Ross N. Mitchell’s research while affiliated with State Key Laboratory of Lithospheric Evolution, Chinese Academy of Sciences and other places

What is this page?


This page lists works of an author who doesn't have a ResearchGate profile or hasn't added the works to their profile yet. It is automatically generated from public (personal) data to further our legitimate goal of comprehensive and accurate scientific recordkeeping. If you are this author and want this page removed, please let us know.

Publications (105)


Persistent but weak magnetic field at Moon's midlife revealed by Chang'e-5 basalt
  • Preprint
  • File available

November 2024

·

238 Reads

·

·

·

[...]

·

Rixiang Zhu

The evolution of the lunar magnetic field can reveal the Moon's interior structure, thermal history, and surface environment. The mid-to-late stage evolution of the lunar magnetic field is poorly constrained, and thus the existence of a long-lived lunar dynamo remains controversial. The Chang'e-5 mission returned the heretofore youngest mare basalts from Oceanus Procellarum uniquely positioned at mid-latitude. We recovered weak paleointensities of 2-4 uT from the Chang'e-5 basalt clasts at 2 billion years ago, attestting to the longevity of a lunar dynamo until at least the Moon's midlife. This paleomagnetic result implies the existence of thermal convection in the lunar deep interior at the lunar mid-stage which may have supplied mantle heat flux for the young volcanism.

Download

Viscosity, basal mantle structures, plumes, and slabs in models with different yield stresses at t = 4.56 Gyr
Viscosity at the surface (columns 1 and 4), basal mantle structures (isosurface of the composition with contour level C=0.5\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$C=0.5$$\end{document}, columns 2 and 5), plumes (isosurface of non-dimensional temperature with contour level fp=0.5\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${f}_{{{\rm{p}}}}=0.5$$\end{document}, columns 3 and 6, orange), and slabs (isosurface of non-dimensional temperature with contour level fs=0.1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${f}_{{{\rm{s}}}}=0.1$$\end{document}, columns 3 and 6, blue). Columns 4–6 show the opposite hemisphere of columns 1–3. From row a to row e, the values of yield stress are 30, 50, 70, 100, and 200 MPa with the same buoyancy ratio of 0.26 and chemical viscosity contrast of 10.
CMB area covered by basal mantle structures and the number of basal mantle structures as a function of yield stress at t = 4.56 Gyr
Note that the antipodal two-pile basal mantle structures similar to the LLVSPs occur within a narrow range of medium yield stress (90–100 MPa), and our preferred model (100 MPa) is marked with a star.
1-D profiles of horizontal velocities of basal mantle structures and the ambient mantles for models with different yield stresses at t = 4.56 Gyr
The averaged mantle horizontal velocity profiles of the basal mantle structures (solid lines), and the ambient mantles (dotted lines) with different yield stress: 30 (orange), 90 ~ 100 (purple), and 200 MPa (green). Gray shadow marks the standard deviation for statistics of 90, 95, and 100 MPa cases. Note that the global average velocity of modern plates is ~ 5 cm yr⁻¹ (ref. ⁴⁹).
Thermal convection model with yield stress of 100 MPa at t = 4.56 Gyr
a Viscosity at the surface (top row), plumes, and slabs (bottom row). The right column shows the opposite hemisphere of the left column. The plumes and slabs are defined by setting fp\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${f}_{{{\rm{p}}}}$$\end{document} = 0.5 and fs\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${f}_{{{\rm{s}}}}$$\end{document} = 0.1, respectively. b Horizontal velocities of plumes and bulk mantle (only the horizontal velocity of thermal plumes in the lower mantle is plotted).
Vote maps of BMSs and plumes for the thermo-chemical model and plumes for the thermal model with yield stress of 100 MPa in the last 630 Myrs
a Vote maps of BMSs at 2800 km depth and plumes at 300 km depth for the thermo-chemical convection model with a yield stress of 100 MPa in the last 630 Myrs (columns 1 and 2) and vote maps of plumes at 2800 km depth and 300 km depth for the thermal convection model with a yield stress of 100 MPa in the last 630 Myrs (columns 3 and 4). Row 2 shows the views of the opposite hemisphere of Row 1. b The distribution histograms of vote maps of BMSs and plumes for the thermochemical model and plumes for the thermal model.
Sluggish thermochemical basal mantle structures support their long-lived stability

