Nature Geoscience

Published by Springer Nature

Online ISSN: 1752-0908

·

Print ISSN: 1752-0894

Articles


Arsenic migration to deep groundwater in Bangladesh influenced by adsorption and water demand
  • Article
  • Full-text available

October 2011

·

365 Reads

·

·

·

[...]

·

Drinking shallow groundwater with naturally elevated concentrations of arsenic is causing widespread disease in many parts of South and Southeast Asia. In the Bengal Basin, growing reliance on deep (>150 m) groundwater has lowered exposure. In the most affected districts of Bangladesh, shallow groundwater concentrations average 100 to 370 μg L(-1), while deep groundwater is typically < 10 μg L(-1). Groundwater flow simulations have suggested that, even when deep pumping is restricted to domestic use, deep groundwater in some areas of the Bengal Basin is at risk of contamination. However, these simulations have neglected the impedance of As migration by adsorption to aquifer sediments. Here we quantify for the first time As sorption on deeper sediments in situ by replicating the intrusion of shallow groundwater through injection of 1,000 L of deep groundwater modified with 200 μg L(-1) of As into a deeper aquifer. Arsenic concentrations in the injected water were reduced by 70% due to adsorption within a single day. Basin-scale modelling indicates that while As adsorption extends the sustainable use of deep groundwater, some areas remain vulnerable; these areas can be prioritized for management and monitoring.
Download
Share

Figure 1: Concentration dependence of MeHg photodegradation rates.a, MeHg degradation by sunlight in water containing Suwannee River humic acid (SRHA) and phosphate (1 mM, pH = 7). The high MeHg treatment (1,500 nM) was exposed in October 2008 (15.2 °C average noon temperature). The low MeHg treatment (15 nM) was exposed in December 2008 (8.9 °C). The error bars represent ±1 s.d. for replicate measurements (n=2–3) of the same sample. b, MeHg degradation by artificial ultraviolet-A (λ = 365 nm) in water containing SRHA (2.8 mg C l−1) and phosphate (10 mM, pH 7.4). The data points represent the average MeHg concentration (±1 s.d.) for duplicate samples.
Figure 2: MeHg degradation through generation of 1O2 from photosensitized humic acid.MeHg was degraded by ultraviolet-A in simulated water containing MeHg (0.5 nM), SRHA (2.8 mg C l−1) and phosphate (10 mM, pH 7.3). a, Replicate samples were amended with either D2O (a singlet-oxygen enhancer), NaN3 or β-carotene (singlet-oxygen quenchers). b, No difference was observed in replicates amended with isoprene (a quencher for triplet-state dissolved NOM) or isopropyl alcohol (quencher for •OH). The error bars represent ±1 s.d. for replicate measurements (n=2–3).
Figure 3: Effect of ligand complexation on degradation of MeHg.a, Singlet-oxygen-induced degradation of MeHg (350 nM) complexed with GSH, MA, Cl− or OH−/HPO42− in water containing 2-chorophenol (40 μM) and phosphate (10 mM, pH=7.3). 1O2 was generated by ultraviolet-A (λ = 365 nm) irradiation of rose bengal. The lines indicate model predictions from rate constants. The error bars represent ±1 s.d.for replicate measurements (n=2–3). b, Direct ultraviolet-C (λ = 254 nm) degradation of MeHg at varying initial ratios of MeHg and GSH (4 μM initial MeHg, 1 mM phosphate, pH 7.4). The solid line indicates a linear regression of data for [GSH]0/[MeHg]0≤1.
Photolytic degradation of methylmercury enhanced by binding to natural organic ligands
Monomethylmercury is a neurotoxin that poses significant risks to human health1 due to its bioaccumulation in food webs. Sunlight degradation to inorganic mercury is an important component of the mercury cycle that maintains methylmercury at low concentrations in natural waters. Rates of photodecomposition, however, can vary drastically between surface waters2-5 for reasons that are largely unknown. Here, we show that photodegradation occurs through singlet oxygen, a highly reactive form of dissolved oxygen generated by sunlight irradiation of dissolved natural organic matter. The kinetics of degradation, however, depended on water constituents that bind methylmercury cations. Relatively fast degradation rates (similar to observations in freshwater lakes) applied only to methylmercury species bound to organic sulfur-containing thiol ligands such as glutathione, mercaptoacetate, and humics. In contrast, methylmercury-chloride complexes, which are dominant in marine systems, were unreactive. Binding by thiols lowered the excitation energy of the carbon-mercury bond on the methylmercury molecule6-7 and subsequently increased reactivity towards bond breakage and decomposition. Our results explain methylmercury photodecomposition rates that are relatively rapid in freshwater lakes2-4 and slow in marine waters5.

Figure 1: Temperature–pressure profiles for worlds in the Solar System with thick atmospheres1, 2, 3, 4, 28. Temperature minima commonly occur around 0.1 bar. Venus has a very weak 0.1 bar tropopause in the global mean (see text). More information regarding data sources is given in the Supplementary Information.
Figure 2: Schematic diagram of thermal structure in a thick planetary atmosphere with a stratospheric inversion. A general feature is a grey infrared optical depth, τ0, of ~ 2–9 at a pressure, p0, of 1 bar. There is a radiative–convective boundary at a scaled infrared optical depth, Dτrc, of about unity or greater. A tropopause temperature minimum occurs at a pressure, ptp, of about 0.1 bar and a scaled infrared optical depth, Dτtp, of about 0.1. The ‘diffusivity factor’ D for the optical depth is ~ 1.66 (see text). The thickened portion of the profile indicates the convective part of the troposphere.
Common 0.1 bar Tropopause in Thick Atmospheres Set by Pressure-Dependent Infrared Transparency

December 2013

·

1,823 Reads

A minimum atmospheric temperature, or tropopause, occurs at a pressure of around 0.1 bar in the atmospheres of Earth, Titan, Jupiter, Saturn, Uranus and Neptune, despite great differences in atmospheric composition, gravity, internal heat and sunlight. In all these bodies, the tropopause separates a stratosphere with a temperature profile that is controlled by the absorption of shortwave solar radiation, from a region below characterised by convection, weather, and clouds. However, it is not obvious why the tropopause occurs at the specific pressure near 0.1 bar. Here we use a physically-based model to demonstrate that, at atmospheric pressures lower than 0.1 bar, transparency to thermal radiation allows shortwave heating to dominate, creating a stratosphere. At higher pressures, atmospheres become opaque to thermal radiation, causing temperatures to increase with depth and convection to ensue. A common dependence of infrared opacity on pressure, arising from the shared physics of molecular absorption, sets the 0.1 bar tropopause. We hypothesize that a tropopause at a pressure of approximately 0.1 bar is characteristic of many thick atmospheres, including exoplanets and exomoons in our galaxy and beyond. Judicious use of this rule could help constrain the atmospheric structure, and thus the surface environments and habitability, of exoplanets.

Figure 2: Upper limits on the atmospheric pressure of early Mars. Comparison of model crater size–frequency distributions to observations. Solid black line corresponds to definite embedded craters. Dashed black line additionally includes rimmed circular mesas. Stair-stepping in the data curves corresponds to individual craters. Coloured lines show model predictions for atmospheric filtering of small impactors at different pressures. Grey hatched regions correspond to 2σ statistical error envelopes around the best-fit palaeopressure to the data (best fits shown by thick grey lines). Survey incompleteness leads to overestimates of median crater size, so best fits are upper limits.
Figure S1. Geologic context for this study. Topographically lower fluvial unit ("F1", no tint) 705 contains large meander belts (cyan outlines). Topographically higher fluvial unit ("F2", white tint) 706 contains many river deposits but lacks large meander belts. F1/F2 contact is shown as a solid blue 707 line where mapped with high confidence, and as a dotted blue line where inferred. Background 708 color is cued to MOLA topography (elevation range ~ 500m). Background image is CTX mosaic; 709 the western rim of Kalba crater is visible at right. DTMs were constructed from HiRISE images 710
Low paleopressure of the Martian atmosphere estimated from the size distribution of ancient craters

April 2014

·

232 Reads

Decay of the CO2-dominated atmosphere is an important component of long-term environmental change on Mars, but direct constraints on paleoatmospheric pressure P are few. Of particular interest is the climate that allowed rivers to flow early in Mars history, which was affected by P via direct and indirect greenhouse effects. The size of craters embedded within ancient layered sediments is a proxy for P: the smaller the minimum-sized craters that form, the thinner the past atmosphere. Here we use high-resolution orthophotos and Digital Terrain Models (DTMs) to identify ancient craters among the river deposits of Aeolis close to Gale crater, and compare their sizes to models of atmospheric filtering of impactors by thicker atmospheres. We obtain an upper limit of P <= 760+/-70 mbar, rising to P <= 1640+/-180 mbar if rimmed circular mesas are excluded. Our work assumes target properties appropriate for desert alluvium: if sediment developed bedrock-like rock-mass strength by early diagenesis, the upper limit increases by a factor of up to 2. If Mars did not have a stable multibar atmosphere at the time that the rivers were flowing, the warm-wet CO2 greenhouse of Pollack et al. (1987) is ruled out, and long-term average temperatures were most likely below freezing.

Layered convection as the origin of Saturn's luminosity anomaly

April 2013

·

135 Reads

As they keep cooling and contracting, Solar System giant planets radiate more energy than they receive from the Sun. Applying the first and second principles of thermodynamics, one can determine their cooling rate, luminosity, and temperature at a given age. Measurements of Saturn's infrared intrinsic luminosity, however, reveal that this planet is significantly brighter than predicted for its age. This excess luminosity is usually attributed to the immiscibility of helium in the hydrogen-rich envelope, leading to "rains" of helium-rich droplets. Existing evolution calculations, however, suggest that the energy released by this sedimentation process may not be sufficient to resolve the puzzle. Here, we demonstrate using planetary evolution models that the presence of layered convection in Saturn's interior, generated, like in some parts of Earth oceans, by the presence of a compositional gradient, significantly reduces its cooling. It can explain the planet's present luminosity for a wide range of configurations without invoking any additional source of energy. This suggests a revision of the conventional homogeneous adiabatic interior paradigm for giant planets, and questions our ability to assess their heavy element content. This reinforces the possibility for layered convection to help explaining the anomalously large observed radii of extrasolar giant planets.

