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Overview of the Caloris basin. All images are mosaics in equirectangular projection, and north is up. ( A ) En- hanced (but still subtle) color image map showing 1000-, 750-, and 480-nm images in the red, green, and blue image planes. Yellow boxes are insets shown at higher resolution in (C), (D), and (E); red circles indicate superposed dark craters; blue circles indicate embayed dark craters; and the black arrow indicates the central crater Apollodorus of the radial graben complex. ( B ) Same view after data trans- formation. PC2, which captures variations be- tween light plains and darker terrain, is shown in the green image plane and inverted in the red plane. The ratio of normalized reflectances at 480 nm/1000 nm, which highlights fresh impact ejecta, is shown in the blue plane. Small red spots are extremely red and elevated in albedo; those in white circles are centered on small rimless depressions. Thicker circles indicate features shown in Fig. 3. ( C ) High-resolution view of inset c in (A), showing radially lineated ejecta (white arrow) and massifs embayed by the interior plains (red 

Overview of the Caloris basin. All images are mosaics in equirectangular projection, and north is up. ( A ) En- hanced (but still subtle) color image map showing 1000-, 750-, and 480-nm images in the red, green, and blue image planes. Yellow boxes are insets shown at higher resolution in (C), (D), and (E); red circles indicate superposed dark craters; blue circles indicate embayed dark craters; and the black arrow indicates the central crater Apollodorus of the radial graben complex. ( B ) Same view after data trans- formation. PC2, which captures variations be- tween light plains and darker terrain, is shown in the green image plane and inverted in the red plane. The ratio of normalized reflectances at 480 nm/1000 nm, which highlights fresh impact ejecta, is shown in the blue plane. Small red spots are extremely red and elevated in albedo; those in white circles are centered on small rimless depressions. Thicker circles indicate features shown in Fig. 3. ( C ) High-resolution view of inset c in (A), showing radially lineated ejecta (white arrow) and massifs embayed by the interior plains (red 

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The Caloris basin, the youngest known large impact basin on Mercury, is revealed in MESSENGER images to be modified by volcanism and deformation in a manner distinct from that of lunar impact basins. The morphology and spatial distribution of basin materials themselves closely match lunar counterparts. Evidence for a volcanic origin of the basin's...

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... Caloris basin, the youngest large im- T pact in its basin entirely known during on Mercury, the first encounter was seen of Mercury by the MESSENGER spacecraft in January 2008 ( 1 ). Caloris provides important information for understanding Mercury ’ s geology because it exposes layering of the planet's crust, and it contains tectonic and volcanic features that are well-preserved as compared with those of older basins more modified by subsequent impact cratering. Imaging coverage of the basin interior and ejecta was therefore a focus of the encounter sequence. Here we make use of color and high-resolution monochrome images to re- construct the geological evolution of the basin and to assess the origin and distribution of smooth plains material interior to the basin, the composi- tional stratification of Mercury ’ s upper crust, and the large-scale deformational history of the region. Over 30 years ago, Mariner 10 imaged the eastern part of Caloris ( 2 – 5 ), and the basin has subsequently been studied with ground-based radar ( 6 ). Major units forming the basin include a rim of concentric massifs with intermontane plains (the Caloris Montes and Nervo Formations), which form an annulus varying in width (up to 250 km) surrounding the light-colored basin in- terior (Fig. 1A). An outlying darker annulus consists of rolling ejecta deposits (the Odin Formation), which grade into radially lineated plains and overlapping secondary craters in clusters, thought to be distal sculpted ejecta (the van Eyck Formation). These formations are comparable to counterparts in lunar basin materials, such as the Montes Rook and Hevelius Formations that surround the Orientale basin ( 7 ). Two types of smooth plains were recognized in association with Caloris. Exterior to the basin, annular smooth plains east of Caloris exhibit pervasive wrinkle ridges. The interior of the basin contains plains proposed on the basis of Mariner 10 images to have originated either as volcanic flows ( 2 , 8 ) or impact melt ( 9 ). In the former case, the interior plains would be equivalent to lavas forming Mare Orientale, and in the latter to the Maunder Formation, which is thought to be impact melt. The interior plains exhibit wrinkle ridges and younger, cross-cutting extensional troughs ( 10 – 12 ). Wrinkle ridges, thought to have formed by a combination of thrust faulting and folding ( 13 – 15 ), occur near the eastern basin margin and are both concentric and radial to the basin, a pattern common in mare basalt-filled lunar basins. The troughs are graben formed by extensional stresses and have linear and sinuous segments that form giant polygons ( 10 , 11 , 15 ). Before MESSENGER, it was not known if or how far the wrinkle ridges and graben extended westward into the then-unimaged portion of the basin, or how consistent their spatial and age relations were across the basin. Imaging by the Mercury Dual Imaging System (MDIS) ( 16 ) during MESSENGER ’ s first Mercury flyby was optimized for coverage of Caloris, with a narrow-angle camera mosaic at 200 to 300 m/pixel, and a wide-angle camera 11- color mosaic at 2.4 km/pixel. Both data sets were photometrically corrected to normalized reflectance at a standard geometry (30° incidence angle, 0° emission angle) and map-projected. From the 11-color data, principal component anal- ysis and spectral ratios were used to highlight the most important trends in the data ( 17 ). The first principal component dominantly represents bright- ness variations, whereas the second principal component (PC2) isolates the dominant color variation: the slope of the spectral continuum. Several higher components isolate fresh craters; a simple color ratio combines these and highlights all fresh craters. PC2 and a 480-nm/1000-nm color ratio thus represent the major observed spectral variations (Fig. 1B). The images show that basin exterior materials, including the Caloris Montes, Nervo, and von Eyck Formations, all share similar color properties, which continue with little variation azimuth- ally around the basin from the part imaged by Mariner 10 (Fig. 1). They have a normalized reflectance of ~0.085 at 560 nm, a red lunarlike spectral continuum, and an absence of light- colored smooth plains that occur as patches in the