In the absence of global plate tectonics, mantle convection and plume-lithosphere interaction are the main drivers of surface deformation on Venus. Among documented tectonic structures, circular volcano-tectonic features known as coronae may be the clearest surface manifestations of mantle plumes and hold clues to the global Venusian tectonic regime. Yet, the exact processes underlying coronae formation and the reasons for their diverse morphologies remain controversial. Here, we use 3D thermomechanical numerical simulations of impingement of a thermal mantle plume upon the Venusian lithosphere to assess the origin and diversity of large Venusian coronae. The ability of the mantle plume to penetrate into the Venusian lithosphere results in four main outcomes: lithospheric dripping, short-lived subduction, embedded plume and plume underplating. During the first three scenarios, plume penetration and spreading induce crustal thickness variations that eventually lead to a final topographic isostasy-driven topographic inversion from circular trenches surrounding elevated interiors to raised rims surrounding inner depressions, as observed on many Venusian coronae. Different corona structures may represent not only different styles of plume-lithosphere

Extensional detachment faults, which have been widely documented in slow-spreading and ultraslow-spreading ridges on Earth, can effectively localize deformation due to their weakness. After the onset of oceanic closure, these weak oceanic detachments may directly control the nucleation of a subduction zone parallel to the former mid-ocean ridge, as is suggested for the Neotethys in Middle Jurassic times. So far, this hypothesis has only been tested by 2D numerical models, whereas the geometry of detachment faults is intrinsically three-dimensional. Here, we conducted a series of 3D numerical thermomechanical experiments in order to investigate the formation of detachment faults in slow oceanic spreading systems and their subsequent response upon inversion from oceanic spreading to convergence.Numerical results show that during the oceanic spreading stage, the formation of detachment faults strongly depends on the magnitude of the healing rate of faulted rocks in the oceanic lithosphere, that reflects the stability of hydrated minerals along fractured rocks. The detachment faults formed in our 3D numerical models deviate from the "rolling hinge model" of oceanic detachment faulting where fault footwalls are rotated and oceanic core complexes are thereby formed. Our results accentuate that the controlling physical parameters for the development of oceanic core complexes and detachment faults can differ, and that their coupled development in nature remains a key target for future research.Upon modelled transition to compression, previously formed asymmetric spreading patterns are prone to asymmetric inversion, where one oceanic plate thrusts under the other. Our results suggest that detachment faults accommodate significant amounts of shortening during the initiation of oceanic closure, but, in contrast to the previously proposed simple conceptual model, no direct inversion of a single detachment fault into an incipient subduction zone is observed. Instead, a widespread interaction of multiple detachment faults occurs after the onset of convergence. Ultimately, the nascent subduction zone

Highlights• Heterogeneity preservation in Earth's mantle depends on rheological contrasts • High bulk moduli promote neutral buoyancy of primordial domains in the lower mantle • Several styles of mantle convection and heterogeneity may occur in rocky planets • Some of these styles can reconcile ancient rock preservation in a convecting mantle

The dynamics and evolution of Venus’ mantle are of first-order relevance for the origin and modification of the tectonic and volcanic structures we observe on Venus today. Solid-state convection in the mantle induces stresses into the lithosphere and crust that drive deformation leading to tectonic signatures. Thermal coupling of the mantle with the atmosphere and the core leads to a distinct structure with substantial lateral heterogeneity, thermally and compositionally. These processes ultimately shape Venus’ tectonic regime and provide the framework to interpret surface observations made on Venus, such as gravity and topography. Tectonic and convective processes are continuously changing through geological time, largely driven by the long-term thermal and compositional evolution of Venus’ mantle. To date, no consensus has been reached on the geodynamic regime Venus’ mantle is presently in, mostly because observational data remains fragmentary. In contrast to Earth, Venus’ mantle does not support the existence of continuous plate tectonics on its surface. However, the planet’s surface signature substantially deviates from those of tectonically largely inactive bodies, such as Mars, Mercury, or the Moon. This work reviews the current state of knowledge of Venus’ mantle dynamics and evolution through time, focussing on a dynamic system perspective. Available observations to constrain the deep interior are evaluated and their insufficiency to pin down Venus’ evolutionary path is emphasised. Future missions will likely revive the discussion of these open issues and boost our current understanding by filling current data gaps; some promising avenues are discussed in this chapter.

Abstract. The nature of compositional heterogeneity in Earth's lower mantle remains a long-standing puzzle that can inform about the long-term thermochemical evolution and dynamics of our planet. Here, we use global-scale 2D models of thermochemical mantle convection to investigate the coupled evolution and mixing of (intrinsically dense) recycled and (intrinsically strong) primordial heterogeneity in the mantle. We explore the effects of ancient compositional layering of the mantle, as motivated by magma ocean solidification studies, and of the physical parameters of primordial material. Depending on these physical parameters, our models predict various regimes of mantle evolution and heterogeneity preservation over 4.5 Gyr. Over a wide parameter range, primordial and recycled heterogeneity are predicted to co-exist with each other in the lower mantle of Earth-like planets. Primordial material usually survives as medium- to large-scale blobs (or streaks) in the mid-mantle, around 1000–2000 km depth, and this preservation is largely independent of the initial primordial-material volume. In turn, recycled oceanic crust (ROC) persists as large piles at the base of the mantle and as small streaks everywhere else. In models with an additional dense FeO-rich layer initially present at the base of the mantle, the ancient dense material partially survives at the top of ROC piles, causing the piles to be compositionally stratified. Moreover, the addition of such an ancient FeO-rich basal layer significantly aids the preservation of the viscous domains in the mid-mantle. Finally, we find that primordial blobs are commonly directly underlain by thick ROC piles and aid their longevity and stability. Based on our results, we propose an integrated style of mantle heterogeneity for the Earth involving the preservation of primordial domains along with recycled piles. This style has important implications for early Earth evolution and has the potential to reconcile geophysical and geochemical discrepancies on present-day lower-mantle heterogeneity.

