Wiley

Geophysical Research Letters

Published by Wiley and American Geophysical Union

Online ISSN: 1944-8007

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Print ISSN: 0094-8276

Disciplines: Earth and space science

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Violin plots for porewater nutrient concentrations and ratios at the eleven sandy beach sites. Red dotted lines represent the mean porewater nutrient concentrations and ratios of the eleven sandy beach sampling sites. Yellow Sea (YS), East China Sea (ECS), and the South China Sea respectively represent the YS, ECS, and South China Sea.
Groundwater nitrogen speciation (a), groundwater to surface water ratios (b), and groundwater nutrient limitation (c) in the eleven sandy beach subterranean estuaries. The relationship between groundwater nitrate and salinity, the fitting curve shows a significant exponential decay of all coastal groundwater nitrates with salinity (d).
Nutrient source‐sink behaviors in the eleven sandy beach subterranean estuaries. Statistical levels were associated with the following p‐values <0.05*, <0.01**, <0.001***, <0.0001****, and <0.00001*****. The multiple nutrient source‐sink behaviors of each study site are shown Figure S3 in Supporting Information S1.
Impacts of anthropogenic and natural drivers of nitrate concentration in eleven sandy beach sites and their potential environmental responses. The “+” and “−” signs indicate whether a specific driver is positively or negatively correlated with nitrate concentration. The width of the blue flow corresponds to the Pearson's R² values. Statistical significance are assumed at p‐values <0.05* or <0.01**.
Sandy Subterranean Estuaries Minimize Groundwater Nitrogen Pollution Impacts on Coastal Waters

January 2025

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531 Reads

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Isaac R. Santos

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Ling Li
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Geophysical Research Letters is an open access journal that publishes high-impact, innovative, and timely communications-length articles on major advances spanning all of the major geoscience disciplines. Papers should have broad and immediate implications meriting rapid decisions and high visibility.

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A schematic representation of the system. Note that the two rectangles represent the side views of two solid cylinders.
The comparison of the proposed model Equation 11, the diffusion‐controlled model Equation 13 (Rutter, 1976), the reaction‐controlled model Equation 15 (Gratier et al., 2009), and an independent numerical simulation (contact radius r0=1µm ${r}_{0}=1\,{\upmu }\mathrm{m}$): (a) The relationship of the compressive stress σ0 ${\sigma }_{0}$ and the dimensionless parameters αR ${\alpha }_{R}$ and αD ${\alpha }_{D}$; (b) The compressive stress σ0 ${\sigma }_{0}$ versus αR/αD ${\alpha }_{R}/{\alpha }_{D}$ when αR·αD=1×10−6 ${\alpha }_{R}\mathit{\cdot }{\alpha }_{D}=1\times {10}^{-6}$; and (c–f) The pressure solution reaction rate Rd ${R}_{d}$ plotted against the compressive stress σ0 ${\sigma }_{0}$ in the reaction‐controlled (αD≪αR ${\alpha }_{D}\mathit{\ll }{\alpha }_{R}$), diffusion‐controlled (αR≪αD ${\alpha }_{R}\mathit{\ll }{\alpha }_{D}$), and transitional regimes (αR∼αD ${\alpha }_{R}\,\mathit{\sim }\,{\alpha }_{D}$).
The comparison of contact and free surfaces (contact radius r0=500µm ${r}_{0}=500\,{\upmu }\mathrm{m}$): (a) The dissolution reaction rate on contact and free surfaces, computed by Equations 11 and 21, respectively and (b) The conditions of stress and reaction rate constant that favor the dissolution on contact or free surfaces.
Displacement rate during pressure solution versus the applied stress. The symbols represent experimental measurements (Gratier et al., 2009). The solid line and the dashed line represent the proposed model Equation 11 and the exponential model Equation 24, respectively.
A Unified Analytical Model for Pressure Solution With Fully Coupled Diffusion and Reaction
  • Article
  • Full-text available

February 2025

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1 Read

Ziyan Wang

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Benjamin Gilbert

Plain Language Summary When solid grains are compressed against each other in an aqueous environment, minerals at the grain‐to‐grain contact dissolve more easily because of the higher stress. This process is known as pressure solution, which involves dissolution reactions and diffusive solute transport. We have developed an analytical model with fully coupled reaction and diffusion processes. Our model can recover the analytical solutions in the literature that are developed for reaction‐dominant and diffusion‐dominant scenarios. The proposed model is also validated against independent numerical simulations. After validation, we employ the model in experimental measurement, where the measured data is interpreted more accurately compared to previous models.