Figure 1: Compton–Belkovich thorium anomaly. The location of the CBTA is northeast of Humboldtianum basin and just beyond the Moon’s eastern limb (LP–GRS 0.5°, ~15 km resolution Th data1, 2 as deconvolved by Lawrence et al. 3, overlain on WAC 400 m per pixel base). The highest measured Th intensity corresponds to a concentration at this resolution of ~10 ppm at the centre of the Th hotspot.
Figure 2: Geomorphology of the CBF. a, Portion of WAC image showing high-reflectance terrain. Dashed outline denotes the topographically elevated area (). b, NAC mosaic showing the central region of the CBF and location of features discussed in text. Arrows indicate arcuate escarpments; double arrow locates the elongate rock body referred to in the text and  as ‘middle dome.’ Numbers 1 and 2 locate corresponding areas on parts b and c, 1, 2, and 3 correspond to irregular depressions (see text). c, Digital terrain model of the area noted in part a. d, Arcuate escarpment along the western side of the central depression. e, Small dome.
Figure 3: Topography of the CBF. a, WAC DTM (200 m per pixel, draped over WAC orthophoto, 100 m per pixel). b, Elevation profiles for sections a–a′ and b–b′ generated from the WAC DTM.
Figure 4: Domes in the CBF. Positive relief features in the CBF inferred to be volcanic in origin.
Non-mare silicic volcanism on the lunar farside at Compton–Belkovich

July 2011

·

702 Reads

Non-basaltic volcanism is rare on the Moon. The best known examples occur on the lunar nearside in the compositionally evolved Procellarum KREEP terrane. However, there is an isolated thorium-rich area—the Compton–Belkovich thorium anomaly—on the lunar farside for which the origin is enigmatic. Here we use images from the Lunar Reconnaissance Orbiter Cameras, digital terrain models and spectral data from the Diviner lunar radiometer to assess the morphology and composition of this region. We identify a central feature, 25 by 35 km across, that is characterized by elevated topography and relatively high reflectance. The topography includes a series of domes that range from less than 1 km to more than 6 km across, some with steeply sloping sides. We interpret these as volcanic domes formed from viscous lava. We also observe arcuate to irregular circular depressions, which we suggest result from collapse associated with volcanism. We find that the volcanic feature is also enriched in silica or alkali-feldspar, indicative of compositionally evolved, rhyolitic volcanic materials. We suggest that the Compton–Belkovich thorium anomaly represents a rare occurrence of non-basaltic volcanism on the lunar farside. We conclude that compositionally evolved volcanism did occur far removed from the Procellarum KREEP terrane.

Figure 3: Storm impact on the resultant drift direction (RDD). (a) The RDD as a function of the storm frequency per equinox with a saltation threshold of 0.04 m/s, using GCM winds (black solid line) or GCM winds with increased gust (black dashed line). Angles are measured anti-clockwise from the East (i.e.-180 • is westward,-90 • is southward and 0 • is eastward). The red line symbolizes the passage from westward to eastward dune growth. (b) Map dune orientation observed with Cassini's radar 29 (red) and map of RDD obtained with the GCM (with increased gust) for low latitudes with a threshold of 0.04 m/s and no storm effect (black). (c) is same as (b) but with the impact of two storms per Titan year. 
Figure 4: Analogy between linear dunes on Titan and in Rub'al-Kali desert on Earth. (a) denoised image of Titan's dunes from Cassini's radar SAR (see Supplementary Information). The inset shows the sand flux rose similar to Fig. 3b, but calculated at 7.5 • S and averaging the effect of Saturn's eccentricity. (b) longitudinal dunes in Rub'al-Kali desert (18 • N, 48 • E) with the sand flux roses calculated from winds at 10 m. For both images, the arrow corresponds to the resultant drift direction calculated with the sand flux rose. 
Figure 8: Threshold friction speed for saltation as a function of the particle diameter. The saltation speed has been calculated using relation (3) for Titan's conditions 21 , with a sediment density of 1000 kg/m 3 and a parameter γ=1.6×10 −4 N/m. 
Figure 9: Sand flux roses obtained by combining the GCM winds with winds produced during one typical gust front every equinox. The arrows correspond to the resultant drift directions. a, b and c correspond to 0 • , 10 • and 20 • N latitudes, respectively, with GCM winds (speed increased by 20 %) and a threshold of 0.04 m/s, and averaging the effect of Saturn's eccentricity. 
Figure 10: Longitudinal dunes in Egypt and Algeria. Map data: Google. (a) Dune field in Egypt (25.5 • N, 26.25 • E) with the sand flux roses calculated from winds at 10 m. (b) Dune field in Algeria (29.5 • N, 5.5 • E). The arrow corresponds to the resultant drift direction calculated with the sand flux rose. 
Methane storms control Titan's dune orientation

April 2015

·

478 Reads

Titan's equatorial regions are covered by eastward propagating linear dunes. This direction is opposite to mean surface winds simulated by Global Climate Models (GCMs), which are oriented westward at these latitudes, similar to trade winds on Earth. Different hypotheses have been proposed to address this apparent contradiction, involving Saturn's gravitational tides, large scale topography or wind statistics, but none of them can explain a global eastward dune propagation in the equatorial band. Here we analyse the impact of equinoctial tropical methane storms developing in the superrotating atmosphere (i.e. the eastward winds at high altitude) on Titan's dune orientation. Using mesoscale simulations of convective methane clouds with a GCM wind profile featuring superrotation, we show that Titan's storms should produce fast eastward gust fronts above the surface. Such gusts dominate the aeolian transport, allowing dunes to extend eastward. This analysis therefore suggests a coupling between superrotation, tropical methane storms and dune formation on Titan. Furthermore, together with GCM predictions and analogies to some terrestrial dune fields, this work provides a general framework explaining several major features of Titan's dunes: linear shape, eastward propagation and poleward divergence, and implies an equatorial origin of Titan's dune sand.

Figure 2 Correlation coefficient for a linear correlation between the 14 C production rate from the floating tree-ring record and the climate-corrected 10 Be flux to Summit. The best agreement is obtained when the floating tree-ring record ends at an age of 12,500 yr BP.
Figure 3 Comparison of tree-ring-based 14 C ages versus calendar ages with several independent calibration records. (i) Tree-ring-based 14 C ages versus calendar ages; (ii)-(vii) independent calibration records, which are from the Cariaco basin 13 (ii), from Lake Gosciaz and Lake Perespilno 20 (data were averaged into 100 yr bins) (iii), from stalagmites from the Bahamas 47 (iv), from corals from Tahiti and Barbados 48 (v), from Lake Suigetsu in Japan 49 (vi) and from pristine corals 38 (measurements on the same sample are averaged) (vii), including the 1σ errors. The marine records have been corrected for an assumed constant reservoir age. The bar above the tree-ring chronology shows the error in the age determination due to uncertainties in the ice-core dating.
Figure 4 Modelled and measured 14 C and δ 18 O during the YD. (i) The tree-ring 14 C data compared with the 10 Be-based 14 C calculated under the assumption of a constant carbon cycle. (ii) The results where we assumed a 30%-decreased ocean ventilation (ocean diffusion constant) during the YD (red line in (iii)). (iii) δ 18 O from the GRIP ice core. The data are plotted on the GICC05 timescale after subtracting a constant offset of 65 yr. Monte Carlo simulations were carried out to assess the error (1σ) of the modelled 14 C record.
Tree rings and ice cores reveal 14C calibration uncertainties during the Younger Dryas

March 2008

·

582 Reads

The Younger Dryas interval during the Last Glacial Termination was an abrupt return to glacial-like conditions punctuating the transition to a warmer, interglacial climate. Despite recent advances in the layer counting of ice-core records of the termination, the timing and length of the Younger Dryas remain controversial. Also, a steep rise in the concentration of atmospheric radiocarbon at the onset of the interval, recorded primarily in the Cariaco Basin, has been difficult to reconcile with simulations of the Younger Dryas carbon cycle. Here we discuss a radiocarbon chronology from a tree-ring record covering the Late Glacial period that has not been absolutely dated. We correlate the chronology to ice-core timescales using the common cosmic production signal in tree-ring 14C and ice-core 10Be concentrations. The results of this correlation suggest that the Cariaco record may be biased by changes in the concentration of radiocarbon in the upper ocean during the early phase of the Younger Dryas climate reversal in the Cariaco basin. This bias in the marine record may also affect the accuracy of a widely used radiocarbon calibration curve over this interval. Our tree-ring-based radiocarbon record is easily reconciled with simulated production rates and carbon-cycle changes associated with reduced ocean ventilation during the Younger Dryas.

Southern Ocean source of 14C-depleted carbon in the North Pacific Ocean during the last deglaciation

October 2010

·

148 Reads

During the last deglaciation, atmospheric carbon dioxide concentrations rose at the same time that the Delta14C of that CO2 fell. This has been attributed to the release of 14C-depleted carbon dioxide from the deep ocean, possibly vented through the Southern Ocean. Recently, a sediment record from the eastern North Pacific Ocean spanning the last deglaciation was interpreted to reflect transport of such radiocarbon-depleted CO2 from the Southern Ocean through Antarctic Intermediate Water. However, the suggestion that the record reflects intermediate water derived from the Southern Ocean remains controversial. Here we assess the source of the deglacial intermediate water by measuring the neodymium isotopes of fossil fish teeth/debris from the same eastern North Pacific core used in the earlier study. The isotopic signature of a water mass, which is captured in the fossil fish teeth, reflects the location in which it formed. Our data exhibit a clear shift in the neodymium isotope values towards Southern Ocean values about 18,000 years ago, coinciding with the negative Delta14C excursion. We conclude that these data support a Southern Ocean source for the deglacial radiocarbon-depleted CO2 detected in the eastern North Pacific.

Surface-temperature trends and variability in the low-latitude North Atlantic since 1552

June 2009

·

420 Reads

Sea surface temperature variability in the North Atlantic Ocean recorded since about 1850 has been ascribed to a natural multidecadal oscillation superimposed on a background warming trend1-6. It has been suggested that the multidecadal variability may be a persistent feature6-8, raising the possibility that the associated climate impacts may be predictable7,8. owever, our understanding of the multidecadal ocean variability before the instrumental record is based on interpretations of high-latitude terrestrial proxy records. Here we present an absolutely dated and annually resolved record of sea surface temperature from the Bahamas, based on a 440-year time series of coral growth rates. The reconstruction indicates that temperatures were as warm as today from about 1552 to 1570, then cooled by about 1° C from 1650 to 1730 before warming until the present. Our estimates of background variability suggest that much of the warming since 1900 was driven by anthropogenic forcing. Interdecadal variability with a period of 15-25 years is superimposed on most of the record, but multidecadal variability becomes significant only after 1730. We conclude that the multidecadal variability in sea surface temperatures in the low-latitude western Atlantic Ocean may not be persistent, potentially making accurate decadal climate forecasts more difficult to achieve.