November 2024

·

262 Reads

·

1 Citation

Large low shear-wave velocity provinces (LLSVPs) in the lowermost mantle are the largest geological structures on Earth, but their origin and age remain highly enigmatic. Geological constraints suggest the stability of the LLSVPs since at least 200 million years ago. Here, we conduct numerical modeling of mantle convection with plate-like behavior that yields a Pacific-like girdle of mantle downwelling which successfully forms two antipodal basal mantle structures similar to the LLSVPs. Our parameterized results optimized to reflect LLSVP features exhibit velocities for the basal mantle structures that are ~ 4 times slower than the ambient mantle if they are thermochemical, while the velocity is similar to the ambient mantle if purely thermal. The sluggish motion of the thermochemical basal mantle structures in our models permits the notion that geological data from hundreds of millions of years ago are related to modern LLSVPs as they are essentially stationary over such time scales.


Conformably Variable Geocentric Axial Dipole at ca. 2.1 Ga: Paleomagnetic Dispersion of the Indin Dyke Swarm, Slave Craton

November 2024

·

103 Reads

Precambrian paleomagnetic studies are critical for testing paleogeographic reconstructions in deep time but rely on the fidelity of the assumption of the geocentric axial dipole (GAD) hypothesis. With high‐reliability data from mafic dykes and volcanic rocks, the scatter of individual virtual geomagnetic poles (VGPs) can be used to test simple GAD models. In order to conduct such a test, the VGPs must be adequate in number and in spatial coverage of the sampling sites. In this study, we targeted the 2.1 Ga Indin dyke swarm of the Slave craton. Building on previous sampling of the Indin dyke swarm in the western and central parts of southern Slave craton, we report results from 9 additional sites in the central and eastern parts of the craton, sites that significantly expand the width of the dyke swarm across the entire craton. The VGPs obtained from 7 of 9 newly identified Indin dykes are broadly similar to previously reported directions, expanding the total of VGPs for individual Indin dykes to n = 28, which is sufficient for a test of the GAD‐based statistical models using VGP scatter. The high VGP scatter of the Indin swarm can be attributed to the relatively high paleolatitude of 56° ± 6° for the Slave craton at the time of dyke emplacement. The Indin data have VGP scatter that is consistent with field models associated with the GAD hypothesis for the indicated paleolatitude, thus confirming the fidelity of the GAD field at ca. 2.1 Ga.