surrounding highlands ( 17 , 18 ). Smooth plains within the Odin Formation lack distinctive color properties. In contrast, Caloris interior plains are about 10% higher in normalized reflectance and have a redder spectral continuum. The northwestern half of the interior plains is both slightly redder and slightly higher in albedo than the southeastern half. The interior plains exhibit craters with diameters of several tens of kilometers whose interiors and ejecta have a lower albedo and less red color than the basin exterior and resemble darker terrain exterior to the basin (red circles, Fig. 1A). The northwestern part of the basin interior exhibits craters with similar dark rims but light floors resembling the interior plains (blue circles, Fig. 1A). The margin of the basin contains diffuse, 30- to 100-km-diameter patches of very red material, typically ~40% higher in normalized reflectance than the basin exterior (red patches in Fig. 1B, circled in white). Fresh impact craters with comparably elevated albedo are spectrally distinctive from the red patches, with a less red spectral continuum than other materials (bluer color in Fig. 1B) as is also typical of fresh lunar craters ( 19 ). Higher-resolution views of the western annulus (Fig. 1, C to E) show smooth to rolling plains surrounding the edge of the basin, which grade into radially lineated equivalents of the van Eyck Formation, particularly in the northwest (white arrow, Fig. 1C). The northwestern part of the basin interior also exhibits interior plains embay- ing knobs of the basin rim as well as a partly preserved inner ring, whose eastern portion was suggested in Mariner 10 images but not identified definitively ( 2 ) (red arrows, Fig. 1C). The western equivalent of the Caloris Montes Formation (red arrows, Fig. 1D) is an inward-facing scarp broken into clusters of knobs, locally higher in normalized reflectance. Fitting the entirety of Caloris Montes yields a main basin ring diameter of 1550 km, as compared with 1340 km estimated from Mariner 10 data. The western interior plains (Fig. 1E) are deformed by both wrinkle ridges and extensional troughs, similarly to the eastern part of the plains imaged by Mariner 10. The continuity in color and morphology around the basin interior and exterior indicates that the units seen by Mariner 10 extend throughout the rest of the basin and its surroundings. Two lines of evidence support the idea that the interior plains were emplaced by volcanism, as the stratigraphic equivalent of lunar maria rather than as Caloris impact melt deposits. The first line of evidence is the occurrence within the main basin ring of craters flooded by light- colored interior plains, analogous to lunar basin interior craters such as Archimedes in Mare Imbrium. Some interior craters (red circles, Fig. 1A) have color and morphology consistent with their superposition on the interior plains (left column, Fig. 2): unbroken crater rims and intact central peak rings; a gradual change in ejecta texture with radial distance from the crater rim; and interior color and albedo properties consistent with the crater wall but distinct from surrounding plains, suggesting that an underlying dark layer was excavated. In contrast, craters interpreted as embayed and infilled (blue circles, Fig. 1A, and right column, Fig. 2) have attributes suggesting that they were flooded by interior plains material: breached rims and discontinuous central peak rings, an abrupt change in texture outside the crater where plains lap onto ejecta, and interior color properties distinct from the crater wall but matching the surrounding, lighter plains. Because the formation times of the several large craters on the Caloris floor must have spanned an interval much longer than that re- quired for the emplacement of impact melts, the infilling of these craters must have occurred subsequently. Spudis and Guest ( 2 ) used Mariner 10 images and similar criteria to interpret a volcanic origin for light-colored interior plains of the Tolstoj basin, located to the southeast of Caloris. Interior flooding and embayment relations similar to these are also seen in smooth plains outside the Caloris basin in the MESSENGER data ( 17 , 18 ). The second line of evidence for volcanism is the presence of diffuse bright deposits concen- trated along the margin of the basin (Fig. 3), asso- ciated with apparent volcanic structures ( 18 ). The bright deposits have a redder spectral continuum than other materials, in contrast to comparably bright fresh impact craters, which also typically display prominent rays ( 19 ). Moreover, the bright deposits are centered on irregularly shaped, scallop-rimmed depressions without raised rims. The morphology of these depressions does not resemble that of impact craters but is ...
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... Fitting the entirety of Caloris Montes yields a main basin ring diameter of 1550 km, as compared with 1340 km estimated from Mariner 10 data. The western interior plains (Fig. 1E) are deformed by both wrinkle ridges and extensional troughs, similarly to the eastern part of the plains imaged by Mariner 10. The continuity in color and morphology around the basin interior and exterior indicates that the units seen by Mariner 10 extend throughout the rest of the basin and its surroundings. Two lines of evidence support the idea that the interior plains were emplaced by volcanism, as the stratigraphic equivalent of lunar maria rather than as Caloris impact melt deposits. The first line of evidence is the occurrence within the main basin ring of craters flooded by light- colored interior plains, analogous to lunar basin interior craters such as Archimedes in Mare Imbrium. Some interior craters (red circles, Fig. 1A) have color and morphology consistent with their superposition on the interior plains (left column, Fig. 2): unbroken crater rims and intact central peak rings; a gradual change in ejecta texture with radial distance from the crater rim; and interior color and albedo properties consistent with the crater wall but distinct from surrounding plains, suggesting that an underlying dark layer was excavated. In contrast, craters interpreted as embayed and infilled (blue circles, Fig. 1A, and right column, Fig. 2) have attributes suggesting that they were flooded by interior plains material: breached rims and discontinuous central peak rings, an abrupt change in texture outside the crater where plains lap onto ejecta, and interior color properties distinct from the crater wall but matching the surrounding, lighter plains. Because the formation times of the several large craters on the Caloris floor must have spanned an interval much longer than that re- quired for the emplacement of impact melts, the infilling of these craters must have occurred subsequently. Spudis and Guest ( 2 ) used Mariner 10 images and similar criteria to interpret a volcanic origin for light-colored interior plains of the Tolstoj basin, located