Trend in (a) 2 m air temperature, (b) sea surface temperature, and (c) and precipitation over the period 1979–2020 in the ERA5 reanalysis. Stippling denotes where the trend is statistically significant at the 95% confidence level.
Trend in 2 m air temperature, sea surface temperature, precipitation, and wind speed over the period 1979–2020 for (a, d, g, j) the HadGEM3‐GC31‐LL historical simulation ensemble mean, (b, e, h, k) the HadGEM3‐GC31‐LL ensemble member with the highest correlation to the ERA5 trend (c, f, i, l) ERA5 reanalysis (repeated from Figure 1 for ease of comparison). Stippling denotes where the trend is statistically significant at the 95% confidence level.
(a, b) 2 m air temperature, (c, d) sea surface temperature, (e, f) sea surface height and (g, h) ocean surface velocity response for the hist‐antwater‐92‐11 and ssp585‐ismip6‐water experiments. The response is computed as the difference between each experiment and its CMIP6 control run with no additional meltwater averaged over 2011–2020 for hist‐antwater‐92‐11 or 2071–2100 for ssp585‐ismip6‐water. Stippling denotes where the response is statistically significant at the 95% confidence level.
Seasonal‐mean near‐surface wind speed response in hist‐antwater‐92‐11 (a–d) and ssp585‐ismip6‐water (e–h). Stippling denotes where the anomaly is statistically significant at the 95% confidence level.
Contours defining the sub‐tropical front (STF) around New Zealand for (a, b) the first 20 years and the last 20 years of the ssp585 simulations. (c, d) The ssp585‐ismip6‐water experiment versus ssp585 averaged over 2081–2100. The left column shows the STF as defined by the 13° ${}^{\circ}$C temperature contour at 100 m depth, and the right column the 34 psu contour at 100 m depth. The shaded region shows the range in STF location given by varying the temperature threshold by ±1° $\pm 1{}^{\circ}$C or the salinity threshold by ±0.2 $\pm 0.2$ psu.
Impacts of Antarctic Ice Mass Loss on New Zealand Climate

February 2025

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3 Reads

Andrew G. Pauling

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Inga J. Smith

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Jeff K. Ridley

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David P. Stevens

We investigate the impacts of meltwater from Antarctic Ice Sheet (AIS) mass loss on New Zealand climate in a state‐of‐the‐art global climate model. We conduct simulations with additional meltwater from AIS mass loss for both the historical period and a high‐emissions future scenario. The ocean surface to the southeast of New Zealand cools, with the largest change in winter and spring. The additional meltwater results in a northward shift of the oceanic sub‐tropical front near New Zealand, which partially offsets the projected southward shift of this front in a warming climate. Wintertime surface westerly winds to the south of New Zealand also increase with the addition of the meltwater. The magnitude of the impact of Antarctic meltwater is uncertain due to the wide spread in estimates of Antarctic mass imbalance, but has important implications for future projections for New Zealand climate.


Left (vectors) and right (color shading) heterogeneous fields of the first month‐reliant SVD mode of the intermember anomalies of 850‐hPa winds and SST (a)–(l) from December to next November using the hindcasts of CanCM4i initialized from December during the period of 1981–2018.
Evolution of the SNR of Niño3.4 index with lead time for the VM years (red) and the non‐VM years (blue) during the period of 1981–2018 using the hindcasts of CanCM4i initialized from February (a), March (b) and April (c). The VM years total 28 and the non‐VM years total 10.
(a) S‐SNR of Niño3.4 index with 12‐month lead for the VM years and the no VM years during the period of 1982–2010 using the hindcasts of NMME models initialized from February. (b) Correction coefficients of the FMA‐averaged VMI and the following DJF‐averaged Niño3.4 index using the hindcasts initialized from February. The solid line is the threshold at the t‐test significant level of 0.01. The star refers to the model that considers the VM as a noise in ENSO prediction.
ACC (a) and RMSE (b) of Niño3.4 index initialized from February, March and April with lead time for the NMME models. The star denotes the model with poor simulation of the VM‐ENSO relationship.
Understanding the Role of the North Pacific Victoria Mode in ENSO Predictability Based on the NMME Hindcasts