Backscattered electron images of the CE-5 basalt fragments
In the early stage of crystallization, olivine has high Mg# and the coexisting spinel has low Ti# (a, b). As the crystallization process continues, Mg# in olivine decreases while Ti# in spinel increases (b, c). In the late stage of crystallization, olivine has low Mg# and the coexisting spinel has high Ti# (d). Mg#= [atomic Mg/ (Mg + Fe)]; Ti#= [atomic Ti/ (Ti + Cr)]. Abbreviations: Cpx, clinopyroxene; Ilm, ilmenite; Pl, plagioclase; Ol, olivine; Spl, Spinel; Tro, troilite.
Oxygen fugacity of the lunar mantle from CE-5 basalts compared with Earth and Mars
a The fO2 estimates of the CE-5 basalt fragments derived from V oxybarometers. The grey bar represents the average fO2 of the original melt of the CE-5 basalt. The gray lines indicate the trend of increased fO2 during late-stage crystallization of the CE-5 basalt when Mg#equilibrium melt ≤ 20. b The mantle fO2 of the Moon, Mars, and Earth. The fO2 data for the Apollo samples are from refs. 18,19; the fO2 data for Mars are from refs. 5,65,67–69; the fO2 data for Earth are from refs. 3,70,71. The average fO2 (ΔIW-1.0 ± 0.9) of the lunar mantle was calculated based on the CE-5 basalt (ΔIW -0.84 ± 0.65) and the Apollo samples18,19; the average fO2 of the mantles of Earth and Mars are from refs. 5,33, respectively, noting that shergottite is considered the most accurate approximation for bulk silicate Mars, and others are excluded from the average calculation (Methods); The grey bars represent the average fO2 of the mantles of Earth, Mars and Moon. The error bar represents 2 standard deviations for each point. Abbreviations: CE-5, Chang’e-5; Ol, olivine; Spl, spinel; VLT, very low Ti. Source data are provided as a Source Data file.
Redox evolution of terrestrial mantles
a The temporal evolution of mantle fO2 for the Moon, Mars, and Earth. The fO2 data for the Earth’s mantle are from mid-ocean ridge basalts and ultramafic lavas1,2. The fO2 data for the Martian mantle are from shergottites⁵. The fO2 data for the lunar mantle are from the Apollo basalts and pyroclastic glasses18,19. The age data are from refs. 1,2,5,72,73. The red star represents the original average fO2 values of Earth, Mars, and the Moon derived from refs. 33,34. The error bar represents 2 standard deviations for each point. b Mechanism diagrams by terrestrial body. The late accretion mass of Earth, Mars, and Moon are from ref. ³⁸. The late accretion mass ratio represents the ratio of late accretion mass to the body mass. Abbreviations: CE-5, Chang’e-5; Ga, Giga annum; GPa, Giga Pascal. Source data are provided as a Source Data file.
Implications for secular mantle cooling from oxygen fugacity estimate
The mantle potential temperature (Tp) of the lunar mantle over time according to different fO2. The average bulk compositions of low-Ti lunar basalts, meteorites, and CE-5 basalts are from refs. 26,62,63, and their ages are from refs. 1,2,5,72,73. Tp values are calculated based on ref. ³¹. The error bars are calculated from the uncertainties in the lunar mantle potential temperature (Tp). CE-5, Chang’e-5; Ga, Giga annum. Source data are provided as a Source Data file.
Long-term reduced lunar mantle revealed by Chang’e-5 basalt

September 2024

·

282 Reads

The redox state of a planetary mantle affects its thermal evolution. The redox evolution of lunar mantle, however, remains unclear due to limited oxygen fugacity (fO2) constraints from young lunar samples. Here, we report vanadium (V) oxybarometers on olivine and spinel conducted on 27 Chang’e-5 basalt fragments from 2.0 billion years ago. These fragments yield an average fO2 of ΔIW -0.84 ± 0.65 (2σ), which closely aligns with the Apollo samples from 3.6–3.0 billion years ago. This temporal uniformity indicates the lunar mantle remained reduced. This observation reveals that the processes responsible for oxidizing mantles of Earth and Mars either did not occur or had negligible oxidizing effects on the Moon. The long-term reduced mantle may lead to a distinctive volatile degassing pathway for the Moon. It could also make the lunar mantle more difficult to melt, preventing internal heat dissipation and consequently resulting in a slow cooling rate.


Evidence of a large igneous province at ca. 347–330 Ma along the northern Gondwana margin linked to the assembly of Pangea: Insights from Usingle bondPb zircon geochronology and geochemistry of the South-Western Branch of the Variscan Belt (Morocco)