to the southeast of Caloris. Interior flooding and embayment relations similar to these are also seen in smooth plains outside the Caloris basin in the MESSENGER data ( 17 , 18 ). The second line of evidence for volcanism is the presence of diffuse bright deposits concen- trated along the margin of the basin (Fig. 3), asso- ciated with apparent volcanic structures ( 18 ). The bright deposits have a redder spectral continuum than other materials, in contrast to comparably bright fresh impact craters, which also typically display prominent rays ( 19 ). Moreover, the bright deposits are centered on irregularly shaped, scallop-rimmed depressions without raised rims. The morphology of these depressions does not resemble that of impact craters but is consistent with volcanic vents observed in the lunar maria ( 20 ). Similar diffuse deposits on the Moon are pyroclastic in origin ( 21 ), and we interpret these deposits to be pyroclastic as well. Spectrally similar materials are also observed surrounding some- what degraded craters on the Caloris interior plains; these craters are smaller than those ex- posing dark material, suggesting that material resembling the diffuse deposits was excavated from a shallower depth in the interior plains. Unlike the lunar maria, the Caloris interior plains are higher in albedo than the underlying basin material and lack spectral evidence for silicates containing ferrous iron (Fe ). Neither fresh craters, nor the diffuse bright patches, nor any other materials exhibit a resolvable absorption at 0.90 to 1.05 m m (the 1- m m absorption) due to Fe-bearing olivine or pyroxene ( 17 ). Such an absorption feature is typical of young lunar craters superposed on either the lunar maria or average highlands. The lack of a 1- m m absorption suggests that the content of Fe in silicates is much lower than in the lunar maria ( 19 ); common ig- neous silicate minerals consistent with the absence of a 1- m m absorption include Mg-rich olivine, Mg- or Mg-Ca rich pyroxene, or plagi- oclase feldspar. MESSENGER images show that graben orientation progresses from a dominantly radial pattern at the center of the basin to a polygonal pattern at the edge of the basin. The outer graben overlap the radial distance range of wrinkle ridges (Fig. 4). The basin-radial graben include more than 230 linear troughs that converge near the center of the basin (~30°N, 163°E) as part of Pantheon Fossae, some of whose distal portions were previously mapped as part of the polygonal graben patterns in the Mariner 10 images of eastern Caloris ( 10 , 11 , 13 ). The measured lengths of individual graben range from ~5 to ~110 km, and widths range from less than 1 km up to a max- imum of ~8 km. An impact crater about 40 km in diameter, Apollodorus, is located near the center of the complex (black arrow, Fig. 1, A and B). The crater's rim, wall, and floor expose dark material, as do other large craters superposed on the interior plains. The crater rim is not cross-cut by the graben, and proximal ejecta obscure the graben. These relations suggest that the graben postdate the plains and that the dep- osition of crater ejecta postdates the graben. Farther from the center of the basin, the polyg- onally arranged graben form a broad annulus of extensional deformation (Fig. 4). The distal graben of Pantheon Fossae appear as segments of the polygons and part of the regional extension. Wrinkle ridges extend farther from the basin center than do the graben. MESSENGER s high-Sun light- ing geometry makes the recognition of low-relief ridges difficult; accordingly, a lower density of wrinkle ridges is recognized in MESSENGER imaging than in overlapping Mariner 10 imaging of eastern Caloris. The cross-cutting relations be- tween wrinkle ridges and graben are consistent in both eastern and western Caloris; where the two types of features intersect, and their age rela- tion can be determined, wrinkle ridges are always cut by and thus are older than the graben. The pattern within Caloris of central radial graben and distal radial and concentric graben cross-cutting wrinkle ridges contrasts sharply with the spatial and temporal distribution of comparable features in lunar basins. In the lunar maria, wrinkle ridges occur predominantly in basin interiors, whereas graben are found in more distal parts or outside the basins ( 22 , 23 ). Wrinkle ridges occur in the youngest lunar mare basalts, whereas lunar graben are restricted to the oldest basalts ( 24 , 25 ). There is also no lunar counterpart to Pantheon Fossae. On the Moon, the distribution of wrinkle ridges and graben is thought to result from loading of the lithosphere by relatively dense, uncompensated mare basalt material, which in- duces subsidence and flexure of the lithosphere, leading to compression in the basin interiors and extension at the margins ( 23 , 26 ). The spatial and temporal distribution of tectonic features in Caloris cannot be fully explained by such models. Wrinkle ridges in Caloris may have formed in response to subsidence of the interior plains ( 10 ), possibly aided by a compressional stress due to global contraction ( 11 ). Two models have been proposed to account for interior extension in Caloris: exterior loading and lateral crustal flow. In the exterior loading model, the superposition of smooth plains exterior to the Caloris basin results in an annular load that causes basin-interior uplift and exten- sion ( , ). The lateral flow model involves movement of the lowest portions of postulated thick crust exterior to the basin inward toward the basin center, which causes late-stage uplift and extension ( 11 ). The central radial graben complex in Caloris presents a new constraint for these models, namely that tangential extensional stress exceeded radial extensional stress throughout the central basin region in order to account for the radial arrangement of the troughs. Another pos- sibility is that Pantheon Fossae formed as the surface expressions of dikes that propagated radially from a magmatic intrusion near the basin center ( 18 ). From the combination of MESSENGER and Mariner 10 data, six major phases in the history of the interior of the Caloris basin can be recognized: (i) formation of an impact basin and emplacement of impact melt ( 27 ) that must now be buried; (ii) superposition of several large craters in the basin interior; (iii) volcanic emplacement of light, redder material to form the interior plains, in part by pyroclastic and in part by ef- fusive processes; (iv) formation (or continued activation) of wrinkle ridges in the outer part of the basin; (v) formation of radial and concentric graben; and (vi) superposition of still more impact craters, with smaller craters penetrating and excavating only the youngest volcanic plains and larger ones penetrating through to underlying darker material. Analysis of crater density variations ( 28 ) suggests that the emplacement of smooth plains exterior to the basin continued after phase ...
