson
JSJason M. Soderblom
Jason M. Soderblom
SSSean C. Solomon
Sean C. Solomon
MZMaria T. Zuber
Maria T. Zuber
The lunar highlands are isostatically compensated at large horizontal scales, but the specific compensation mechanism has been difficult to identify. With topographic data from the Lunar Orbiter Laser Altimeter and gravity data from the Gravity Recovery and Interior Laboratory, we investigate support of highland topography. Poor correlation between crustal density and elevation shows that Pratt compensation is not important in the highlands. Using spectrally weighted admittance, we compared observed values of geoid‐to‐topography ratio (GTR) with those predicted by isostatic models. Observed GTRs are 25.8+7.5–5.7 m/km for the nearside highlands and 39.3+5.7–6.2 m/km for the farside highlands. These values are not consistent with flexural compensation of long‐wavelength topography or Airy isostasy defined under an assumption of equal mass in crustal columns. Instead, the observed GTR values are consistent with models of Airy compensation in which isostasy is defined under a requirement of equal pressures at equipotential surfaces at depth. The gravity and topography data thus reveal that long‐wavelength topography on the Moon is most likely compensated by variations in crustal thickness, implying that highland topography formed early in lunar history before the development of a thick elastic lithosphere.