August 2024

·

424 Reads

Earth-Science Reviews

The migration and composition of magmatism over time can provide important insights into the tectonic evolution of an orogen like the Variscan Belt. To identify Large Igneous Provinces (LIPs), key criteria include large magmatic volume, intraplate-origin volcanic geochemistry, and significant plumbing systems. Based on such criteria, we present evidence of ca. 347–330 Ma LIP “fragments” in the South-Western Branch of the Variscan Belt (Morocco), exemplified by the Variscan Central Jebilet Massif. The interpretations are based on four new zircon Usingle bondPb ages obtained by sensitive high-resolution ion microprobe (SHRIMP), a geochemical database of Carboniferous mafic sills, dykes, and gabbroic intrusions together, with subordinate layered ultramafic intrusions, silicic intrusive and volcanic rocks of Central Jebilet Massif, combined with previously published and unpublished data including Srsingle bondNd isotope analyses. Geochemistry data indicate that the early Carboniferous magmatism of the Jebilet Massif is plume-related. Furthermore, primary magmas of the mafic rocks were generated in an intraplate setting and derived by partial melting of complex sources involving asthenosphere, lithospheric mantle, and subducting slab components (Rheic dead slabs), and were modified by crustal contamination during ascent. Magmatic rocks in the same stratigraphic position also occur in other Carboniferous basins including Western Meseta (Rehamna and Moroccan Central Massif). The newly obtained and compiled zircon Usingle bondPb ages from Western Meseta rocks, encompassing an area of ~400,000 km2, indicate that magmatism occurred between ca. 347–330 Ma, coeval with volcanic activity in the Eastern Meseta in northeastern Morocco. The similar emplacement ages, in combination with the tectonic reconstruction of northwestern Gondwana at ca. 330 Ma, suggest that the igneous subprovinces of the Jebilet, Rehamna, and Moroccan Central Massif in Western Meseta, along with Tazekka, Debdou, and Mekkam in Eastern Meseta, the igneous rocks of the Maritimes (Magdalen) Basin, the St. Jean du Doigt bimodal layered intrusion (Brittany, France), and other equivalents such as the Iberian Pyrite Belt and the Southern Vosges magmatism, may represent the eroded and/or deformed remnants of a Large Igneous Province (LIP), which we name here the North Gondwana–Avalonia LIP. We argue that this newly identified LIP was formed by a mantle plume that may have played a role in the breakup along the northwestern margin of the precursor megacontinent Gondwana and the assembly of Pangea. The plume was likely centered under the thick lithosphere of Avalonia. The large-scale sublithospheric plume-flow channeling from the plume head led to the development of widespread tholeiitic/alkaline magmatism in the thinned lithosphere of Western Meseta, interpreted here as a large thin-spot domain, and calc-alkaline/alkaline magmatism in the thickened lithosphere of the Eastern Meseta. The mantle plume may have been most active during the periods of ca. 390–330 Ma (Maritimes Event), ca. 370–338 Ma (Iberia Event), ca. 347–330 Ma (Meseta Event), and the multipulsed ca. 300 Ma, 290–275 Ma, and 250 Ma European North West African Magmatic Province (EUNWA or EUNWAMP), which were the periods when most of the Variscan mafic rocks were produced in these areas.


A Model for Melt‐Preferred Orientation and Permeabilities in Deformed Partially Molten Peridotites

August 2024

·

111 Reads

In a deforming partially molten rock, melt concentrates into a grain‐scale melt pocket aligned at a preferred orientation (melt‐preferred orientation, or MPO). However, observing this texture alone provides limited information on the 3D orientation and geometry of these melt pockets, which are critical parameters for estimating permeability. Here, we modeled the MPO of experimentally deformed peridotites by simulating melt streaks arising from melt pockets of various shapes and 3D orientations. The model aims to identify 3D distribution and characteristics of melt pockets that could account for the observed length, thickness, and the probability of melt streaks. Results show that melt pockets at preferred orientation exhibit greater length, thickness, and number density compared to those perpendicular. These results can be incorporated into the simulation of melt flow through individual melt pockets, which allows us to estimate the permeability corresponding to the observed MPO. We found that the permeability of vertically compressed peridotites increases with increasing compressive strain and a more elongated and thickened shape for melt pocket aligned at preferred orientation. The vertical permeability in the sample with 30% compressive strain is at least 40 times larger than that of an undeformed sample. For peridotites deformed under simple shear, the permeability exhibits an anisotropy of at least three. Such anisotropic permeability, coupled with the formation of melt‐rich bands and other melt channels, is believed to cause lateral melt focusing beneath mid‐ocean ridges.