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... of the encounter sequence. Here we make use of color and high-resolution monochrome images to re- construct the geological evolution of the basin and to assess the origin and distribution of smooth plains material interior to the basin, the composi- tional stratification of Mercury ’ s upper crust, and the large-scale deformational history of the region. Over 30 years ago, Mariner 10 imaged the eastern part of Caloris ( 2 – 5 ), and the basin has subsequently been studied with ground-based radar ( 6 ). Major units forming the basin include a rim of concentric massifs with intermontane plains (the Caloris Montes and Nervo Formations), which form an annulus varying in width (up to 250 km) surrounding the light-colored basin in- terior (Fig. 1A). An outlying darker annulus consists of rolling ejecta deposits (the Odin Formation), which grade into radially lineated plains and overlapping secondary craters in clusters, thought to be distal sculpted ejecta (the van Eyck Formation). These formations are comparable to counterparts in lunar basin materials, such as the Montes Rook and Hevelius Formations that surround the Orientale basin ( 7 ). Two types of smooth plains were recognized in association with Caloris. Exterior to the basin, annular smooth plains east of Caloris exhibit pervasive wrinkle ridges. The interior of the basin contains plains proposed on the basis of Mariner 10 images to have originated either as volcanic flows ( 2 , 8 ) or impact melt ( 9 ). In the former case, the interior plains would be equivalent to lavas forming Mare Orientale, and in the latter to the Maunder Formation, which is thought to be impact melt. The interior plains exhibit wrinkle ridges and younger, cross-cutting extensional troughs ( 10 – 12 ). Wrinkle ridges, thought to have formed by a combination of thrust faulting and folding ( 13 – 15 ), occur near the eastern basin margin and are both concentric and radial to the basin, a pattern common in mare basalt-filled lunar basins. The troughs are graben formed by extensional stresses and have linear and sinuous segments that form giant polygons ( 10 , 11 , 15 ). Before MESSENGER, it was not known if or how far the wrinkle ridges and graben extended westward into the then-unimaged portion of the basin, or how consistent their spatial and age relations were across the basin. Imaging by the Mercury Dual Imaging System (MDIS) ( 16 ) during MESSENGER ’ s first Mercury flyby was optimized for coverage of Caloris, with a narrow-angle camera mosaic at 200 to 300 m/pixel, and a wide-angle camera 11- color mosaic at 2.4 km/pixel. Both data sets were photometrically corrected to normalized reflectance at a standard geometry (30° incidence angle, 0° emission angle) and map-projected. From the 11-color data, principal component anal- ysis and spectral ratios were used to highlight the most important trends in the data ( 17 ). The first principal component dominantly represents bright- ness variations, whereas the second principal component (PC2) isolates the dominant color variation: the slope of the spectral continuum. Several higher components isolate fresh craters; a simple color ratio combines these and highlights all fresh craters. PC2 and a 480-nm/1000-nm color ratio thus represent the major observed spectral variations (Fig. 1B). The images show that basin exterior materials, including the Caloris Montes, Nervo, and von Eyck Formations, all share similar color properties, which continue with little variation azimuth- ally around the basin from the part imaged by Mariner 10 (Fig. 1). They have a normalized reflectance of ~0.085 at 560 nm, a red lunarlike spectral continuum, and an absence of light- colored smooth plains that occur as patches in the surrounding highlands ( 17 , 18 ). Smooth plains within the Odin Formation lack distinctive color properties. In contrast, Caloris interior plains are about 10% higher in normalized reflectance and have a redder spectral continuum. The northwestern half of the interior plains is both slightly redder and slightly higher in albedo than the southeastern half. The interior plains exhibit craters with diameters of several tens of kilometers whose interiors and ejecta have a lower albedo and less red color than the basin exterior and resemble darker terrain exterior to the basin (red circles, Fig. 1A). The northwestern part of the basin interior exhibits craters with similar dark rims but light floors resembling the interior plains (blue circles, Fig. 1A). The margin of the basin contains diffuse, 30- to 100-km-diameter patches of very red material, typically ~40% higher in normalized reflectance than the basin exterior (red patches in Fig. 1B, circled in white). Fresh impact craters with comparably elevated albedo are spectrally distinctive from the red patches, with a less red spectral continuum than other materials (bluer color in Fig. 1B) as is also typical of fresh lunar craters ( 19 ). Higher-resolution views of the western annulus (Fig. 1, C to E) show smooth to rolling plains surrounding the edge of the basin, which grade into radially lineated equivalents of the van Eyck Formation, particularly in the northwest (white arrow, Fig. 1C). The northwestern part of the basin interior also exhibits interior plains embay- ing knobs of the basin rim as well as a partly preserved inner ring, whose eastern portion was suggested in Mariner 10 images but not identified definitively ( 2 ) (red arrows, Fig. 1C). The western equivalent of the Caloris Montes Formation (red arrows, Fig. 1D) is an inward-facing scarp broken into clusters of knobs, locally higher in normalized reflectance. Fitting the entirety of Caloris Montes yields a main basin ring diameter of 1550 km, as compared with 1340 km estimated from Mariner 10 data. The western interior plains (Fig. 1E) are deformed by both wrinkle ridges and extensional troughs, similarly to the eastern part of the plains imaged by Mariner 10. The continuity in color and morphology around the basin interior and exterior indicates that the units seen by Mariner 10 extend throughout the rest of the basin and its surroundings. Two lines of evidence support the idea that the interior plains were emplaced by volcanism, as the stratigraphic equivalent of lunar maria rather than as Caloris impact melt deposits. The first line of evidence is the occurrence within the main basin ring of craters flooded by light- colored interior plains, analogous to lunar basin interior craters such as Archimedes in Mare Imbrium. Some interior craters (red circles, Fig. 1A) have color and morphology consistent with their superposition on the interior plains (left column, Fig. 2): unbroken crater rims and intact central peak rings; a gradual change in ejecta texture with radial distance from the crater rim; and interior color and albedo properties consistent with the crater wall but distinct from surrounding plains, suggesting that an underlying dark layer was excavated. In contrast, craters interpreted as embayed and infilled (blue circles, Fig. 1A, and right column, Fig. 2) have attributes suggesting that they were flooded by interior plains material: breached rims and discontinuous central peak rings, an abrupt change in texture outside the crater where plains lap onto ejecta, and interior color properties distinct from the crater wall but matching the surrounding, lighter plains. Because the formation times of the several large craters on the Caloris floor must have spanned an interval much longer than that re- quired for the emplacement of impact melts, the infilling of these craters must have occurred subsequently. Spudis and Guest ( 2 ) used Mariner 10 images and similar criteria to interpret a volcanic origin for light-colored interior plains of the Tolstoj basin, located to the southeast of Caloris. Interior flooding and embayment relations similar to these are also seen in smooth plains outside the Caloris basin in the MESSENGER data ( 17 , 18 ). The second line of evidence for volcanism is the presence of diffuse bright deposits concen- trated along the margin of the basin (Fig. 3), asso- ciated with apparent volcanic structures ( 18 ). The bright deposits have a redder spectral continuum than other materials, in contrast to comparably bright fresh impact craters, which also typically display prominent rays ( 19 ). Moreover, the bright deposits are centered on irregularly shaped, scallop-rimmed depressions without raised rims. The morphology of these depressions does not resemble that of impact craters but is consistent with volcanic vents observed in the lunar maria ( 20 ). Similar diffuse deposits on the Moon are pyroclastic in origin ( 21 ), and we interpret these deposits to be pyroclastic as well. Spectrally similar materials are also observed surrounding some- what degraded craters on the Caloris interior plains; these craters are smaller than those ex- posing dark material, suggesting that material resembling the diffuse deposits was excavated from a shallower depth in the interior plains. Unlike the lunar maria, the Caloris interior plains are higher in albedo than the underlying basin material and lack spectral evidence for silicates containing ferrous iron (Fe ). Neither fresh craters, nor the diffuse bright patches, nor any other materials exhibit a resolvable absorption at 0.90 to 1.05 m m (the 1- m m absorption) due to Fe-bearing olivine or pyroxene ( 17 ). Such an absorption feature is typical of young lunar craters superposed on either the lunar maria or average highlands. The lack of a 1- m m absorption suggests that the content of Fe in silicates is much lower than in the lunar maria ( 19 ); common ig- neous silicate minerals consistent with the absence of a 1- m m absorption include Mg-rich olivine, Mg- or Mg-Ca rich pyroxene, or plagi- oclase feldspar. MESSENGER images show that graben orientation progresses from a dominantly radial pattern at the center of the basin to a polygonal pattern at the ...