Figure 1: Climate records from the North Atlantic region.a, Instrumental record of the NAO (ref. 1) annually (grey) and 5 year running mean (black). b, Three year averaged coral winter SST from Sr/Ca (grey) and instrumental data (black) (HadISST (ref. 35)) versus time. Three year averages are shown, as this is the shortest time period of coherence between the winter coral Sr/Ca and the instrumental NAO. A significant coherence (>95%) is found between the winter coral Sr/Ca and SST (r=0.44, p=0.0030, n=43). c, A multiproxy record of Northern Hemisphere surface temperature anomalies24—annually (grey) and 5 year running mean (black).
Figure 2: Spectral analysis of regional records.a, The spectral coherence (r) (solid) between the negative of the winter Sr/Ca and the NAO instrumental records, including the 95% confidence (dashed), from 1864 to 1999 (the full length of the NAO record). b, The phase relationship between the Sr/Ca and NAOI records (solid black), including error calculation (solid grey), surrounding periods of significant coherence. c, Spectral results of the NAOI (solid black), SST (solid grey) and Sr/Ca (dashed) from 1871 to 1999, the duration of HadISST, which is the shortest record. The error bar represents 90% confidence.
Figure 3: NAOI records and wavelet analysis.a, Records of the NAOI combining periodicities of 20–100 years and 3–5 years from coral Sr/Ca (red), instrumental1 (dark blue) and terrestrial7 (light blue) data. b, 3–5 year band-pass filter of Sr/Ca, instrumental and terrestrial data. c, Square root of the variance in spectral power over a 3–5 year frequency band for coral Sr/Ca and for terrestrial data. d, 20–100 year band-pass filter of Sr/Ca, instrumental and terrestrial data. e, Square root of the variance in spectral power over a 20–50 year frequency band for coral Sr/Ca and for terrestrial data7.
Increased multidecadal variability of the North Atlantic Oscillation since 1781

November 2008

·

455 Reads

The North Atlantic Oscillation is a meridional oscillation of atmospheric mass measured between Iceland and the Açores, which drives winter climate variability in eastern North America and Europe. A prolonged period of the positive phase during the 1990s led to the suggestion that anthropogenic warming was affecting the behaviour of the North Atlantic Oscillation. However, instrumental records are too short to compare observations during periods of extended warm and cold hemispheric temperatures, and existing palaeoclimate reconstructions primarily capture terrestrial variability. Here we present a record of Sr/Ca, a sea surface temperature proxy, from a Bermuda coral from 1781 to 1999. We use this monthly resolved record to reconstruct past variability of the North Atlantic Oscillation at multiple frequencies. Our record shows enhanced multidecadal scale variability during the late twentieth century compared with the end of the Little Ice Age (1800-1850). We suggest that variability within the North Atlantic Oscillation is linked to the mean temperature of the Northern Hemisphere, which must be considered in any long-term predictions.

Figure 3: Vertical motions produced by the 1 April 2007 earthquake.Red circles indicate uplift; blue circles indicate subsidence; size is scaled to the amount of vertical displacement. The star is the US Geological Survey epicentre for the 1 April main shock; the beachball indicates the centroid moment tensor focal mechanism and centroid location27. The inset compares vertical motions along a transect A–A' with motions calculated for 5 m slip along the rectangular fault in .
Rupture across arc segment and plate boundaries in the 1 April 2007 Solomons earthquake

March 2008

·

304 Reads

The largest earthquakes are generated in subduction zones, and the earthquake rupture typically extends for hundreds of kilometres along a single subducting plate. These ruptures often begin or end at structural boundaries on the overriding plate that are associated with the subduction of prominent bathymetric features of the downgoing plate. Here, we determine uplift and subsidence along shorelines for the 1 April 2007 moment magnitude MW 8.1 earthquake in the western Solomon Islands, using coral microatolls which provide precise measurements of vertical motions in locations where instrumental data are unavailable. We demonstrate that the 2007 earthquake ruptured across the subducting Simbo ridge transform and thus broke through a triple junction where the Australian and Woodlark plates subduct beneath the overriding Pacific plate. Previously, no known major megathrust rupture has involved two subducting plates. We conclude that this event illustrates the uncertainties of predicting the segmentation of subduction zone rupture on the basis of structural discontinuities.

Erratum : Climate and human influences on global biomass burning over the past two millennia (Nature Geoscience (2009) 1:697-702)

September 2008

·

469 Reads

Large, well-documented wildfires have recently generated worldwide attention, and raised concerns about the impacts of humans and climate change on wildfire regimes. However, comparatively little is known about the patterns and driving forces of global fire activity before the twentieth century. Here we compile sedimentary charcoal records spanning six continents to document trends in both natural and anthropogenic biomass burning for the past two millennia. We find that global biomass burning declined from AD 1 to 1750, before rising sharply between 1750 and 1870. Global burning then declined abruptly after 1870. The early decline in biomass burning occurred in concert with a global cooling trend and despite a rise in the human population. We suggest the subsequent rise was linked to increasing human influences, such as population growth and land-use changes. Our compilation suggests that the final decline occurred despite increasing air temperatures and population. We attribute this reduction in the amount of biomass burned over the past 150 years to the global expansion of intensive grazing, agriculture and fire management.

Stress transfer in the Tokai subduction zone from the 2009 Suruga Bay earthquake in Japan

June 2010

·

105 Reads

Southwestern Japan lies at the boundary between the subducting Philippine Sea plate and the overriding Eurasian plate. A magnitude 8 megathrust earthquake ruptured the Tonankai and Nankai segments in 1944 and 1946, respectively, but the neighbouring Tokai segment of the plate boundary remained locked1. A large megathrust earthquake in the Tokai region has therefore been expected. In 2009, a magnitude 6.4 earthquake took place in Suruga Bay, within the Philippine Sea subducting plate, close to the Tokai segment. Here, we use a fault-slip model to examine the impact of the stress changes2 caused by the Suruga Bay event on the Tokai segment. We show that the occurrence rate of plate-boundary seismicity increased following the earthquake. Most of the presumed strongly locked patches of the Tokai segment are located within areas of increased stress. Rupturing of a locked patch—following a threshold level of seismic stress—could trigger the rupture of the entire Tokai segment, leading to a megathrust earthquake.

Table 1 | Magma-intrusion time sequence.
Figure 3: Time series and spectrograms of April 2011 earthquake swarm. a, Spectrogram of OBH-E record from 2 to 20 April 2011, overlain with r.m.s. amplitude of the OBH (black line) and centre caldera BPR (red line). r.m.s. values are calculated in the 0.1–125 Hz band from one-minute windows. Broadband energy and r.m.s. peaks mark earthquake-swarm onset. Short-duration, broadband signals are periods of strong volcanic tremor. b, OBH record and spectrogram of typical Axial Seamount earthquake showing first arrival phase and multiple seafloor and surface reflections30. c, Spectrogram from 15 April showing detail of tremor episodes T1 and T2.
Seismic precursors and magma ascent before the April 2011 eruption at Axial Seamount

June 2012

·

325 Reads

Volcanoes at spreading centres on land often exhibit seismicity and ground inflation months to years before an eruption, caused by a gradual influx of magma to the source reservoir. Deflation and seismicity can occur on time scales of hours to days, and result from the injection of magma into adjacent rift zones. Volcanoes at submarine rift zones, such as Axial Seamount in the northeast Pacific Ocean, have exhibited similar behaviour, but a direct link between seismicity, seafloor deformation and magma intrusion has never been demonstrated. Here we present recordings from ocean-bottom hydrophones and an established array of bottom-pressure recorders that reveal patterns of both microearthquakes and seafloor deformation at Axial Seamount on the Juan de Fuca Ridge, before it erupted in April 2011. Our observations show that the rate of seismicity increased steadily during a period of several years, leading up to an intrusion and eruption of magma that began on 6 April 2011. We also detected a sudden increase in seismo-acoustic energy about 2.6h before the eruption began. Our data indicate that access to real-time seismic data, projected to be available in the near future, might facilitate short-term forecasting and provide sufficient lead-time to prepare in situ instrumentation before future intrusion and eruption events.

Boe J, Hall A, Qu X.. September sea-ice cover in the Arctic Ocean projected to vanish by 2100. Nature Geosci 2: 341-343

March 2009

·

443 Reads

The Arctic climate is changing rapidly(1). From 1979 to 2006, September sea-ice extent decreased by almost 25% or about 100,000 km(2) per year (ref. 2). In September 2007, Arctic sea-ice extent reached its lowest level since satellite observations began(3) and in September 2008, sea-ice cover was still low. This development has raised concerns that the Arctic Ocean could be ice-free in late summer in only a few decades, with important economic and geopolitical implications. Unfortunately, most current climate models underestimate significantly the observed trend in Arctic sea-ice decline(4), leading to doubts regarding their projections for the timing of ice-free conditions. Here we analyse the simulated trends in past sea-ice cover in 18 state-of-art-climate models and find a direct relationship between the simulated evolution of September sea-ice cover over the twenty-first century and the magnitude of past trends in sea-ice cover. Using this relationship together with observed trends, we project the evolution of September sea-ice cover over the twenty-first century. We find that under a scenario with medium future greenhouse-gas emissions, the Arctic Ocean will probably be ice-free in September before the end of the twenty-first century.

Submarine groundwater discharge revealed by 228Ra distribution in the upper Atlantic Ocean

April 2008

·

252 Reads

Submarine groundwater discharge is defined as any flow of water at continental margins from the seabed to the coastal ocean, regardless of fluid composition or driving force1. The flux of submarine groundwater discharge has been hypothesized to be a pathway for enriching coastal waters in nutrients, carbon and metals2. Here, we estimate the submarine groundwater flux from the inventory of 228Ra in the upper Atlantic Ocean, obtained by interpolating measurements at over 150 stations. Only 46% of the loss in 228Ra from radioactive decay is replenished by input from dust, rivers and coastal sediments. We infer that the remainder must come from submarine groundwater discharge. Using estimates of 228Ra concentrations in submarine groundwater discharge, we arrive at a total flux from submarine groundwater discharge of 2–41013 m3 yr- 1, between 80 and 160% of the amount of freshwater entering the Atlantic Ocean from rivers. Submarine groundwater discharge is not a freshwater flux, but a flux of terrestrial and sea water that has penetrated permeable coastal sediments. Our assessment of the volume of submarine groundwater discharge confirms that this flux represents an important vehicle for the delivery of nutrients, carbon and metal to the ocean.

Bell, R. E. The role of subglacial water in ice-sheet mass balance. Nature Geosci. 1, 297-304

April 2008

·

347 Reads

In the coming decades, significant changes in the polar regions will increase the contribution of ice sheets to global sea-level rise. Under the ice streams and outlet glaciers that deliver ice to the oceans, water and deformable wet sediments lubricate the base, facilitating fast ice flow. The influence of subglacial water on fast ice flow depends on the geometry and capacity of the subglacial hydrologic system: water moving rapidly through a well-connected system of conduits or channels will have little impact on ice-sheet velocities, but water injected into a spatially dispersed subglacial system may reduce the effective pressure at the base of the ice sheet, and thereby trigger increased ice-sheet velocities. In Greenland, the form of the subglacial hydrologic system encountered by increasing surface melt water will determine the influence of changing atmospheric conditions on ice-sheet mass balance. In Antarctica, subglacial lakes have the capacity to both modulate velocities in ice streams and outlet glaciers and provide nucleation points for new fast ice-flow tributaries. Climate models of ice-sheet responses to global change remain incomplete without a parameterization of subglacial hydrodynamics and ice dynamics.