February 2025

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5 Reads

Zhengyi Ren

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Zongrong Li

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Ruiqiang Ding

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Jiangyu Mao

Plain Language Summary The El Niño–Southern Oscillation (ENSO) is a climate phenomenon that exerts global environmental and socioeconomic effects. Understanding and extending the predictability of ENSO is one of the most important issues in climate science. The North Pacific Victoria mode (VM) has been demonstrated as a precursor signal for ENSO events in observations and models, which may potentially improve ENSO prediction. However, some studies suggest that the VM can increase the prediction uncertainty of ENSO through air‐sea coupling processes, which may limit ENSO prediction skill. To address the controversy, this study employed the signal‐to‐noise ratio method to evaluate the contribution of the VM to ENSO predictability in forecast models. The results show that the VM can increase the potential predictability of ENSO, suggesting that the VM primarily acts as a signal in ENSO prediction. The accurate simulation of the robust relationship between the VM and ENSO is essential to improve ENSO predictability and prediction in forecast models.


Koopman Autoencoder schematic. The encoder and decoder are denoted by the brackets labeled E(x) $E(x)$ and D(z) $D(z)$, respectively, and the inset shows the linear propagator. Yellow blocks indicate convolutional layers, and orange shading indicates ReLU activations. Red and green blocks indicate pooling and upsampling layers, respectively.
Forecast MSE and Pattern Correlation in the North Pacific and North Atlantic on daily and monthly timescales. Colors indicate dimensionality reduction techniques (red for the Koopman Autoencoder, blue for PCA, and light green for CAE), while markers indicate propagation techniques (x's for the Koopman Autoencoder, filled circles for LIM, and open circles for DP). The black dotted line indicates the climatological MSE of SSH.
Sensitivity of the Koopman Autoencoder to dimensionality for predicting North Pacific daily‐averaged SSH. (a) Reconstruction error by dimensionality for PCA (blue), CAE (light green), and the Koopman Autoencoder (red). (b) Domain‐averaged MSE skill scores of the Koopman Autoencoder predictions relative to climatology for different latent space dimensionalities. (c) Domain‐averaged skill score of the Koopman Autoencoder relative to equivalent dimensionality PCA‐LIM for different forecast leads.
Koopman Autoencoder MSE skill scores for daily‐averaged North Pacific (a, c–h) and North Atlantic (b, i–n) SSH predictions. (a, b): Domain‐averaged skill as a function of lead time. Red: Skill of Koopman Autoencoder relative to PCA‐DP. Purple: Koopman Autoencoder relative to PCA + LIM. Cyan: Skill of PCA‐LIM relative to PCA‐DP. Black dotted lines indicate forecast leads used for panels (c–h). (c, d, e, i, j, k): Skill scores of Koopman Autoencoder relative to PCA‐DP at select time lags. (f, g, h, l, m, n): Same but for skill relative to PCA‐LIM.
Learning Propagators for Sea Surface Height Forecasts Using Koopman Autoencoders

February 2025

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2 Reads

Andrew E. Brettin

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Laure Zanna

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Elizabeth A. Barnes

Due to the wide range of processes impacting the sea surface height (SSH) on daily‐to‐interannual timescales, SSH forecasts are hampered by numerous sources of uncertainty. While statistical‐dynamical methods like Linear Inverse Modeling have been successful at making forecasts, they often rely on assumptions that can be hard to satisfy given the nonlinear dynamics of the climate. Here, we train convolutional autoencoders with a dynamical propagator in the latent space to generate forecasts of SSH anomalies. Learning a nonlinear dimensionality reduction and the prediction timestepping together results in a propagator that produces better predictions for daily‐ and monthly‐averaged SSH in the North Pacific and Atlantic than if the dimensionality reduction and dynamics are learned separately. The reconstruction skill of the model highlights regions in which better representation results in improved predictions: in particular, the tropics for North Pacific daily SSH predictions and the Caribbean Current for the North Atlantic.