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... There has been much speculation that Mercury's 1,550-km-diameter Caloris basin is a multiring basin (Fassett et al., 2009;Murchie et al., 2008;Oberst et al., 2010;Spudis, 1993;Spudis & Guest, 1988;Strom et al., 1975). However, Caloris' candidate ring locations identified using Mariner 10 imagery (e.g., Spudis & Guest, 1988) were either not evident in the higher resolution images provided by the MESSENGER spacecraft (Fassett et al., 2009) or found to be highly eroded and azimuthally discontinuous (Oberst et al., 2010), comparable to the putative rings encircling SPA (cf., Garrick-Bethell & Zuber, 2009). ...
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In contrast to multiring basins, megabasins lack clear ring structures and display crustal profiles characterized by a thin layer of crust at their center that gradually increases in thickness to the surrounding region. The 1,550‐km‐diameter Caloris basin on Mercury is often speculated to be a multiring basin; however, its crustal structure is indicative of a megabasin, perhaps explaining the lack of discernible rings. Here, we model the formation of Caloris basin using iSALE‐2D under a range of preimpact thermal conditions to determine whether the processes responsible for its megabasin crustal structure could lead to the formation of basin rings. We find that thermal gradients between 22 and 30 K/km—hotter than previously inferred—facilitate the reproduction of Caloris basin's crustal structure through crustal flowback, though such preimpact thermal structures preclude its formation as a multiring basin. Instead, repeated thrusting and necking events during transient crater collapse induce instances of fault reactivation, which diminish initial fault offsets and produce a series of discrete crustal blocks. Models assuming cooler thermal gradients lead to overly thin or non‐existent crust at the basin center, in contrast to observations. Even if crustal deficits were made up via a differentiating melt pool, the crust elsewhere would be overly thick, supporting the idea that the crustal structure of megabasins is primarily associated with transient crater collapse. We conclude that the transition to a megabasin morphology on terrestrial planetary surfaces, like the multiring transition, is dependent upon the size of the basin compared to the lithospheric thickness.
... 10.1029/2023JE007796 3 of 18 Murchie et al., 2008;Strom et al., 2008;Wang et al., 2021), the impact rate declined sharply (Denevi et al., 2018) and the global effusive volcanism ceased in the period of 3.7-3.5 Ga as well (Byrne et al., 2016;Wang et al., 2021). ...
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The elastic thickness of a planet's lithosphere is essential to the investigation of its thermal evolution. Our work focuses on the largest visible impact basin on Mercury, Caloris, which has undergone complex magma‐tectonic deformation after its formation. Using a flexural lithosphere model with the initial mantle plug loading, we estimated the elastic thickness in the Caloris region to be 18.0 ± $\pm $ 4.4 km. The successful application of the mantle loading model and the small load ratio indicates that major load in the Caloris region is the mantle plug rather than the lateral density anomaly. The 18 km effective elastic thickness indicates the lithospheric temperature at the time of loading. The current heat production rate in Mercury mantle is estimated as 2.2–4.2 × 10⁻¹² W/kg. Comparison between the effective elastic thickness predicted from the thermal model and loading model suggests that the megaregolith in the Caloris basin region has a certain thickness (>3 km) to ensure the formation of a lithosphere with 18 km elastic thickness. The temperature model results also indicate that the mantle heat production rate at 3.6 Ga is closer to that calculated based on a model with heat‐producing elements abundance close to CI chondrite‐like primitive silicate portion of Mercury. The surface heat flow in the Caloris region is consistent with other megaregolith‐covered regions.
... Subsequent work on lunar wrinkle ridges has quantified their map-view patterns, crosssectional shapes, spatial distributions, geologic contexts, and formation ages (e.g., Tjia, 1970;Strom, 1972;Bryan, 1973;Plescia and Golombek, 1986;Watters, 1988Watters, , 2022Yue Z et al., 2015Yue Z et al., , 2017Li B et al., 2018). Images collected by spacecrafts through the inner solar system show that linear and sinuous positive landforms similar to lunar wrinkle ridges occur on all rocky planets : (1) Mercury (Murray et al., 1974;Strom et al., 1975;Strom, 1979;Maxwell and Gifford, 1980;Murchie et al., 2008;Watters et al., 2009a, b;Byrne et al., 2014;Crane and Klimczak, 2019;Schleicher et al., 2019;Watters, 2021), (2) Venus (Watters, 1992;McGill, 1993McGill, , 2004Kreslavsky and Basilevsky, 1998;Bilotti and Suppe, 1999;Basilevsky and Head, 2006;Hansen and Olive, 2010;Ivanov and Head, 2011;Byrne et al., 2021;Bethell et al., 2022), (3) Mars (Wilhelms, 1974;Carr et al., 1977;Greeley and Spudis, 1978a, b;Lucchitta, 1978;Lucchitta and Klockenbrink, 1981;Watters, 1991Watters, , 1993Zuber 1995;Watters and Robinson, 1997;Mangold et al., 1998;Schultz, 2000;Golombek et al., 2001;Head et al., 2002;Montési and Zuber, 2003;Mueller and Golombek, 2004;Ruj and Kawai, 2021;Karagoz et al., 2022a, b), and (4) the Earth (Reidel, 1984;Plescia and Golombek, 1986). A shared characteristic of wrinkle ridges on the rocky planets and the Moon is that their formation is closely associated in space and possibly in time with flood-basalt volcanism (e.g., Plescia and Golombek, 1986;Watters, 1988). ...