Figure 4: Spatial relationships between microfossils and pyrite (SP9D2a–b, SPV3b). a, Partial microfossil walls (black arrows) intermixed with pyrite coating quartz grains. Pyrite (right image, white) occurs as 1–10 μm grains exterior to the microfossils and as nano-grains within microfossil walls (white arrows). b, TEM images of a partial microfossil wall showing pyrite occurring as sub-micrometre grains within and adjacent to the wall. c, NanoSIMS maps of nitrogen (26CN−) and sulphur (32S−) showing a putative spheroidal microfossil (arrow) associated with micrometre-sized pyrite. d, Spheroidal microfossil associated with pyrite (P), exhibiting a partially preserved ‘double wall’ and putative expulsion of cellular contents (arrow).
Microfossils of sulphur-metabolizing cells in 3.4-billion-year-old rocks of Western Australia

August 2011

·

1,344 Reads

Sulphur isotope data from early Archaean rocks suggest that microbes with metabolisms based on sulphur existed almost 3.5 billion years ago, leading to suggestions that the earliest microbial ecosystems were sulphur-based. However, morphological evidence for these sulphur-metabolizing bacteria has been elusive. Here we report the presence of microstructures from the 3.4-billion-year-old Strelley Pool Formation in Western Australia that are associated with micrometre-sized pyrite crystals. The microstructures we identify exhibit indicators of biological affinity, including hollow cell lumens, carbonaceous cell walls enriched in nitrogen, taphonomic degradation, organization into chains and clusters, and delta13C values of -33 to -460/00 Vienna PeeDee Belemnite (VPDB). We therefore identify them as microfossils of spheroidal and ellipsoidal cells and tubular sheaths demonstrating the organization of multiple cells. The associated pyrite crystals have Delta33S values between -1.65 and +1.430/00 and delta34S values ranging from -12 to +60/00 Vienna Canyon Diablo Troilite (VCDT). We interpret the pyrite crystals as the metabolic by-products of these cells, which would have employed sulphate-reduction and sulphur-disproportionation pathways. These microfossils are about 200 million years older than previously described microfossils from Palaeoarchaean siliciclastic environments.

Figure 4: Tsunami calculation.a–d, Heights of the sea surface at 4, 30, 70 and 90 min after the earthquake. The direct wave travels to the North African coast and into the Adriatic, consistent with the historical record. e, A schematic map of Alexandria at the time of the AD 365 earthquake. The Island of Pharos was connected to the mainland by a narrow causeway, known as the Heptastadion, which was overtopped by the tsunami. Our calculations show that the wave would have arrived from the southwest (white arrow), explaining how the Heptastadion was inundated despite the apparent protection offered by Pharos Island against a direct wave from Crete, to the northwest. f, A plot of the wave height against time that would be observed in the open ocean off Alexandria in water of 20 m depth. The wave height would have been greatly amplified during run-up through shallower water towards the city.
Figure 5: Schematic diagram of tectonic setting of the AD 365 earthquake.a, Continuous GPS data show shortening of 1 mm yr-1 between Chrisoskalitissa (C) and Anopoli (A) in southern Crete and Milos (M) and Santorini (S), 200 km to the northeast. b, Southwestward speed, calculated from model illustrated in c, of points within the Aegean, relative to the Mediterranean Ridge. c, Distribution of shear stresses calculated15 for a planar fault, representing the interface between the African plate and the Aegean lithosphere, that slips 4 mm yr-1 more rapidly beneath 70 km (open line) than above 45 km (red line), with the slip varying linearly between those two depths (blue line). Relative values of shear stress are shown by the colour bar; absolute values, at any particular time, depend linearly on the slip difference that has accumulated between the two fault segments.
Eastern Mediterranean tectonics and tsunami hazard inferred from the AD 365 earthquake

March 2008

·

954 Reads

Historical accounts describe an earthquake and tsunami on 21 July AD 365 that destroyed cities and drowned thousands of people in coastal regions from the Nile Delta to modern-day Dubrovnik. The location and tectonic setting of this earthquake have been uncertain until now. Here, we present evidence from radiocarbon data and field observations that western Crete was lifted above sea level, by up to 10 m, synchronously with the AD 365 earthquake. The distribution of uplift, combined with observations of present-day seismicity, suggest that this earthquake occurred not on the subduction interface beneath Crete, but on a fault dipping at about 30° within the overriding plate. Calculations of tsunami propagation show that the uplift of the sea floor associated with such an earthquake would have generated a damaging tsunami through much of the eastern Mediterranean. Measurement of the present rate of crustal shortening near Crete yields an estimate of 5,000 yr for the repeat time of tsunamigenic events on this single fault in western Crete, but if the same process takes place along the entire Hellenic subduction zone, such events may occur approximately once every 800 yr.

Avis CA, Weaver AJ, Meissner KJ.. Reduction in areal extent of high-latitude wetlands in response to permafrost thaw. Nat Geosci 4: 444-448

June 2011

·

216 Reads

Wetlands are vegetated regions that are inundated with water on a permanent, seasonal or intermittent basis. These ecosystems play an important role in the carbon cycle: wetlands take up and store carbon, and release carbon dioxide and methane through the decomposition of organic matter. More than 50% of wetlands are located in the high northern latitudes, where permafrost also prevails and exerts a strong control on wetland hydrology. Permafrost degradation is linked to changes in Arctic lakes: between 1973 and 2004 the abundance of lakes increased in continuous permafrost zones, but decreased in other zones. Here, we use a global climate model to examine the influence of permafrost thaw on the prevalence of high-latitude northern wetlands, under four emissions scenarios. We show that as permafrost degrades, the areal extent of wetlands declines; we found a net loss in wetland extent in the three highest emissions scenarios. We also note an initial increase in the number of days of the year conducive to wetland formation, owing to an increase in unfrozen surface moisture resulting from a lengthening of the thaw season. This is followed by a dramatic decline in the number of wetland-conducive days, owing to a deepening of the permafrost surface, and drainage of near-surface moisture to deeper soil layers. We suggest that a reduction in the areal extent and duration of wetlands will influence high-latitude carbon emissions.

Figure 2 Relation between amplifying feedbacks f and climate sensitivity S. A truncated normal distribution with a mean of 0.65 and standard deviation of 0.13 for the feedback f (solid blue line) is assumed here for illustration. These values are typical for the current set of GCMs 8,33. Because f is substantially positive and the relation between f and S is nonlinear (black line, equation (2)), this leads to a skewed distribution in S (solid red line) with the characteristic long tail seen in most studies. Horizontal and vertical lines mark 5-95% ranges. A decrease in the uncertainty of f by 30% (dashed blue line) decreases the range of S, but the skewness remains (dashed red line). The uncertainty in the tail of S depends not only on the uncertainty in f but also on the mean value of f. Note that the assumption of a linear feedback (equation (1)) is not valid for f near unity. Feedbacks of 1 or more would imply unphysical, catastrophic runaway effects. (Modifi ed from ref. 8.)
Figure 4 The observed global warming provides only a weak constraint on climate sensitivity. A climate model of intermediate complexity 3 , forced with anthropogenic and natural radiative forcing, is used to simulate global temperature with a low climate sensitivity and a high total forcing over the twentieth century (2 °C, 2.5 W m −2 in the year 2000; blue line) and with a high climate sensitivity and low total forcing (6 °C, 1.4 W m −2 ; red line). Both cases (selected for illustration from a large ensemble) agree similarly well with the observed warming (HadCRUT3v; black line) over the instrumental period (inset), but show very different long-term warming for SRES scenario A2 (ref. 101). For simplicity, ocean parameters are kept constant here.
Figure 6 Allowed emissions for a stabilization of atmospheric CO 2 at 450 p.p.m. as shown in Fig. 5. Emission reductions needed for stabilization at 450 p.p.m. (red) must be much larger than in any of the illustrative SRES scenarios (blue lines). The best guess (red line) is based on a climate sensitivity of 3.2 °C and standard carbon cycle settings in a climate model of intermediate complexity 99. Uncertainties in emission reduction (red band) are quantifi ed by combining a low climate sensitivity (1.5 °C) with a fast carbon cycle and a high climate sensitivity (4.5 °C) with a slow carbon cycle. The emission pathway over the next few decades for stabilization at low levels is not strongly affected by the uncertainty in climate sensitivity. Accounting for non-CO 2 forcings requires even lower emissions than shown here to reach the same equivalent radiative forcing target. (Modifi ed from ref. 99.)
Knutti, R. & Hegerl, G. C. The equilibrium sensitivity of the Earth's temperature to radiation changes. Nature Geosci. 1, 735-743

October 2008

·

3,356 Reads

The Earth's climate is changing rapidly as a result of anthropogenic carbon emissions, and damaging impacts are expected to increase with warming. To prevent these and limit long-term global surface warming to, for example, 2 °C, a level of stabilization or of peak atmospheric CO2 concentrations needs to be set. Climate sensitivity, the global equilibrium surface warming after a doubling of atmospheric CO2 concentration, can help with the translation of atmospheric CO2 levels to warming. Various observations favour a climate sensitivity value of about 3 °C, with a likely range of about 2–4.5 °C. However, the physics of the response and uncertainties in forcing lead to fundamental difficulties in ruling out higher values. The quest to determine climate sensitivity has now been going on for decades, with disturbingly little progress in narrowing the large uncertainty range. However, in the process, fascinating new insights into the climate system and into policy aspects regarding mitigation have been gained. The well-constrained lower limit of climate sensitivity and the transient rate of warming already provide useful information for policy makers. But the upper limit of climate sensitivity will be more difficult to quantify.

Figure 3: 13C NMR projections from 2D 1H–13C spectra of humic extracts from the warmed and control soil.The projection shows only protonated carbons, which enables the increase in alkyl carbon (mainly from cuticle, red arrow) in the warmed soil humic material and the decrease of methoxy carbon (from lignin, black arrow) to be easily visualized. DMSO: dimethylsulphoxide.
Feng X, Simpson A, Wilson K, WD D, Simpson M.. Increased cuticular carbon sequestration and lignin oxidation in response to soil warming. Nat Geosci 1: 836-839

November 2008

·

1,462 Reads

Rising temperatures are predicted to accelerate the decomposition of labile soil organic compounds such as proteins and carbohydrates, whereas biochemically resistant compounds, such as lipids from leaf cuticles and roots and lignin from woody tissues, are expected to remain stable on decadal to centennial timescales. However, the extent to which soil warming changes the molecular composition of soil organic matter is poorly understood. Here we examine the impact of soil warming in a mixed temperate forest on the molecular make-up of soil organic matter. We show that the abundance of leaf-cuticle-derived compounds is increased following 14 months of soil warming; we confirm this with nuclear magnetic resonance spectra of soil organic matter extracts. In contrast, we find that the abundance of lignin-derived compounds is decreased after the same treatment, while soil fungi, the primary decomposers of lignin in soil, increase in abundance. We conclude that future warming could alter the composition of soil organic matter at the molecular level, accelerating lignin degradation and increasing leaf-cuticle-derived carbon sequestration. With annual litterfall predicted to increase in the world's major forests with a 3C warming, we suggest that future warming may enhance the sequestration of cuticular carbon in soil.