The locations used in this work, falling within 5 broad categories: marine (Pacific, Atlantic, and Indian Oceans, Graciosa, Kennaook), biogenic (the Amazon, Congo, and Borneo rainforests, and the Ozarks), urban (Los Angeles, Paris, Kinshasa, Beijing), desert (El Djouf), and polar (Utqiagvik and McMurdo Station).
The distribution of all two‐reaction cycle timescales for 16 locations, sampled from the surface (∼1,000 hPa) at noon local time in July. Colors follow the dominant local chemical sources described in Section 2.1: ocean‐dominated regions are in dark blue, desert in orange‐brown, biogenically‐dominated regions are in green, urban locations are in gray, and the remote polar regions are in light blue.
The bivariate distributions of two‐reaction cycle timescales along secondary dimensions, including (a) NOx concentration, (b) HO2 concentration, (c) OH reactivity, and (d) proportion of OH reactivity determined by reactions with NOx (plotted for urban and biogenic locations only, for clarity of visualization). The distributions use all two‐reaction cycles with timescales less than 10⁸ s (∼3.2 years) cycle⁻¹ from the surface locations at 539 daytime samples (determined by a threshold of greater than 0.4 for the cosine of solar zenith angle) in July, October, January, and April. This includes all noon locations plotted in Figure 2 except McMurdo Station, which is in polar night in the snapshot of local noon timescale distributions in Figure 2. The median timescales of all other distributions from Figure 2 are shown as stars. Topographic isolines indicate the number of points contained within the bounds of the two‐dimensional kernel density estimate, in increments of 10%.
The hexbin plots, with color of each hex showing the number of cycles contained in that hexbin, show the frequency of cycle timescales having rate‐limiting timesteps. Each plot captures the cycles across all 16 locations at the surface at local noon. On the horizontal axis we plot the timescale of the full cycle, while on the vertical axis we track the contribution of the longest participating reaction timescale in a particular cycle to the overall cycle timescale. For each cycle length across two‐, three‐, and four‐reaction cycles, the density of cycles with a rate‐limiting timestep decrease for cycles faster than 1 s.
Characterizing the Speed of Chemical Cycling in the Atmosphere

February 2025

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1 Read

Emy W. Li

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Patrick Obin Sturm

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Sam J. Silva

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Christoph A. Keller

Chemical cycling drives the production and loss of many important atmospheric constituents. The speed of atmospheric chemical cycling is a particularly valuable indicator for characterizing and measuring the effects of such cycles on oxidant chemistry, air quality, and climate. Here, we apply graph theoretical methods to explicitly quantify and analyze the characteristic timescales of gas‐phase chemical cycles in the troposphere and stratosphere, as simulated by the GEOS‐Chem chemical mechanism. We identify all two‐, three‐, and four‐reaction cycles in the mechanism and calculate a characteristic timescale for each individual cycle. We find that the speed of chemical cycling varies by orders of magnitude at any given location but tends to be faster in urban‐ and biogenically‐dominated chemical regions, and slower during the night. We further quantify the fraction of cycling that contains a rate‐determining step, and explicitly demonstrate the large potential for mechanisms to recycle oxidants like OH.


Maps of ALPOD lakes. Panels (a–d) show ALPOD lake statistics: (a) lake fraction, (b) average lake size within each watershed, (c) lake density, and (d) total shoreline distance. Panel (e) shows the open water occurrence image and polygon boundaries for individual lakes, and (f) displays a detailed example of the vector within the Little Black River floodplain near the Yukon Flats.
Landscape controls on lake distribution. (a) Permafrost extent across Alaska and glacial coverage during the Last Glacial Maximum. Substrate texture is shown in Figure S5 of Supporting Information S1. (b) A comparison of lake fractions in watersheds binned by glacial history and substrate texture. The remaining terrain classes are displayed in Figure S7 of Supporting Information S1. Lake fraction increases with permafrost extent in unglaciated watersheds with fine geologic substrate (p < 0.0001), whereas lake fraction decreases with permafrost extent in postglacial watersheds with coarse substrate (p < 0.0001). (c) Comparing lake density (number of lakes per 100 km²) in watersheds binned by substrate texture and permafrost extent. Lake densities are higher in fine substrate and increase with permafrost class (p‐value < 0.0001). Watersheds underlain by coarse substrate exhibit lower overall lake density and a negative correlation between permafrost extent and lake density (p‐value < 0.0001). (d) Size distribution of ALPOD lakes.
Schematic comparing permafrost controls on lake fraction across physiographic settings. Each panel displays the oblique view of topography and ALPOD lakes from a watershed in our study that represents distinct glacial and permafrost classes. The inset panel shows the number of study sites from Webb and Liljedahl (2023) that exhibited decreasing, increasing, or insignificant decadal‐scale lake area trends within the corresponding physiographic settings. The subsurface distribution of permafrost and seasonally freezing active layer are generated to illustrate permafrost hydrology mechanisms.
Estimated lake area loss based on our space‐for‐time substitution and projected permafrost thaw under RCP 8.5. (a) Displays uniform predictions extrapolating negative correlations between lake area and permafrost extent in unglaciated‐fine substrate watersheds to the entire study site (b) shows predictions constrained based on physiographic setting. The stable lake area in Northern Alaska reflects minimal projected permafrost thaw in this region (Figure S9 in Supporting Information S1).
Glacial History Modifies Permafrost Controls on the Distribution of Lakes and Ponds