Geological map of North China Craton and the area studied
a Map showing outcrops of Archaean–Paleoproterozoic basement and reported pre-Neoarchaean rocks in North China Craton (modified from Wan et al. ¹); b Geological map from Anshan to Jiapigou (modified from Guo et al. ²).
Zircon U–Pb dating and Hf–O isotopes
a Zircon concordia diagram and kernel density estimate plot for Palaeoarchaean–Neoarchaean granitoids. b Representative zircon CL images of the c. 3.3 Ga monzogranite sample 22BS20-3. c Compilation of zircon epsilon hafnium (εHf(t)) values of Eoarchaean-to-Mesoarchaean TTGs from other ancient cratons versus ²⁰⁷Pb/²⁰⁶Pb age. d Compilation of zircon εHf(t) values from the North China Craton versus ²⁰⁷Pb/²⁰⁶Pb age. e Diagram of initial ¹⁷⁶Hf/¹⁷⁷Hf value versus ²⁰⁷Pb/²⁰⁶Pb age. f Compilation of zircon δ¹⁸O values versus ²⁰⁷Pb/²⁰⁶Pb age. Note only analyses showing no significant Pb loss are plotted. Depleted mantle lines are based on models of a present depleted mantle with a ¹⁷⁶Hf/¹⁷⁷Hf of 0.283251 and a ¹⁷⁶Lu/¹⁷⁷Hf of 0.0384 (ref. ⁶⁸), and the 3.8 Ga Depleted mantle curve is extrapolated from the assumption that growth of the depleted mantle began at 3.8 Ga (εHf = 0) and evolved to the present-day depleted mantle reservoir¹⁴. The δ¹⁸O value range for “mantle zircon” is from ref. ⁵⁵.
Geochemical diagrams of the 3.3–2.5 Ga granitoids of the Baishanhu nucleus
a Primitive mantle-normalised multi-element diagram, where normalised primitive mantle values are from Sun and McDonough⁶⁹. b Al2O3/(FeOT + MgO)–3*CaO–5*(K2O/Na2O) ternary diagram²⁵. c Sr/Y versus Y diagram. Dashed lines represent basalt partial melting curves leaving either 10% garnet amphibolite or eclogite restite assemblages²⁶. d MgO versus SiO2 diagram for adakite²⁸.
Archaean crustal architecture of the north Liaoning–south Jilin region, North China Craton
Contour maps of zircon U–Pb age (a), zircon Hf TDM age (b), and zircon εHf(t) value (c), constructed following ref. ⁷⁰.
Tectono-magmatic model of the Eoarchaean to early Neoarchaean evolution of the North China Craton
a Mafic magma underplating during 3.8–3.6 Ga resulted in partial melting of a pre-existing 4.2–3.8 Ga mafic protocrust to generate 3.8–3.6 Ga TTG and form the earliest coherent continental nucleus in the North China Craton. b Another mafic magma underplating event during 3.3–2.9 Ga led to the reworking of previously formed 3.8–3.6 Ga felsic crust. As a result, abundant 3.3–2.9 Ga potassium-rich granites formed in the Anshan and Baishanhu nuclei. c The 2.8–2.6 Ga magma underplating event led to the reworking of 3.8–3.6 Ga ancient felsic crust and 3.2–2.9 Ga juvenile mafic crust, which resulted in the formation of 2.72 Ga potassium-rich granite in the Baishanhu nucleus and c. 2.7 Ga TTG in the North Liaoning to South Jilin granite-greenstone belt, respectively. The green layers in the models represent mafic crusts formed during different stages.
Archaean multi-stage magmatic underplating drove formation of continental nuclei in the North China Craton

July 2024

·

479 Reads

·

2 Citations

The geodynamic processes that formed Earth’s earliest continents are intensely debated. Particularly, the transformation from ancient crustal nuclei into mature Archaean cratons is unclear, primarily owing to the paucity of well-preserved Eoarchaean–Palaeoarchaean ‘protocrust’. Here, we report a newly identified Palaeoarchaean continental fragment—the Baishanhu nucleus—in northeastern North China Craton. U–Pb geochronology shows that this nucleus preserves five major magmatic events during 3.6–2.5 Ga. Geochemistry and zircon Lu–Hf isotopes reveal ancient 4.2–3.8 Ga mantle extraction ages, as well as later intraplate crustal reworking. Crustal architecture and zircon Hf–O isotopes indicate that proto-North China first formed in a stagnant/squishy lid geodynamic regime characterised by plume-related magmatic underplating. Such cratonic growth and maturation were prerequisites for the emergence of plate tectonics. Finally, these data suggest that North China was part of the Sclavia supercraton and that the Archaean onset of subduction occurred asynchronously worldwide.