Article
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Wrinkle ridges are common landforms documented on all rocky planets and the Moon in the inner solar system. Despite the long research history, their formation mechanisms remain debated. A key unresolved issue is whether the wrinkle-ridge formation is related to igneous processes. This is because wrinkle ridges are mostly associated in space and possibly in time with the occurrence of flood-basalt volcanism in all cases in the inner solar system. To address this issue, we conducted geomorphological mapping, a topographic-data analysis, and a detailed landform and landsystem analysis of satellite images at a resolution of 25 cm/pixel to 6 m/pixel in the central Tharsis region of Mars. The main results of this work are in the form of (1) a regional geomorphological map at a resolution of 6 m/pixel and (2) a local geomorphological map at a resolution of 50 cm/pixel. Our work suggests the following older-to-younger sequence of geological events in the study area: (1) formation of a northeast-trending mountain range (i.e., the Thaumasia plateau) along the eastern margin of the Tharsis rise that was created by the Himalayan-style crustal-scale thrusting; (2) coeval volcanic-plateau construction west of the thrusting-induced rising mountain range; (3) eastward-flowing lavas that were sourced from a volcanic plateau to the west terminated at the rising Thaumasia plateau to the east; (4) wrinkle-ridge development by decollement folding of recently emplaced warm, ductile volcanic-lava piles; (5) emplacement of a regionally extensive ice sheet over the central Tharsis region that produced extensive boulder-bearing materials, striated surfaces, and boulder-bearing dendritic-ridge networks possibly representing subglacial eskers; and (6) local deposition of highly concentrated glacial flours resulted in the formation of mantled terrain on plains between wrinkle ridges. Our work supports the early suggestion that the Tharsis wrinkle ridges were created by horizontal shortening induced by crustal-scale tectonic processes. In detail, however, the occurrence of flow-front-like fold margins associated with many mapped wrinkle ridges suggests the involvement of ductile-flow deformation during ridge formation. We attribute the flow-like fold fronts to ductile deformation of thermally weakened lava piles that were emplaced during or immediately before the folding event. Our compression-induced wrinkle-ridge model also differs from the early hypotheses in that the thin-skinned folding is associated with basement subduction, which explains the lack of coeval and parallel folding and extensional faulting associated with wrinkle ridge formation in the study area. Post-folding glacial modification means that the present wrinkle-ridge morphologies may differ significantly from the original fold shapes, which prevents the utility of using topographic profiles across wrinkle ridges for inverting the underlying thrust geometries.
... Subsequent work on lunar wrinkle ridges has quantified their map-view patterns, crosssectional shapes, spatial distributions, geologic contexts, and formation ages (e.g., Tjia, 1970;Strom, 1972;Bryan, 1973;Plescia and Golombek, 1986;Watters, 1988Watters, , 2022Yue Z et al., 2015Yue Z et al., , 2017Li B et al., 2018). Images collected by spacecrafts through the inner solar system show that linear and sinuous positive landforms similar to lunar wrinkle ridges occur on all rocky planets : (1) Mercury (Murray et al., 1974;Strom et al., 1975;Strom, 1979;Maxwell and Gifford, 1980;Murchie et al., 2008;Watters et al., 2009a, b;Byrne et al., 2014;Crane and Klimczak, 2019;Schleicher et al., 2019;Watters, 2021), (2) Venus (Watters, 1992;McGill, 1993McGill, , 2004Kreslavsky and Basilevsky, 1998;Bilotti and Suppe, 1999;Basilevsky and Head, 2006;Hansen and Olive, 2010;Ivanov and Head, 2011;Byrne et al., 2021;Bethell et al., 2022), (3) Mars (Wilhelms, 1974;Carr et al., 1977;Greeley and Spudis, 1978a, b;Lucchitta, 1978;Lucchitta and Klockenbrink, 1981;Watters, 1991Watters, , 1993Zuber 1995;Watters and Robinson, 1997;Mangold et al., 1998;Schultz, 2000;Golombek et al., 2001;Head et al., 2002;Montési and Zuber, 2003;Mueller and Golombek, 2004;Ruj and Kawai, 2021;Karagoz et al., 2022a, b), and (4) the Earth (Reidel, 1984;Plescia and Golombek, 1986). A shared characteristic of wrinkle ridges on the rocky planets and the Moon is that their formation is closely associated in space and possibly in time with flood-basalt volcanism (e.g., Plescia and Golombek, 1986;Watters, 1988). ...