Abstract. The nature of compositional heterogeneity in Earth’s lower mantle remains a long-standing puzzle that can inform about the long-term thermochemical evolution and dynamics of our planet. Here, we use global-scale 2D models of thermochemical mantle convection to investigate the coupled evolution and mixing of (intrinsically-dense) recycled and (intrinsically-strong) primordial heterogeneity in the mantle. We explore the effects of ancient compositional layering of the mantle, as motivated by magma-ocean solidification studies, and of the physical parameters of primordial material. Depending on these physical parameters, our models predict various regimes of mantle evolution and heterogeneity preservation over 4.5 Gyrs. Over a wide parameter range, primordial and recycled heterogeneity are predicted to coexist with each other in the lower mantle of Earth-like planets. Primordial material usually survives as mid-to-large scale blobs (or streaks) in the mid-mantle, around 1000–2000 km depth. This preservation is largely independent on the initial primordial-material volume. In turn, recycled oceanic crust (ROC) persists as large piles at the base of the mantle and as small streaks everywhere else. In models with a dense FeO-rich layer that is initially present at the base of the mantle, the FeO-rich material partially survives at the top of ROC piles, causing the piles to be compositionally stratified. Moreover, the addition of an ancient FeO-rich basal layer in the lowermost mantle significantly aids the preservation of the viscous domains in the mid-mantle. Primordial blobs are commonly (but not always) directly underlain by thick ROC piles, and aid their longevity and stability. The preservation of primordial domains along with recycled piles is relevant for Earth as it may reconcile geophysical and geochemical constraints on lower mantle heterogeneity.

The evolution of the system Earth is critically influenced by the long-term dynamics, composition and structure of the mantle. While cosmochemical and geochemical constraints indicate that the lower mantle hosts an ancient primordial reservoir that may be enriched in SiO2 with respect to the upper mantle, geophysical observations and models point to efficient mass transfer and convective mixing across the entire mantle. Recent hypotheses of primordial-material preservation in a convecting mantle involve delayed mixing of intrinsically dense and/or intrinsically strong heterogeneity. Yet, the effects of composition-dependent rheology and density upon heterogeneity preservation and the dynamics of mantle mixing remain poorly understood. Here, we present two-dimensional numerical models in spherical geometry, investigating the preservation styles of primordial material as a function of its physical properties (i.e., viscosity and density contrasts). We establish multiple regimes of primordial-material preservation that can occur in terrestrial planets. These include (1) efficient mixing, (2) double-layered convection with or without topography, and (3) variable styles of partial heterogeneity preservation (e.g., as diffuse domains, piles or viscous blobs in the lower mantle). Some of these regimes are here characterised for the first time, and all regimes are put into context with each other as a function of model parameters. The viscous-blobs and diffuse-domains regimes can reconcile the preservation of primordial domains in a convecting mantle, potentially resolving the discrepancy between geochemical and geophysical constraints for planet Earth. Several, if not all, regimes characterised here may be relevant to understand the long-term evolution of terrestrial planets in general.

<p>In the absence of global plate tectonics, mantle convection and plume-lithosphere interaction are the main drivers of surface deformation on Venus. Whether Venus is geologically active today remains in question: the apparent young surface age and random distribution of impact craters on the planet, initially ascribed as resulting from a global resurfacing event 500-700 Myr ago<sup>1</sup><sup>,</sup><sup>2</sup><sup>,</sup><sup>3</sup>, can also be explained by equilibrium processes, suggestive of ongoing regional resurfacing<sup>4,5</sup>. Moreover, recent studies have identified active hotspots<sup>6,7,8,9 </sup>and young individual lava flows<sup>10 </sup>on the planet.</p> <p>Among documented tectonic structures, circular volcano-tectonic features known as coronae are perhaps the clearest surface manifestations of mantle plumes and may hold clues to the global Venusian tectonic regime. Coronae are characteristic quasi-circular volcano-tectonic features that are abundant on the Venusian surface and generally associated with volcanism, topographic relief, and concentric or radial faulted patterns<sup>9</sup><sup>,</sup><sup>11</sup><sup>,</sup><sup>12 </sup>(left panels of Fig. 1). They feature a wide range of sizes and morphology but typically display an annulus of closely spaced concentric fractures and/or ridges superimposed on a raised rim, with a central relief ranging from domes to depressions<sup>12</sup>. The exact processes underlying their development and the reasons for their diverse morphologies remain controversial.</p> <p>We conducted a systematic 3D numerical study of plume-lithosphere interaction that links the morphological diversity of large coronae to lithospheric structure and provide guidance for identifying which coronae are currently active. The morphology of at least thirty-seven coronae, dominantly located in a region covering Themis Regio, Lada Terra, and Alpha Regio, is consistent with present-day activity. We thereby provide evidence for widespread plume activity on the planet. <em>The work presented here has just been published in Nature Geoscience</em><sup>13</sup>.    <br /><br /><img src="data:image/jpeg;base64, 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