Fig. 1. Traditional discriminant diagram of non-S-type (including TTG) and S-type zircon. (A) Diagram showing the boundary of I-(TTG) and S-type zircon and the trace element distribution of detrital, I-(TTG) and S-type zircon. Green shadow, upper line and lower line show the "traditional S-type region" and related I/S boundary (20), that zircon with P > 15 (μmol/g) and 0.77*P < (REE+Y) < 1.23*P is S-type zircon, and otherwise is non-S-type zircon. The inset shows the cumulative frequency of all Hadean-Archean detrital zircon. (B) P contents of detrital zircon and I-and S-type zircon used in this study (Dataset S1). The Inset shows P-content time series for igneous and sedimentary rocks from (33, 34) as bootstrapped averages in 10-million-year bins.
Fig. 2. Trace element fingerprints of zircon. These bars show the composition and availability of the top 30 most common trace elements in the zircon dataset (SI Appendix, Table S1) and a detrital zircon dataset from ref. 22 (Dataset S2). Box-and-whiskers plot shows the maximum, 3rd quartile, median, 1st quartile, and minimum values. The highest and lowest 20% of values of each element are excluded to reduce scatter. Trace element availability is calculated by n/N, where n is the available trace element data and N is the size of the dataset. Those elements used as input features for machine learning are indicated with stars.
Fig. 3. Comparison of the machine-learning method (TSVM model) and the traditional P criterion in recognizing S-type zircon. (A) The accuracy of both methods for non-S-and S-type zircon with different P contents in the dataset. The distribution of P contents for non-S-and S-type zircon are shown in the red and blue histograms, respectively. The accuracy of each model in our dataset (both training and test sets) is calculated using a bin size of 5 μmol/g (Dataset S2). (B) Clear-cut discrimination of non-S-and S-type zircon by TSVM value = 0, where TSVM values mean the prediction output value of TSVM (defined in Materials and Methods). Blue open circles are S-type zircon, red open circles are non-S-type zircon, and orange filled circles are detrital zircon with Hadean to Archean ages. TSVM value is calculated based on the decision function of the machine-learning model (Materials and Methods), TSVM value = (5.66) * P + (0.54) * Y + (-1.66) * Ce+ (0.49) * Sm+ (-1.47) * Eu+ (-0.69) * Dy+ (-3.90) * Lu+ (0.42) * Th+ (0.58) * U, where >0 means S-type zircon and <0 indicates non-S-type zircon.
Fig. 4. S-type detrital zircon on early Earth and the evolution of magma sources. (A) Hf isotopes of the Jack Hills zircon (9, 62, 63). The isotope trajectories of the putative depleted mantle (64), mafic crust (65), and upper continental crust (UCC) (66) are shown for reference, assuming silicate Earth differentiation at 4.5 Ga. Arrows mark the trend of prolonged internal crustal recycling of Hadean to Eoarchean crust and the transition at 3.8 to 3.7 Ga toward increasing juvenile contributions to magma sources. (B) Detrended Hf isotope of Hadean-Archean detrital zircon (67). (C) Bootstrapped average of S-type zircon proportion through time with 1 SE (SI Appendix, Table S4) and crustal recycling rate (68). (D) Stacked histogram of the distribution of I-and S-type zircon through time as classified by machine learning, including detrital zircon from the Jack Hills, Australia, and 12 other locations. The Inset shows δ 18 O step-change of Jack Hills zircon (61) and a histogram of zircon older than 4.0 Ga. The dashed line shows the probability density plot of detrital zircon along the traverse through the Jack Hills belt (69). See SI Appendix, Table S3, for the individual distributions of S-type zircon in each of the 12 locations studied. All the zircon presented have U-Pb ages that are <10% discordant.
Sediment subduction in Hadean revealed by machine learning