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Key Points: Wrinkle ridges in the Tharsis region of Mars were induced by decollement folding. q Folding occurred during flood-basalt volcanism. q Undeformed basement of the folded strata was subducted below the volcanic eruption zone. q Regional glaciation across the Tharsis rise modified the original shapes of the wrinkle ridges. q Citation: Yin, A., and Wang, Y. C. (2023). Formation and modification of wrinkle ridges in the central Tharsis region of Mars as constrained by detailed geomorphological mapping and landsystem analysis. Earth Planet. Phys., 7(2), 161-192. http://doi. Abstract: Wrinkle ridges are common landforms documented on all rocky planets and the Moon in the inner solar system. Despite the long research history, their formation mechanisms remain debated. A key unresolved issue is whether the wrinkle-ridge formation is related to igneous processes. This is because wrinkle ridges are mostly associated in space and possibly in time with the occurrence of flood-basalt volcanism in all cases in the inner solar system. To address this issue, we conducted geomorphological mapping, a topographic-data analysis, and a detailed landform and landsystem analysis of satellite images at a resolution of 25 cm/pixel to 6 m/pixel in the central Tharsis region of Mars. The main results of this work are in the form of (1) a regional geomorphological map at a resolution of 6 m/pixel and (2) a local geomorphological map at a resolution of 50 cm/pixel. Our work suggests the following older-to-younger sequence of geological events in the study area: (1) formation of a northeast-trending mountain range (i.e., the Thaumasia plateau) along the eastern margin of the Tharsis rise that was created by the Himalayan-style crustal-scale thrusting; (2) coeval volcanic-plateau construction west of the thrusting-induced rising mountain range; (3) eastward-flowing lavas that were sourced from a volcanic plateau to the west terminated at the rising Thaumasia plateau to the east; (4) wrinkle-ridge development by decollement folding of recently emplaced warm, ductile volcanic-lava piles; (5) emplacement of a regionally extensive ice sheet over the central Tharsis region that produced extensive boulder-bearing materials, striated surfaces, and boulder-bearing dendritic-ridge networks possibly representing subglacial eskers; and (6) local deposition of highly concentrated glacial flours resulted in the formation of mantled terrain on plains between wrinkle ridges. Our work supports the early suggestion that the Tharsis wrinkle ridges were created by horizontal shortening induced by crustal-scale tectonic processes. In detail, however, the occurrence of flow-front-like fold margins associated with many mapped wrinkle ridges suggests the involvement of ductile-flow deformation during ridge formation. We attribute the flow-like fold fronts to ductile deformation of thermally weakened lava piles that were emplaced during or immediately before the folding event. Our compression-induced wrinkle-ridge model also differs from the early hypotheses in that the thinskinned folding is associated with basement subduction, which explains the lack of coeval and parallel folding and extensional faulting associated with wrinkle ridge formation in the study area. Post-folding glacial modification means that the present wrinkle-ridge morphologies may differ significantly from the original fold shapes, which prevents the utility of using topographic profiles across wrinkle ridges for inverting the underlying thrust geometries.
... Subsequent work on lunar wrinkle ridges has quantified their map-view patterns, crosssectional shapes, spatial distributions, geologic contexts, and formation ages (e.g., Tjia, 1970;Strom, 1972;Bryan, 1973;Plescia and Golombek, 1986;Watters, 1988Watters, , 2022Yue Z et al., 2015Yue Z et al., , 2017Li B et al., 2018). Images collected by spacecrafts through the inner solar system show that linear and sinuous positive landforms similar to lunar wrinkle ridges occur on all rocky planets : (1) Mercury (Murray et al., 1974;Strom et al., 1975;Strom, 1979;Maxwell and Gifford, 1980;Murchie et al., 2008;Watters et al., 2009a, b;Byrne et al., 2014;Crane and Klimczak, 2019;Schleicher et al., 2019;Watters, 2021), (2) Venus (Watters, 1992;McGill, 1993McGill, , 2004Kreslavsky and Basilevsky, 1998;Bilotti and Suppe, 1999;Basilevsky and Head, 2006;Hansen and Olive, 2010;Ivanov and Head, 2011;Byrne et al., 2021;Bethell et al., 2022), (3) Mars (Wilhelms, 1974;Carr et al., 1977;Greeley and Spudis, 1978a, b;Lucchitta, 1978;Lucchitta and Klockenbrink, 1981;Watters, 1991Watters, , 1993Zuber 1995;Watters and Robinson, 1997;Mangold et al., 1998;Schultz, 2000;Golombek et al., 2001;Head et al., 2002;Montési and Zuber, 2003;Mueller and Golombek, 2004;Ruj and Kawai, 2021;Karagoz et al., 2022a, b), and (4) the Earth (Reidel, 1984;Plescia and Golombek, 1986). A shared characteristic of wrinkle ridges on the rocky planets and the Moon is that their formation is closely associated in space and possibly in time with flood-basalt volcanism (e.g., Plescia and Golombek, 1986;Watters, 1988). ...
... One possible cryovolcanic caldera (Sippar Sulcus) and one impact crater chain should be further examined, which are currently the two most promising features Triton Identification Tectonic fracturing, cryovolcanic? Three plumes identified unambiguously (Croft et al., 1995;Hofgartner et al., 2022); four to 14 additional potential plumes and ≥100 fans (inferred to be cryovolcanic vents and/or phase change caves) in the Southern Hemisphere terrain require further examination One catena (Robbins et al., 2019) and at least 13 lobate aprons that may support talus caves should be further studied Comet 67P Identification Sublimation, fracturing, landslides 18 sublimation pits identified (Vincent, Bodewits, et al., 2015); however, none of these features were considered SAPs; talus caves also possible, but not confirmed Table 1 Research Stage (Identification, Characterization, and Exploration;Refer to Titus, Wynne, Malaska, et al. [2021] There are other depressions on Mercury that are not impact in nature, including: likely sublimation features termed "hollows" ; irregularly shaped, coalesced depressions interpreted as sites of explosive volcanic activity (Rothery et al., 2014), such as those along the inner perimeter of the Caloris impact basin (e.g., Murchie et al., 2008); and large depressions in expansive lava channels in the planet's northern hemisphere (Byrne et al., 2013). The origin of this third type of depression is unclear, but by all accounts, none of these depressions can be considered SAPs using the currently available data. ...
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We provide the first solar system wide compendium of speleogenic processes and products. An examination of 15 solar system bodies revealed that six cave‐forming processes occur beyond Earth including volcanic (cryo and magmatic), fracturing (tectonic and impact melt), dissolution, sublimation, suffusion, and landslides. Although no caves (i.e., confirmed entrances with associated linear passages) have been confirmed, 3,545 SAPs (subsurface access points) have been identified on 11 planetary bodies and the potential for speleogenic processes (and thus SAPs) was observed on an additional four planetary bodies. The bulk of our knowledge on extraterrestrial SAPs is based on global databases for the Moon and Mars, which are bodies for which high‐resolution imagery and other data are available. To further characterize most of the features beyond the Moon and Mars, acquisition (preferably global coverage) and subsequent analysis of high‐resolution imagery will be required. The next few decades hold considerable promise for further identifying and characterizing caves across the solar system.