Figure 3: Changes in the monsoonal rains.Zonally averaged precipitation over the Sahel and Gulf of Guinea (the square in the inset in a) between the water-hosing and control runs. a, Monthly mean precipitation change during the 60 year model simulation, showing a drastic increase of the summer monsoon rainfall south of 5° N about 20–25 years into the simulation following the onset of the equatorial warming (d). The red (blue) shading denotes an increase (a decrease) of precipitation in a range between 0.5 m yr-1 and 3.5 m yr-1. b, Fractional change of the precipitation annual cycle during the first 20 years of the simulation. c, The same fractional change during the last 20 years. The fractional change is defined as the precipitation difference between the two runs divided by the precipitation of the control run.
LETTERS Oceanic link between abrupt changes in the North Atlantic Ocean and the African monsoon

May 2008

·

295 Reads

Abrupt changes in the African monsoon can have pronounced socioeconomic impacts on many West African countries. Evidence for both prolonged humid periods and monsoon failures have been identified throughout the late Pleistocene and early Holocene epochs 1,2. In particular, drought conditions in West Africa have occurred during periods of reduced North Atlantic thermohaline circulation, such as the Younger Dryas cold event 1. Here, we use an ocean–atmosphere general circulation model to examine the link between oceanographic changes in the North Atlantic Ocean and changes in the strength of the African monsoon. Our simulations show that when North Atlantic thermohaline circulation is substantially weakened, the flow of the subsurface North Brazil Current reverses. This leads to decreased upper tropical ocean stratification and warmer sea surface temperatures in the equatorial South Atlantic Ocean

Figure 1 | The gas hydrate volume fraction (V frac,h ≡ S h φ) with respect to depth below the sea floor at different seafloor temperatures T sf (Case I). D sf = 2.0 km. The total gas hydrate volume per unit seafloor area (V h , in m 3 m −2 ) is given for each curve. For the parameters see Supplementary Table S2. Note that changes in V h are not straightforward because temperature impacts multiple parameters (Supplementary Table S2).
Figure 2 | Methane production profiles with respect to depth below the sea floor at different seafloor temperatures (Case I). D sf = 2.0 km. The effects of higher organic carbon input and elevated methanogenesis rates at higher sediment temperatures have been included. The black bars show the base of the GHSZ for each T sf. The parameters (Supplementary Table S2) are the same as those in Fig. 1.
Figure 3 | Contour plots showing the ratio of total hydrate volume at 
Abundant Early Palaeogene marine gas hydrates despite warm deep-ocean temperatures

November 2011

·

227 Reads

Abrupt periods of global warming between 57 and 50 million years ago--known as the Early Palaeogene hyperthermal events--were associated with the repeated injection of massive amounts of carbon into the atmosphere. The release of methane from the sea floor following the dissociation of gas hydrates is often invoked as a source. However, seafloor temperatures before the events were at least 4-7°C higher than today, which would have limited the area of sea floor suitable for hosting gas hydrates. Palaeogene gas hydrate reservoirs may therefore not have been sufficient to provide a significant fraction of the carbon released. Here we use numerical simulations of gas hydrate accumulation at Palaeogene seafloor temperatures to show that near-present-day values of gas hydrates could have been hosted in the Palaeogene. Our simulations show that warmer temperatures during the Palaeogene would have enhanced the amount of organic carbon reaching the sea floor as well as the rate of methanogenesis. We find that under plausible temperature and pressure conditions, the abundance of gas hydrates would be similar or higher in the Palaeogene than at present. We conclude that methane hydrates could have been an important source of carbon during the Palaeogene hyperthermal events.

Figure 1: Location of the GPS transect on the western margin of the GrIS.The four GPS sites are located in the ablation zone of the GrIS across an altitudinal range of 395–1,060 m a.s.l., contours show altitude where ice thickness ranges from ~270–920 m (ref. 29) and are located along a flowline from the ice sheet interior as determined by interferometric synthetic aperture radar observations30. Simultaneous measurements of air temperature were made at each site to constrain surface melt rates.
Figure 2: Seasonal development of melt-induced ice velocity variations.a–d, 24-h horizontal velocity (blue) and surface height (green) at GPS site 1 (395 m a.s.l.) (a), site 2 (618 m a.s.l.) (b), site 3 (795 m a.s.l.) (c) and site 4 (1,063 m a.s.l.) (d). The surface height is shown relative to an arbitrary datum with a linear, surface-parallel, slope removed. The dashed lines show winter background velocity (black) and velocities from periods with sparse data (blue). The shaded sections identify periods of ice acceleration associated with ice-surface uplift (red), and slower ice motion associated with a decrease in surface height (blue). The solid lines indicate different phases of longer-term ice velocity versus surface uplift relationship. e, Temperature record from sites 1 (magenta), 3 (red) and 4 (blue).
Seasonal evolution of subglacial drainage and acceleration in a Greenland outlet

May 2010

·

702 Reads

The Greenland ice sheet contains enough water to raise sea levels by 7 m. However, its present mass balance and future contribution to sea level rise is poorly understood. Accelerated mass loss has been observed near the ice sheet margin, partly as a result of faster ice motion. Surface melt waters can reach the base of the ice sheet and enhance basal ice motion. However, the response of ice motion to seasonal variations in meltwater supply is poorly constrained both in space and time. Here we present ice motion data obtained with global positioning system receivers located along a 35 km transect at the western margin of the Greenland ice sheet throughout a summer melt season. Our measurements reveal substantial increases in ice velocity during summer, up to 220% above winter background values. These speed-up events migrate up the glacier over the course of the summer. The relationship between melt and ice motion varies both at each site throughout the melt season and between sites. We suggest that these patterns can be explained by the seasonal evolution of the subglacial drainage system similar to hydraulic forcing mechanisms for ice dynamics that have been observedat smaller glaciers.

Figure 3: IODP Sites C0004 and C0008; core data.Compilation of the magnetostratigraphy, biostratigraphy, lithostratigraphy and content of calcite values for Sites C0004 (ref. 20) and C0008 (ref. 21). Blue boxes in the nanofossil event column indicate likely reworking due to mass movements. The dashed vertical line in the content of calcite plot marks the interpreted threshold condition for deposition below or above the calcite compensation depth CCD (4.00.6 km; ref. 22). Note that we have interpreted this value as 10% calcite, which still accounts for some (10%) calcite reworking by downslope sediment transport processes. The magnetostratigraphy abbreviations are: B: Brunhes chron, M: Matuyama chron, Ga: Gauss chron, Gi: Gilbert chron, J: Jaramillo subchron, CM: Cobb Mountain subchron, O: Olduvai subchron, E: Emporer event.
Figure 4: Summary diagram showing the splay-fault origin and evolution in the Nankai accretionary wedge.a–d, Left and right panels show overall sketches of accretionary prism scale and close-up views on the shallow megasplay system, respectively, for different time steps. The sizes of the red and blue arrows indicate the relative activities of the splay fault and prism forward growth, respectively. The dashed horizontal line shows the approximate depth of the carbonate compensation depth (CCD). The splay-fault system initiated 1.95 Myr ago as an OOST in the lower part of the accretionary wedge. From 1.55 Myr, this initial OOST has been uplifted and became reactivated, favouring ongoing'megasplay' slip along it. Alternating periods of high and low splay-fault activity are linked in an out-of-phase mode to accretionary prism forward growth and in-sequence frontal imbrications.
Origin and evolution of a splay fault in the Nankai accretionary wedge

August 2009

·

654 Reads

Subduction zones are often characterized by wedge-shaped sedimentary complexescalled accretionary prismsthat form when sediments are scraped off the subducting plate and added to the overriding plate. Large, landward-dipping thrust faults can cut through such a prism: these faults, known as megasplay faults, originate near the top of the subducting plate and terminate at the shallow, landward edge of the prism. Megasplay faults have been the subject of numerous geological and geophysical studies, but their initiation and evolution through time remains poorly constrained. Here we combine seismic reflection data from the Nankai accretionary wedge with geological data collected by the Integrated Ocean Drilling Program (IODP) and find that the splay fault cutting this wedge initiated 1.95 Million years (Myr) ago in the lower part of the prism as an out-of-sequence thrust (OOST). After an initial phase of high activity, the movement along the fault slowed down, but uplift and reactivation of the fault resumed about 1.55 Myr ago. The alternating periods of high and low activity along the splay fault that we document hint at episodic changes in the mechanical stability of accretionary prisms.

Atmospheric chemistry: Natural atmospheric acidity

December 2011

·

45 Reads

Formic acid exerts a significant influence on atmospheric chemistry and rainwater acidity. Satellite observations and model simulations suggest that terrestrial vegetation accounts for around 90% of the formic acid produced annually.

Glacier advance in southern middle-latitudes during the Antarctic Cold Reversal

September 2010

·

144 Reads

During the last deglaciation, warming over Antarctica was interrupted by a return to colder conditions from about 14,540 to 12,760yr ago. This period, known as the Antarctic Cold Reversal, is well documented in Antarctic ice cores, but the geographic extent of the cooling throughout the Southern Hemisphere remains unclear. Here we use 10Be surface-exposure ages from two glacial moraine sets from the Southern Alps, New Zealand, to assess whether the glacier advance was associated with the Antarctic Cold Reversal. We find that widespread glacier resurgence culminated 13,000years ago, at the peak of Antarctic cooling. Subsequent glacier retreat in the Southern Alps coincided with warming in Antarctica. We conclude that the climate deterioration associated with the Antarctic Cold Reversal extended into the southern mid-latitudes of the southwestern Pacific Ocean. We suggest that the extensive cooling was caused by northward migration of the southern Subtropical Front, and concomitant northward expansion of cold Southern Ocean waters.

Figure 1: Kohat Plateau (yellow polygon) flanked by neighbouring plateaux. Rupture area of 20 May 1992 Mw=6.0 earthquake shown as green rectangle in map (a) and green line in section (b) with inset mechanism. a, InSAR tracks numbered as inclined rectangles. The blue arrow indicates the velocity (mm yr−1) of convergence of the Peshawar Basin with the fixed Indian Plate3. Seismicity from US Geological Survey Preliminary Determination of Epicenters catalogue 1973–2008 (blue circles with scale top left). b, Three sections illustrate the morphology of the Bannu Basin (BB, grey), Potwar Plateau (PP, dashed blue) and Kohat Plateau (red) respectively. KR, Kishor Range; MR, Marwat Range; SR, Salt Range; KF, Kalabagh Fault; PB, Peshawar Basin.
Stick–slip advance of the Kohat Plateau Pakistan

January 2012

·

656 Reads

Throughout most of the Himalaya, slip of the Indian Plate is restrained by friction on the interface between the plate and the overlying wedge of Himalayan rocks. Every few hundred years, this interface--or décollement--ruptures in one or more Mw >=8 earthquakes. In contrast, in the westernmost Himalaya, the Indian Plate slips aseismically beneath wide plateaux fronting the Kohistan Mountains. The plateaux are underlain by viscous décollements that are unable to sustain large earthquakes. Potwar, the widest of these plateaux is underlain by viscous salt, which currently permits it to slide at rates of about 3mmyr-1 (refs , ), much slower than its 2 Myr average. This deceleration has been attributed to recently increased friction through the loss of salt from its décollement. Here we use interferometric synthetic aperture radar and seismic data to assess movement of the Kohat Plateau--the narrowest and thickest plateau. We find that in 1992 an 80 km2 patch of the décollement ruptured in a rare Mw 6.0 earthquake, suggesting that parts of the décollement are locally grounded. We conclude that this hybrid seismic and aseismic behaviour represents an evolution of the mode of slip of the plateaux from steady creep towards increasingly widespread seismic rupture.