July 2024

·

607 Reads

·

2 Citations

Proceedings of the National Academy of Sciences

Due to the scarcity of rock samples, the Hadean Era predating 4 billion years ago (Ga) poses challenges in understanding geological processes like subaerial weathering and plate tectonics that are critical for the evolution of life. The Jack Hills zircon from Western Australia, the primary Hadean samples available, offer valuable insights into magma sources and tectonic genesis through trace element signatures. However, a consensus on these signatures has not been reached. To address this, we developed a machine learning classifier capable of deciphering the geochemical fingerprints of zircon. This allowed us to identify the oldest detrital zircon originating from sedimentary-derived “S-type” granites. Our results indicate the presence of S-type granites as early as 4.24 Ga, persisting throughout the Hadean into the Archean. Examining global detrital zircon across Earth’s history reveals consistent supercontinent-like cycles from the present back to the Hadean. These findings suggest that a significant amount of Hadean continental crust was exposed, weathered into sediments, and incorporated into the magma sources of Jack Hills zircon. Only the early operation of both subaerial weathering and plate subduction can account for the prevalence of S-type granites we observe. Additionally, the periodic evolution of S-type granite proportions implies that subduction-driven tectonic cycles were active during the Hadean, at least around 4.2 Ga. The evidence thus points toward an early Earth resembling the modern Earth in terms of active tectonics and habitable surface conditions. This suggests the potential for life to originate in environments like warm ponds rather than extreme hydrothermal settings.



The assembly of Pangea: geodynamic conundrums revisited

June 2024

·

188 Reads

Journal of the Geological Society

Geodynamic models for Pangea assembly require knowledge of Paleozoic mantle convection patterns. Application of basic geodynamic principles to Neoproterozoic–Paleozoic plate reconstructions yields Pangea in the incorrect configuration (predicting that Pangea should have formed by consumption of the exterior paleo-Pacific Ocean instead of Iapetus, Rheic, and Proto-Tethys oceans). We contend that the mantle legacy of Late Neoproterozoic–Cambrian amalgamation of Gondwana must be factored into models for Pangea amalgamation. Proxy data suggest that the mantle downwelling driving Pan-African collisions and Gondwana assembly evolved into a mantle upwelling as evidenced by the interplay between subduction-related and plume-related tectonics around the periphery of Gondwana. Orthoversion theory, whereby a supercontinent assembles ∼90° away from the centre of the previous supercontinent, suggests that Gondwana amalgamated above an intense downwelling along a meridional subduction girdle that bisected two antipodal sub-equatorial upwellings. Several processes beneath and around Gondwana reduced the intensity of the original downwelling, as evidenced by plume-related activity along its margins, initiation of subduction zone roll-back, and the export of terranes from Gondwana that collided with the margin of Laurentia–Baltica. As upwelling beneath it intensified, Gondwana migrated along the girdle until it collided with Laurentia–Baltica, resulting in the final assembly of Pangea.


Citations (64)


... Stationary LLSVPs have been hypothesized to result in fixed surface hotspots (Torsvik et al., 2010), but the proposal has also been vigorously debated (Bodur & Flament, 2023;M. Li & Zhong, 2017;Shi et al., 2024). In our models, uprising plumes are mainly detached from LLSVP ridges instead of bottom margins, and plumes are also subject to lateral migration before reaching the surface (Figure 3). ...

Reference:

The Evolution of Dense ULVZs Originating Outside LLSVPs and Implications for Dynamics at LLSVP Margins
Sluggish thermochemical basal mantle structures support their long-lived stability

... The North China Craton (NCC) preserves ancient rocks dating back to ca. 3.8 Ga, and has witnessed multiple magmatic-metamorphic events during the Archean-Proterozoic era [1][2][3]. This critical period may have marked the transformation of the geodynamic regime on early Earth. ...

Archaean multi-stage magmatic underplating drove formation of continental nuclei in the North China Craton

... A TPW oscillation on Earth occurs when there are two sequential back-and-forth TPW shifts, possibly caused by inversion of the geoid kernel as a mass anomaly moves through the lower mantle (Greff-Lefftz & Besse, 2014). Large-scale TPW leads to a redistribution of solar radiation on the Earth's surface, resulting in rapid environmental and biodiversity changes, and even mass extinctions (Hou et al., 2024;Jing et al., 2022;Mitchell et al., 2021;Muttoni & Kent, 2016;Yi et al., 2019). Therefore, TPW plays a crucial role in linking the geodynamic processes between the Earth's interior and surface (Evans, 2003;Gold, 1955). ...

Completing the loop of the Late Jurassic–Early Cretaceous true polar wander event

... In addition, the foreland is a regional sink for subsurface groundwater flow from the northern Qilian Shan thrust belt and northern Plateau margin. The steep north-directed hydraulic gradient along the plateau margin and oblique overthrusting of the plateau crust over the Tarim-Dunhuang Block to the north (e.g., Wu et al., 2024) ensure continuous fluid ingress into the active fault zones of the northern Tibetan foreland such as the NJFS and SWSF (e.g., L. Zhang et al., 2015). Magnetotelluric survey data strongly suggest that these fault systems ultimately root and shallow to the south into the ATF as part of a regional half-flower structure (D. ...