... basin yielded an absolute model age of ∼3.8 Ga, slightly older than CIP and NSP (Mancinelli et al., 2016;Murchie et al., 2008;Strom et al., 2008). Geophysical modeling revealed that thermal disturbance caused by the Caloris impact can last over 100 Myr, enhancing volcanism in the basin interior (Padovan et al., 2017;Roberts & Barnouin, 2012). ...
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Plain Language Summary The history of volcanism is a pulse curve of geodynamics of planetary bodies. Large smooth plains on Mercury were formed by effusive volcanism before 3.5 Ga. Small smooth plains occupy a substantial portion of this planet and they have a wider geographic distribution than larger ones, but their possible origins have not been systematically studied. The patchy occurrence of small smooth plains indicates that they may better represent the global thermal evolution. Here, we update the global distribution of small smooth plains and investigate the absolute model age and possible origin for each case. At least 123 of the 315 cataloged small smooth plains were likely emplaced by effusive volcanism that preferentially occurred at thin crust areas. Smooth plains, regardless of origins and sizes, were mainly formed in ∼200 million years around 3.7 Ga, revealing that >24.9% of Mercury surface was emplaced by short‐term effusive volcanism. The preferential occurrence of volcanic smooth plains around the Caloris, Rembrandt, and Beethoven basins suggests a possible trigger by these impact events. We report evidence showing that coeval and collocated small smooth plains can have different origins, as some smooth plains may be ponded ejecta deposits that were emplaced by contemporaneous impact basins.
... Major smooth plains deposits on Mercury (Fig. 4) include: Borealis Planitia (formerly known as Mercury's "northern smooth plains" or the "northern volcanic plains": Head et al., 2011;Ostrach et al., 2015); Caloris Planitia (the smooth plains within the Caloris Basin, the largest well-preserved impact basin on Mercury: Murchie et al., 2008;Fassett et al., 2009), and the circum-Caloris smooth plains that almost entirely surround the basin rim . As an example, Borealis Planitia, the largest contiguous area of smooth plains on Mercury, has an estimated minimum volume of 4 × 10 6 km 3 (Ostrach et al., 2015), which is comparable to the volume of the Siberian Traps large igneous province on Earth (Fedorenko et al., 2000). ...
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Mercury's geological history has been dominated by global contraction caused by secular cooling of the planet's interior. This cooling has had a profound effect on the expression of the planet's volcanism and tectonism, and the expressions of these two surface evolutionary processes are deeply intertwined. Here, we use case studies from the Hokusai quadrangle of Mercury to gain insight into the interplay between Mercury's volcanism and tectonism, which we review throughout this paper. We perform the first crater size–frequency analysis of the southernmost extent of Borealis Planitia, Mercury's largest expanse of volcanic plains, and find that it formed ~3.8–3.7 Ga. We discuss the importance of “intermediate plains”, a widespread unit in the Hokusai quadrangle, as the manifestation of relatively low-volume effusions with an uncertain stratigraphic relationship with Borealis Planitia. Finally, we detail the formation of the Suge Facula pitted ground during the geological history of Rachmaninoff crater, and hypothesise that such textures probably formed more widely on Mercury but have often either been buried by thick lava flows or otherwise obscured. Unanswered questions in this work can be used to drive the next phase of Mercury exploration and research with the arrival of the BepiColombo mission.
... In addition, the smooth plains inside the Rembrandt basin are modified by multiple sets of contractional and extensional tectonic structures, developed both radially and concentrically towards the center of the basin [24,25]. Other major impact craters on Mercury, such as the Caloris basin, display similar pattern and structures [45,67,68]. Therefore, we chose to distinguish two main features: contractional (e.g., thrust faults and wrinkle ridges) and extensional (e.g., grabens). ...
Article
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Planetary geologic maps are usually carried out following a morpho‐stratigraphic approach where morphology is the dominant character guiding the remote sensing image interpretation. On the other hand, on Earth a more comprehensive stratigraphic approach is preferred, using lithology, overlapping relationship, genetic source, and ages as the main discriminants among the different geologic units. In this work we produced two different geologic maps of the Rembrandt basin of Mercury, following the morpho‐stratigraphic methods and symbology adopted by many authors while mapping quadrangles on Mercury, and an integrated geo‐stratigraphic approach, where geologic units were distinguished also on the basis of their false colors (derived by multispectral image data of the NASA MESSENGER mission), subsurface stratigraphic position (inferred by crater excavation) and model ages. We distinguished two different resurfacing events within the Rembrandt basin, after the impact event, and four other smooth plains units outside the basin itself. This provided the basis to estimate thicknesses, volumes, and ages of the smooth plains inside the basin. Results from thickness estimates obtained using different methodologies confirm the presence of two distinct volcanic events inside the Rembrandt basin, with a total thickness ranging between 1–1.5 km. Furthermore, model ages suggest that the volcanic infilling of the Rembrandt basin is among the ones that extended well into the mid‐Calorian period, when Mercury’s effusive volcanism was previously thought to be largely over.
... The Caloris basin is the largest known impact basin on Mercury, with a diameter of 1550 km (Murchie et al., 2008). As seen in Figs. ...
Preprint
The X-Ray Spectrometer (XRS) on the MESSENGER spacecraft provided measurements of major-element ratios across Mercury's surface. We present global maps of Mg/Si, Al/Si, S/Si, Ca/Si, and Fe/Si derived from XRS data collected throughout MESSENGER's orbital mission. We describe the procedures we used to select and filter data and to combine them to make the final maps, which are archived in NASA's Planetary Data System. Areal coverage is variable for the different element-ratio maps, with 100% coverage for Mg/Si and Al/Si, but only 18% coverage for Fe/Si north of 30 $^{\circ}$ N, where the spatial resolution is highest. The spatial resolution is improved over previous maps by 10-15% because of the inclusion of higher-resolution data from late in the mission when the spacecraft periapsis altitude was low. Unlike typical planetary data maps, however, the spatial resolution of the XRS maps can vary from pixel to pixel, and thus care must be taken in interpreting small-scale features. We provide several examples of how the XRS maps can be used to investigate elemental variations in the context of geological features on Mercury, which range in size from single $\sim$100-km-diameter craters to large impact basins. We expect that these maps will provide the basis for and/or contribute to studies of Mercury's origin and geological history for many years to come.