Figure 3: Frequency of occurrence for six bins of cloud top height and six subsets of concentration of condensation nuclei (CN). The dashed line is the mean freezing level (~3.3 km). Arrows indicate the trend of the frequency with increasing concentration of condensation nuclei. Except for 2–3 km and >7 km cloud top height bins, the trends are all significant at 95% significance levels.
Figure 4: Changes in rainfall frequency and rain rate distribution with concentration of condensation nuclei (CN). a, Rainfall frequency as a function of concentration of condensation nuclei for different LWP bins at the SGP site during all summer seasons. Clouds are grouped into two categories: LWP>0.8 mm and LWP<0.8 mm. Note that different ranges of rainfall frequencies are used, as indicated by the two y axes. b, Frequency of occurrence of rain amount per rain event during all summer seasons. The rain events are grouped into two categories (clean, CN<2,000 cm−3, and dirty, 4,000<CN<6,000 cm−3) on the basis of concentration of condensation nuclei measured 1.5 h before the rain event.
Figure 5: Cloud base height (CBH) as a function of concentration of condensation nuclei (CN) for single-layer clouds during all summer seasons. No constraint is applied to cloud top height. Error bars, s.e.m.
Figure 6: Modelled changes in cloud thickness, CTH, rain frequency and rain amount with CCN. SGP0708 indicates the summertime warm-base (CBT of about 19 °C) convective cloud case and SGP0402 indicates the springtime cool-base (CBT of about 11 °C) convective cloud case. Cloud thickness and top height are averaged over the grid points where LWP>0.8 mm. The rain frequency is the number of grid points with a rain rate greater than 0.01 mm h−1 divided by the total number of grid points (as a percentage). The rain amount is averaged over the domain that covers the convective system but excludes the effect from the boundaries.
Long-term impacts of aerosols on the vertical development of clouds and precipitation

November 2011

·

2,041 Reads

Aerosols alter cloud density and the radiative balance of the atmosphere. This leads to changes in cloud microphysics and atmospheric stability, which can either suppress or foster the development of clouds and precipitation. The net effect is largely unknown, but depends on meteorological conditions and aerosol properties. Here, we examine the long-term impact of aerosols on the vertical development of clouds and rainfall frequencies, using a 10-year dataset of aerosol, cloud and meteorological variables collected in the Southern Great Plains in the United States. We show that cloud-top height and thickness increase with aerosol concentration measured near the ground in mixed-phase clouds-which contain both liquid water and ice-that have a warm, low base. We attribute the effect, which is most significant in summer, to an aerosol-induced invigoration of upward winds. In contrast, we find no change in cloud-top height and precipitation with aerosol concentration in clouds with no ice or cool bases. We further show that precipitation frequency and rain rate are altered by aerosols. Rain increases with aerosol concentration in deep clouds that have a high liquid-water content, but declines in clouds that have a low liquid-water content. Simulations using a cloud-resolving model confirm these observations. Our findings provide unprecedented insights of the long-term net impacts of aerosols on clouds and precipitation.

Figure 2: Palaeoenvironmental records of the NGRIP ice core, MD95 2042 and GeoB7920 for the last 120 kyr BP.a, Variations of the air temperature over Greenland indicated by the 18O record of the NGRIP ice core and the numbered interstadial events30. b, Alkenone-based SST reconstruction of core MD95 2042 (ref. 23). c,d, 18O (c) and 13C (d) record of benthic foraminifera Cibicidoides wuellerstorfi of core GeoB7920-2. e, Continental humidity index of core GeoB7920-2 as indicated by log[EM3/(EM1+EM2)]. f, Age–depth relationship of GeoB7920-2 (see Supplementary Information). g, Average summer insolation at 30° N. The grey bars indicate North Atlantic ice rafted debris events22, 23.
Figure 3: Model–data comparison of the northern Africa humidity and vegetation cover during the last 120 kyr BP.a,b, AOV-IC model simulation of the vegetation cover and the annual mean daily precipitation (mm d-1) (black dashed line) in the Sahara grid box (20°–30° N) (a) and the Sahel grid box (10°–20° N) (b). c, Temporal variation of the continental humidity index of core GeoB7920.
Figure 4: Model–data comparison of the northern Africa humidity and vegetation cover from 65 to 15 kyr BP.a,b, AOV-IV-f model simulation of the vegetation cover and the annual mean daily precipitation (mm d-1) (black dashed line) in the Sahara grid box (20°–30° N) (a) and the Sahel grid box (10°–20° N) (b). The grey bars indicate North Atlantic freshwater pulses triggered every 7.5 kyr. c, Temporal variation of the continental humidity index of core GeoB7920. The grey bars indicate North Atlantic ice rafted debris events22, 23.
Figure SF6. Resolution and present-day orography of CLIMBER-2 [32, 34]. The model specifies atmospheric grid boxes (dashed lines), the Atlantic, the Pacific, and the Indian Ocean basins (thick solid lines). In the model, the Mediterranean Sea belongs to the Indian Ocean, even though it is separated from it by land masses.
Figure SF7. Transient forcing to trigger D/O and Heinrich events in simulation AOV-ICf. a, Changes in inland ice volume I in metres of sea level change (m SL) compared to today (dashed line is volume Eurasian ice sheet, solid line is global ice volume). b, Freshwater forcing in the North Atlantic in Sverdrup (1 SV = 10 6 m 3 s-1 ). The top curve is the freshwater forcing to trigger Heinrich Events, and the lowest curve is a random white noise forcing at high northern latitude which triggers D/O events). The middle curve is a small sinusoidal forcing which itself is too weak to trigger D/O events, but which synchronizes D/O events via the mechanism of stochastic resonance [42-44].
Coherent high- and low-latitude control of the northwest African hydrological balance

September 2008

·

1,210 Reads

The evolution of the northwest African hydrological balance throughout the Pleistocene epoch influenced the migration of prehistoric humans. The hydrological balance is also thought to be important to global teleconnection mechanisms during Dansgaard-Oeschger and Heinrich events. However, most high-resolution African climate records do not span the millennial-scale climate changes of the last glacial-interglacial cycle, or lack an accurate chronology. Here, we use grain-size analyses of siliciclastic marine sediments from off the coast of Mauritania to reconstruct changes in northwest African humidity over the past 120,000 years. We compare this reconstruction to simulations of palaeo-humidity from a coupled atmosphere-ocean-vegetation model. These records are in good agreement, and indicate the reoccurrence of precession-forced humid periods during the last interglacial period similar to the Holocene African Humid Period. We suggest that millennial-scale arid events are associated with a reduction of the North Atlantic meridional overturning circulation and that millennial-scale humid events are linked to a regional increase of winter rainfall over the coastal regions of northwest Africa.

Atmospheric dynamics: The age of stratospheric air

January 2009

·

51 Reads

Climate models predict that increasing greenhouse gas levels will invigorate the circulation in the upper atmosphere. But a close look at observations of the age of stratospheric air over 30 years reveals no acceleration in the circulation.

Figure 1: Tectonic map of southern Alaska.Plate motion vectors are from ref. 29.
Figure 2: Sample locations and main tectonic structures.Samples Y1, Y2, Y3 and CH46 were published in Enkelmann et al.14. CSEF: Chugach/St Elias fault, separating the Yakutat terrane from the Prince William terrane. The Contact fault sutures the Prince William from the Chugach terrane, and the Border Range fault sutures the Chugach (south) from the Wrangellia terrane (north). The drainage area of the Seward–Malaspina glacier is outlined in red. Thermochronological ages from bedrock studies are shown1, 2, 3, 10. AHe: apatite (U–Th)/He, AFT: apatite fission track, ZHe: zircon (U–Th)/He, ZFT: zircon fission-track.
Figure 3: Comparison of U/Pb zircon ages.Probability density plots of U/Pb zircon ages of samples IB3 and IB4 compared with the zircon U/Pb ages from sample CH46 (ref. 14) representing material of the Chugach metamorphic complex that was transported by the Bagley Ice field/Tana glaciers system (), and the detrital zircon results of the Yakutat Group sample dated for this study (see Supplementary Table S3). The Yakutat Group is the metasedimentary basement of the Yakutat terrane.
Intense localized rock uplift and erosion in the St Elias orogen of Alaska

April 2009

·

232 Reads

The timing and role of exhumation in the StElias orogen, the worlds highest coastal mountain range, has been unclear. Sampling is limited to high mountain ridges that tower over widespread ice fields that sit in deeply eroded parts of the orogen. Existing bedrock studies in the region are therefore prone to bias. Here we analyse detrital material of active sediment systems in the StElias orogen to obtain age information from the inaccessible ice-covered valley bottoms. We present 1,674 detrital zircon fission-track ages from modern rivers that drain the glaciers. We find a population of very young ages of less than 3 Myr from the Seward-Malaspina glacier systems that is sharply localized in the area of the orogens highest relief, highest seismicity and at the transition from transform to subduction tectonics. Our data provide evidence for intense localized exhumation that is driven by coupling between erosion and active tectonic rock uplift.

Figure 1: Regional area-average glacier mass balance in northwest North America between 1962 and 2006.The boundaries and names of the different glaciated regions follow those of Arendt et al.2, except that the Wrangell Mountains have been included in the St Elias Mountains. AR: Alaska Range.
Figure 3: Hypsometry and rate of ice elevation change versus altitude in the Western Chugach Mountains.Upper panel: The hypsometry (distribution of ice-covered areas with altitude) for the whole mountain range (9,149 km2) and Columbia Glacier (1,066 km2). Lower panel: 1957–2007 rate of ice elevation changes (averaged every 50 m elevation bins) extracted from the sequential DEM for the Western Chugach Mountains, the Columbia Glacier and along the altimetric laser profiles (see ) surveyed by Arendt et al.2.
Contribution of Alaskan glaciers to sea-level rise derived from satellite imagery

January 2010

·

609 Reads

Over the past 50 years, retreating glaciers and ice caps contributed 0.5 mm yr-1to sea-level rise, and one third of this contribution is believed to come from ice masses bordering the Gulf of Alaska. However, these estimates of ice loss in Alaska are based on measurements of a limited number of glaciers that are extrapolated to constrain ice wastage in the many thousands of others. Uncertainties in these estimates arise, for example, from the complex pattern of decadal elevation changes at the scale of individual glaciers and mountain ranges. Here we combine a comprehensive glacier inventory with elevation changes derived from sequential digital elevation models. We find that between 1962 and 2006, Alaskan glaciers lost 41.9 ± 8.6 km 3yr-1 of water, and contributed 0.12 ± 0.02 mm yr-1 to a-level rise, 34% less than estimated earlier2,3. Reasons for our lower values include the higher spatial resolution of our glacier inventory as well as the reduction of ice thinning underneath debris and at the glacier margins, which were not resolved in earlier work. We suggest that estimates of mass loss from glaciers and ice caps in other mountain regions could be subject to similar revisions.

Albertan oil

April 2010

·

13 Reads

Anna Armstrong reviews Dirty Oil by Leslie Iwerks, Dogwoof: 2010. UK release date: 19 March 2010.