Underthrusting of Tarim Lower Crust Beneath the Tibetan Plateau Revealed by Receiver Function Imaging

... Therefore, although other possibilities may also exist, the carbon isotope compositions in the Wumishan Formation are more likely due to the intense remineralization of the DOC reservoir from increased oxygen (cf. Guo et al., 2013;Mitchell et al., 2023). In a redox-stratified ocean, respiration processes in surface waters can lead to a significant accumulation of the DOC reservoir in anoxic deep-ocean environments, even exceeding the magnitude of the DIC reservoir (Rothman et al., 2003). ...

Carbonate�Corganic decoupling during the first Neoproterozoic carbon isotope excursion
  • Citing Article
  • January 2023

The Innovation Geoscience

... In-situ ground-penetrating radar (GPR) was introduced in planetary science in 2013 as part of the scientific payloads of Yutu-1 the Lunar rover of the Chinese Chang'E-3 mission [1]. Since then, GPR was part of the scientific payloads of the Yutu-2 rover from the Chang'E-4 mission [2], the lander of the Chang'E-5 [3] and Chang'E-6 missions, the rover Perseverance [4] from Mars 2020, and Zhurong rover from Tianwen-1 mission [5]. Moreover, GPR is planned to be used in the future missions Chang'E-7 [6] and ExoMars [7], both missions expected to take place before 2030. ...

Buried palaeo-polygonal terrain detected underneath Utopia Planitia on Mars by the Zhurong radar

Nature Astronomy

... In North China there was a long-term drying trend from the early to late Permian (Wang et al., 2022b;Song et al., 2023). Coals with a relatively low ash and sulfur content occur from the lower Permian Taiyuan, Shanxi formations repetitively (Ge et al., 1985;Cheng et al., 1990;Tang et al., 2013). ...

Andean-type orogenic plateau as a trigger for aridification in the arcs of northeast Pangaea

... At Acasta, there is a steepening of whole-rock REE patterns through time (23), which is reproduced in our AGC samples ( Fig. 1A and Dataset S1). Titanium isotope compositions of orthogneisses in the AGC record a similar temporal evolution in melt regime, with a transition from exclusively intraplate tholeiitic compositions to the appearance of hydrated calc-alkaline-like magmatism at 3.8 Ga (46), contemporaneous with whole-rock, quartz, and zircon Si-O isotope evidence for the Eoarchean appearance of surface silicon recycling (47). In comparison, felsic gneisses from Saglek do not display a systematic relationship between age and wholerock chemistry, with evidence of deep-seated melting in the presence of residual garnet apparent as early as 3.9 Ga, followed by REE patterns reflective of variable melting depths thereafter (ref. ...

No evidence of supracrustal recycling in Si-O isotopes of Earth's oldest rocks 4 Ga ago

Science Advances

... TPW is when a planet 'tips over' to keep most of its mass anomalies on the equator, much like your arms are drawn out when you spin yourself. There is ample evidence for TPW during Ediacaran and early Cambrian times [9,11,12], as all major continental fragments show large, great-circle arcs in the location of their ancient rotational axes determined through paleomagnetic studies. In fact, by moving the bits of Gondwana around on a sphere until these arcs line up, one can recreate the well-known Ediacaran-Cambrian assembly of Gondwana [9]. ...

True polar wander in the Earth system

Science China Earth Sciences

... The thermal history of the basalt clasts in this study is somewhat different from those regolith breccias. The cooling timescale of the Chang'e-5 lava flows was estimated to within a range from days to hundreds of days according to diffusion modeling results of the olivine crystals in the returned basalt clasts (74), which excludes the possibility that basalt clasts in this study record a transient impact field when they cooled down after eruption. After the lava flows erupted and sat on the lunar surface, they might have experienced a certain extent of impacts, which produced the regolith soils and basalt clasts. ...

Surges in volcanic activity on the Moon about two billion years ago