Figure 4: Geomorphic and sedimentary evidence of post-glacial valley infill and dissection of inner gorges, Landquart River (see  for location). a, LiDAR-derived river longitudinal profile showing inset gorges (yellow) and the infilled remnant of former bedrock gorge ~400 m above the present channel (thick dashed line). Red vertical figures are the minimum inner gorge relief on tributaries (vertical dashed lines). b, Topographic map showing remnants of fill terraces (red) and alluvial fan (green) that cap former inner gorge confluence, and is graded to post-glacial valley fill with a maximum depth of ~180 m. Yellow dots are abandoned bedrock gorge segments flanked by truncated bedrock spurs.
Figure 5: LiDAR-derived topography of southern front of the ~9 kyr Flims rockslide (yellow brown shade, l1; see  for location). Local slope gradients indicated by greyscale hue. Rockslide motion was SSE, with highly mobile fragmented debris entering tributary valleys, causing ephemeral blockage (former dam, former lake) and deposition of backwater (fp) and alluvial (fpa) sediments capping >100-m thick rockslide debris emplaced in pre-existing V-shaped bedrock inner gorge (g). Younger landslides (l2) cover the southern margin of Flims rockslide deposit.
Preservation of inner gorges through repeated Alpine glaciations

December 2010

·

340 Reads

Extensive valley glaciers have repeatedly covered the inner gorges of the Swiss Alps during Quaternary glaciations. Two controversial explanations of the development of the features have been proposed. In the first, the gorges would have formed anew each time the glaciers receded, through fluvial incision of the previously glaciated surfaces. Alternatively, the valleys could be palimpsest features, carved through successive glacial-interglacial cycles. Here we use topographic data derived from LiDAR measurements to show that fluvial erosion rates of 8.5-18mmyr-1 would be required to create the current relief of Swiss gorges solely during the present interglacial period. Such high rates exceed the long-term average bedrock erosion rates of even the most tectonically active regions. This scenario would also require that previously incised valleys were erased during successive glaciations by commensurately high glacial erosion rates, a suggestion that is incompatible with available constraints of exhumation from thermochronometry. We therefore suggest that the gorges observed in the Swiss Alps are resilient to repeated glaciations. Our data are most consistent with the hypothesis that gorges are progressively incised below the elevations of glacial trough valleys through multiple glaciations.

Significant increase in relief of the European Alps during Mid-Pleistocene glaciations

September 2011

·

425 Reads

Some of Earth's greatest relief occurs where glacial processes act on mountain topography. This dramatic landscape is thought to be an imprint of Pleistocene glaciations. However, whether the net effect of glacial erosion on mountains is to increase or decrease relief remains disputed. It has been suggested that in the European Alps, the onset of widespread glaciation since the mid-Pleistocene climate transition led to the growth of large, long-lived and strongly erosive alpine glaciers that profoundly influenced topography. Here we use 4He/3He thermochronometry and thermal-kinematic models to show that the Rhône Valley in Switzerland deepened by about 1-1.5km over the past one million years. Our results indicate that while the valley was incised and back-cut, high-altitude areas were preserved from erosion. We find an approximately two-fold increase in both local topographic relief and valley concavity, which occurred around the time of the mid-Pleistocene transition. Our results support the proposed link between the onset of efficient glacial erosion in the European Alps and the transition to longer, colder glacial periods at the middle of the Pleistocene epoch.

Brucite and carbonate assemblages from altered olivine-rich materials on Ceres

March 2009

·

132 Reads

The dwarf planet Ceres is the largest object in the asteroid belt, and is generally thought to be a differentiated body composed primarily of silicate materials and water ice. Some remotely observed features, however, indicate that Ceres may instead have a composition more similar to that of the most common types of carbonaceous meteorite. In particular, Ceres has been shown to have a distinct infrared absorption feature centred at a wavelength of 3.06 m that is superimposed on a broader absorption from 2.8 to 3.7 m (refs5,8), which suggests the presence of OH- or H 2 O-bearing phases. The specific mineral composition of Ceres and its relationship to known meteorite mineral assemblages, however, remains uncertain. Here we show that the spectral features of Ceres can be attributed to the presence of the hydroxide brucite, magnesium carbonates and serpentines, a mineralogy consistent with the aqueous alteration of olivine-rich materials. We therefore suggest that the thermal and aqueous alteration history of Ceres is different from that recorded by carbonaceous meteorites, and that samples from Ceres are not represented in existing meteorite collections.

Figure 1: Temperature change drives both the biotic precipitation of Fe(III) minerals and the abiotic precipitation of silica.a, Dependence of Rhodobacter ferrooxidans sp. strain SW2 Fe(II) oxidation rates on temperature (4 mM dissolved Fe(II); 800 lux). b, Microbial oxidation of 0.5 mM Fe(II) by strain SW2 in the presence of 2.0 mM silica, at 75 lux. c, Temperature dependence of dissolved silica concentration in non-inoculated medium. Error bars depict standard deviation from the mean (triplicate experiments).
Figure 2: Possible deposition of alternating iron and silicate mineral layers in BIFs as triggered by temperature variations in ocean waters.a, Experimentally determined microbial Fe(II) oxidation rates at fluctuating temperature and the resulting Fe(III) mineral precipitation. The effect of temperature fluctuations between 5 and 30 °C on abiotic silica precipitation. b, Oxidation of dissolved Fe(II) by strain SW2 at changing temperatures and in a 20 °C control. Error bars depict standard deviation from the mean (triplicate experiments). c, Demonstration of microbial Fe(III) mineral precipitation in the presence of silica at 25 °C, and silica precipitation after temperature drop to 4 °C.
Alternating Si and Fe deposition caused by temperature fluctuations in Precambrian oceans

September 2008

·

505 Reads

Precambrian banded iron formations provide an extensive archive of pivotal environmental changes and the evolution of biological processes on early Earth. The formations are characterized by bands ranging from micrometre- to metre-scale layers of alternating iron- and silica-rich minerals. However, the nature of the mechanisms of layer formation is unknown. To properly evaluate this archive, the physical, chemical and/or biological triggers for the deposition of both the iron- and silica-rich layers, and crucially their alternate banding, must be identified. Here we use laboratory experiments and geochemical modelling to study the potential for a microbial mechanism in the formation of alternating iron–silica bands. We find that the rate of biogenic iron(III) mineral formation by iron-oxidizing microbes reaches a maximum between 20 and 25 °C. Decreasing or increasing water temperatures slow microbial iron mineral formation while promoting abiotic silica precipitation. We suggest that natural fluctuations in the temperature of the ocean photic zone during the period when banded iron formations were deposited could have led to the primary layering observed in these formations by successive cycles of microbially catalysed iron(III) mineral deposition and abiotic silica precipitation.

Drinking up the Amazon

September 2009

·

7 Reads

Anna Armstrong reviews Big River Man by John Maringouin, Self Pictures: 2009. UK release date: 4 September 2009.

Figure 1: The WIS possessed a pronounced palaeobiogeographic zonation during Late Cretaceous time; inferred circulation patterns differ radically. Map modified from research describing vertebrate palaeobiogeography in the seaway8. Specimens analysed in this study were collected from the Niobrara-age formations of western Kansas (KS) and the Mississippi embayment (MS) located near the junction of the WIS and the western Tethys region. These areas are separated by about 5° palaeolatitude. Insets show different predictions for sources of KS surface waters and WIS circulation: Tethyan1, boreal2, and reversing circulation of northern waters3, 9. JJA=June, July, August; DJF=December, January, February.
Isotopic evaluation of ocean circulation in the Late Cretaceous North American seaway

November 2011

·

209 Reads

During the mid- and Late Cretaceous period, North America was split by the north-south oriented Western Interior Seaway. Its role in creating and maintaining Late Cretaceous global greenhouse conditions remains unclear. Different palaeoceanographic reconstructions portray diverse circulation patterns. The southward extent of relatively cool, low-salinity, low-δ18O surface waters critically distinguishes among these models, but past studies of invertebrates could not independently assess water temperature and isotopic compositions. Here we present oxygen isotopes in biophosphate from coeval marine turtle and fish fossils from western Kansas, representing the east central seaway, and from the Mississippi embayment, representing the marginal Tethys Ocean. Our analyses yield precise seawater isotopic values and geographic temperature differences during the main transition from the Coniacian to the early Campanian age (87-82 Myr), and indicate that the seaway oxygen isotope value and salinity were 2‰ and 3‰ lower, respectively, than in the marginal Tethys Ocean. We infer that the influence of northern freshwater probably reached as far south as Kansas. Our revised values imply relatively large temperature differences between the Mississippi embayment and central seaway, explain the documented regional latitudinal palaeobiogeographic zonation and support models with relatively little inflow of surface waters from the Tethys Ocean to the Western Interior Seaway.

Figure 1: Arctic amplification of zonal mean surface air temperature change for a doubling of CO2. Annual mean temperature change as a function of latitude for standard mixing (black line), for increased mixing (blue line) and decreased mixing (red line) in stable conditions (see Supplementary Information). The vertical bars on the right denote the mean Arctic (70°–90° N) seasonal range in the temperature change for each case. The inset shows the geographical distribution of surface air temperature change (K) for the standard model in winter.
Figure 2: Zonal mean winter (DJF) changes in clear-sky TOA infrared radiation for a doubling of CO2. Change in simulated (EC-Earth) TOA outgoing longwave radiation with the total (black) being composed of a contribution from the surface (blue) and from the atmosphere (red), averaged over 10° latitude bands. The method to evaluate these contributions is outlined in the Supplementary Information.
Figure 3: Zonal mean changes in wintertime (DJF) atmospheric cooling efficiency, inversion strength and vertical temperature profile for a doubling of CO2. a, Change in atmospheric cooling efficiency γ (see Supplementary Information). The larger the value of γ, the stronger the cooling efficiency. The cooling efficiency diminishes because the warming-induced infrared radiation emitted by the atmosphere is largely directed downward. b, Change in inversion strength (defined here as the temperature difference between the 925 hPa and 1,000 hPa level). Inversion strengths diminish because of surface warming. c, Change in vertical temperature profile (mean over 70°–90° N) for each of the three mixing cases. Note that the data in b and c are for all-sky conditions (important because inversion strength most probably depends on clouds being present or not).
Figure 4: Change in DJF longwave all-sky longwave radiation components averaged over the Arctic region (70°–90° N) for a doubling of CO2. a, Total outgoing longwave radiation (black) is composed of a contribution from the surface LTsur(blue) and from the atmosphere LTatm (red). Results are shown for the standard model, and for the models with increased and decreased mixing in stable conditions. b, DJF changes in downward longwave radiation at the surface and outgoing radiative flux by the atmosphere as a function of DJF change in surface air temperature. The three data points represent, from left to right, the increased mixing case (INCMIX), the standard mixing case (CONTROL) and the decreased mixing case (DECMIX) runs. Positive values indicate that the atmospheric radiative energy loss increases (either to the surface or to space).
Arctic winter warming amplified by the thermal inversion and consequent low infrared cooling to space

October 2011

·

1,232 Reads

Pronounced warming in the Arctic region, coined Arctic amplification, is an important feature of observed and modelled climate change. Arctic amplification is generally attributed to the retreat of sea-ice and snow, and the associated surface-albedo feedback, in conjunction with other processes. In addition, the predominant thermal surface inversion in winter has been suggested to pose a negative feedback to Arctic warming by enhancing infrared radiative cooling. Here we use the coupled climate model EC-Earth in idealized climate change experiments to quantify the individual contributions of the surface and the atmosphere to infrared radiative cooling. We find that the surface inversion in fact intensifies Arctic amplification, because the ability of the Arctic wintertime clear-sky atmosphere to cool to space decreases with inversion strength. Specifically, we find that the cold layers close to the surface in Arctic winter, where most of the warming takes place, hardly contribute to the infrared radiation that goes out to space. Instead, the additional radiation that is generated by the warming of these layers is directed downwards, and thus amplifies the warming. We conclude that the predominant Arctic wintertime temperature inversion damps infrared cooling of the system, and thus constitutes a positive warming feedback.

Figure 1: Sea-level curves derived using five different methods.a, Model6 driven by benthic oxygen isotope (18O) stack. b, Sea-level curve based on benthic 18O data and ice-volume model8. c, Reconstructions on the basis of sea water 18O calculated from paired Mg/Ca and 18O measurements on planktonic foraminifera2. d, Reconstruction of Red Sea sea water 18O (ref. 3). e, Reconstruction derived from open-system U–Th ages of corals7. Shading indicates periods of time for which sea level rises above -20 m (dashed lines), the approximate depth of Argentarola Cave speleothems. Note differences in the number of MIS 7 highstands predicted to exceed -20 m and the difference in elevation predicted for MIS 7.3 in particular.
Figure 3: Summary of MIS 7 highstands.Submerged speleothem U–Th data represent growth periods and should be above the sea-level curve, whereas coral data should be just below the curve. Solid lines connecting speleothem U–Th ages represent periods of uninterrupted growth. The error bars for samples next to hiatuses are shown as dashed lines. Peak MIS 7.5 coral data were assumed to sit at modern sea-level7. The remainder of the Barbados coral elevations are calculated assuming constant uplift rates, which introduces some error into the elevation estimates7. Closed-system ages are shown for corals with 234Uinital within 2 of sea water7, 17, 29.
Phasing and amplitude of sea-level and climate change during the penultimate interglacial

April 2009

·

1,025 Reads

Earth's climate has oscillated between short-lived interglacial and extended glacial periods for the past million years. Before the last interglacial, absolutely dated markers of sea level become increasingly rare; hence, our knowledge of sea-level change driven by the waxing and waning of continental ice sheets before that time is largely based on proxy records from deep-sea cores(1-3) that lack direct age control. Here we present precise U-Th ages for a remarkable collection of submerged speleothems(4,5) from Italy, which record three sea-level highstands during the penultimate interglacial period, Marine Isotope Stage 7, from 245,000 to 190,000 years ago. We find that sea level rose above-18m (relative to modern sea level) several thousand years before maximum Northern Hemisphere insolation during the first and third highstands. In contrast, the second highstand, Marine Isotope Stage 7.3, is essentially synchronous with the insolation maximum, and sea level during this highstand only peaked at about 18 m, even though the concurrent insolation forcing was the strongest of the three highstands. We attribute the different phasing and amplitude of the Marine Isotope Stage 7.3 highstand to the extensive continental glaciation that preceded it. This finding highlights the significance of cryosphere response time to the climate system.

Early biosphere: Magnifying ancient microstructures

September 2009

·

28 Reads

Purported 3,465-million-year-old microfossils from Australia have been the subject of considerable debate. A method to distinguish between pristine fossils, mineral artefacts and subsequent microbial contamination will aid the search for ancient biogenic material.

Palaeoceanography: Tracking ancient sea ice

November 2009

·

16 Reads

Sea ice is an integral component of the climate system, but a difficult one to reconstruct. Biochemical tracers preserved in marine sediments now reveal the waxing and waning of sea ice since the Last Glacial Maximum in an Arctic Ocean gateway.

Ancient ocean on Mars supported by global distribution of deltas and valleys

June 2010

·

896 Reads

The climate of early Mars could have supported a complex hydrological system and possibly a northern hemispheric ocean covering up to one-third of the planets surface. This notion has been repeatedly proposed and challenged over the past two decades, and remains one of the largest uncertainties in Mars research. Here, we used global databases of known deltaic deposits, valley networks and present-day martian topography to test for the occurrence of an ocean on early Mars. The distribution of ancient martian deltas delineates a planet-wide equipotential surface within and along the margins of the northern lowlands. We suggest that the level reconstructed from the analysis of the deltaic deposits may represent the contact of a vast ocean covering the northern hemisphere of Mars around 3.5 billion years ago. This boundary is broadly consistent with palaeoshorelines suggested by previous geomorphologic, thermophysic and topographic analyses, and with the global distribution and age of ancient valley networks. Our findings lend credence to the hypothesis that an ocean formed on early Mars as part of a global and active hydrosphere.

Figure 1: Map showing distributions of Cenozoic volcanic fields and deep faults in northeast China. The distributions are from ref. 28. The distance from Tianchi volcano, which is located in the central part of the Changbaishan area, is shown. Grey dashed lines indicate locations of cross-sections shown in . See  for colour legend.
Figure 2: Vertical cross-sections of P-wave velocity tomography under northeast Asia. The locations of a, east–west and b, north–south cross-sections are shown in . Black crosses and white circles show the shallow and deep earthquakes. The figure is slightly modified from ref. 6.© 2009 Elsevier
Figure 3: Spatial variations in Ba/Th and Pb/U ratios of late Cenozoic basaltic lavas from northeast China. The horizontal axis shows the distance from the Tianchi volcano, located at the centre of the Changbaishan area. Quaternary samples are indicated by filled circles and Tertiary samples (<10 Myr) and samples of unknown ages are indicated by open circles. Samples with a significant Eu anomaly (Eu*>1.1 or Eu*<0.9), which may be significantly affected by crustal processes (that is, plagioclase fractionation or accumulation), are not plotted. See Supplementary Information for the source of the data.
Figure 4: Lead isotopic compositions of late Cenozoic basalts from northeast China. Present-day compositions of continental crust-derived sediment that has evolved with μ=2, starting 1.5–0 Gyr ago, from a modified two-stage model of ref. 29 (see Supplementary Fig. S6 caption) are shown. Compositions of Japan Sea basalts (open crosses), altered oceanic crust (filled triangle), pelagic sediment (grey area), and EM1 are taken from refs 30, 18, 24, and 12, respectively. Large open circles show the present-day compositions of the three possible endmember components (Supplementary Fig. S6). The data source for lavas is given in the Supplementary Information.
Intensive hydration of the mantle transition zone beneath China caused by ancient slab stagnation

September 2011

·

713 Reads

The mantle transition zone, located at depths of 410-660km between the lower and upper mantle, is an important water reservoir in the Earth's interior. However, there are regional-scale heterogeneities in the distribution of water. The zone beneath northeast China, in particular, is remarkably hydrous, but when and how it became hydrous remains uncertain. Here we combine analyses of the geochemistry of late Cenozoic basalts in northeast China with published geochemical analyses. We find a spatial correlation between basalt geochemistry and the distribution of a low-velocity zone in the underlying mantle that is interpreted as a plume upwelling from the mantle transition zone. We therefore use the basalt geochemistry to infer the composition of the mantle transition zone. The basalts have high Ba/Th and 207Pb/206Pb ratios, which we suggest record an ancient hydration event in the transition zone that occurred more than one billion years ago, probably as a result of dehydration of a subducted slab. We suggest that this ancient hydration event, combined with a more recent hydration event linked to dehydration of the subducted Pacific slab, can account for the hydrous nature of the mantle transition zone beneath China. Our results demonstrate that the mantle transition zone can remain as a stable water reservoir in Earth's interior for timescales of more than a billion years.

Figure 1: Extended trace-element patterns for the MA (black) and CA (grey) series compared with lamproite from Leucite Hills8. MA series show a less pronounced ‘subduction’ signature compared with the CA series. Note that the MA lavas show multiple-times-higher concentrations for a number of trace elements compared with upper continental crust30 (UCC; see more details in Supplementary Information) and approach the extreme values observed in ultrapotassic melts such as lamproites derived from SCLM (ref. 8).
Figure 1 | Present-day map of the Caribbean region; tectonic features after refs 11,13. The star symbols show the approximate locations of the studied samples. Note the position of the MA to the west of the CA centres. The dotted line shows the extent of the Grenvillian-age basement in South and Central America 11,25 .
Figure 2: Present-day Sr–Nd–Pb isotopes. a, Sr versus Pb comparison of the MA lavas with EM1 and EM2. b, Sr versus Nd compositions of the MA and CA lavas compared with possible sources in the Caribbean region and Kerguelen. Support for Gondwanan origin of the MA source is evident in the distinct trend for the Kerguelen–Hispaniola lavas compared with other EM1 lavas in Sr–Pb space. MA–CA series have distinct Sr–Nd compared with possible plume sources (Galapagos and CLIP; refs 19, 20) and the Mid-Cayman rise (MCR; ref. 21). CAMP (ref. 23), EM1 (ref. 1), Galapagos and MORB (Pacific and Atlantic) and Antilles data from http://www.petdb.org and http://www.georoc.mpch-mainz.gwdg.de.
Figure 3: Present-day Pb isotopes for MA and CA compared with possible sources in the region. a,b, The isotopic compositions of the MA-series lavas are distinct compared with samples from the MCR, CLIP, CAMP, MORB and Antilles lavas. The CA series lie on a mixing trend between the MA and Antilles subduction components. Note that the Colombia Grenville trend best explains all of the Pb isotope systematics of the MA series. NHRL—Northern Hemisphere reference line; data sources are the same as ; Colombia and Mexico Grenvillian terranes, ref. 25.
Ancient lithospheric source for Quaternary lavas in Hispaniola

July 2011

·

361 Reads

Fragments of ancient continental lithosphere, entrained in the shallow oceanic mantle, have been found in a number of locations in the Southern Hemisphere, including rare arc settings. Lavas erupted in these locations exhibit Pb isotopic characteristics that are similar to the so-called enriched mantle 1 reservoir, one of the end-members that define the isotopic composition of the Earth's mantle. However, no lavas with isotopic signatures resembling enriched mantle 1 have been identified in the Caribbean region. Here we present isotopic analyses for mafic-alkaline lavas from Quaternary volcanic centres in Hispaniola. We identify unusual isotopic characteristics indicating the presence of a mantle component similar to enriched mantle 1 beneath Hispaniola. Furthermore, we find evidence for an involvement of this mantle component in the genesis of spatially associated calk-alkaline lavas. On the basis of these isotopic systematics we estimate that the mafic-alkaline lavas are derived from an ancient lithospheric fragment with affinities to the supercontinent Gondwana. We conclude that the fragment originated from the Grenvillian terranes of Central America and Mexico, which also have affinities to Gondwana, indicating that Hispaniola interacted tectonically with these terranes.

Kick-starting ancient warming

March 2009

·

42 Reads

Rapid global warming marked the boundary between the Palaeocene and Eocene periods 55.6 million years ago, but how the temperature rise was initiated remains elusive. A catastrophic release of greenhouse gases from the Kilda basin could have served as a trigger.