February 2025

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8 Reads

Eric S. Levenson

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Sarah Cooley

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Andrew Mullen

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[...]

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Jennifer Watts

Plain Language Summary Lakes and ponds are key indicators of the Arctic's vulnerability to rapid warming. Their presence influences the water cycle, wildlife habitat, permafrost temperatures, and the balance between carbon storage and release to the atmosphere. Scientists expect permafrost thaw to cause lake area to decline over time, representing a major shift in the landscape with consequences for ecosystems, water resources, and carbon cycling. The extent of lake drainage across the northern permafrost zone remains unclear, especially given recent studies that have found both increasing and decreasing lake area. Here, we demonstrate that differences in glacial history and geology can explain many of the conflicting trends reported in these previous studies. We show that thawing permafrost tends to reduce lake area in regions without past glaciation. However, in regions shaped by glaciers, lake areas can slightly increase with permafrost thaw. To do this, we use the new the Alaska Lake and Pond Occurrence Data set, which maps over 800,000 lakes and ponds and their seasonal fluctuations in unprecedented detail. We discuss potential mechanisms for long‐term landscape evolution to influence modern lake responses to permafrost thaw. Finally, we use our results to improve projections of future changes to lake area across Alaska.


(a) Auto‐correlation structure of standardized daily evaporation. Dark red line corresponds to mean auto‐correlation coefficient for all grid cells of GLEAM data set (solid line) with 0.1 and 0.9 quantiles (dotted line). Dark blue line, similarly for CAMELE data set. Light blue line, represents the theoretical AR(1) stochastic process, again with 0.1 and 0.9 quantiles. (b) Comparison of different ExEvE definitions for the warm season (April—September) of 2003 over a random grid cell. Red circles correspond to standardized evaporation extremes (above the 0.95 quantile) and blue to the values of the ExEvE using the definition of this study. Rectangles correspond to quantile regression extremes. The ExEvEs for four alternative definitions appear on the bottom of figure. (c) As in panel (b) but for the cold season (October—March) of 2003–2004.
Relationship between evaporation and (a) downward shortwave radiation, (b) downward longwave radiation, (c) precipitation, (d) sensible heat, (e) temperature during ExEvEs and non‐ExEvEs for March, June, September, and December.
Monthly values of mean evaporation, shortwave radiation, longwave radiation, precipitation, sensible heat, temperature on the onset and termination of the ExEvEs and the non‐ExEvEs average. Onset is defined as the first day of the event and termination the day after the last day of the event.
Temporal change of evaporation and its extremes. (a) Annual sum of evaporation for all days of the year, extreme evaporation evants, and non‐extreme evaporation events. Vertical dashed line corresponds to year 2002. (b) As in panel (a), but for intensity. (c) Spatial distribution of ratios of ExEvEs evaporation in 2002–2022 versus ExEvE evaporation in 1981–2001. (d) As in panel (c) but for monthly values over the whole region. Bar plots indicate the ratio of ExEvE evaporation and points the evaporation ratio for all days. Error bars correspond to the 0.01 and 0.99 quantiles.
Changes in water availability over land and water cycle acceleration. Each point pair represents a grid cell. Water availability is estimated by the mean daily residual of precipitation minus evaporation (P − E), and water cycle acceleration/deceleration as the mean monthly land‐atmosphere water exchange P+E2 $\left(\frac{P+E}{2}\right)$ for: (a) All days. (b) Extreme evaporation events. (c) Days with normal conditions. Monthly values for whole Czechia can be found in Supplementary Information (Figure S2 in Supporting Information S1).
On the Definition of Extreme Evaporation Events

February 2025

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19 Reads

Plain Language Summary Evaporation plays a key role in the transfer of water and energy from Earth's surface to the atmosphere. Although the physical processes that govern it are well‐understood, much less is known about its extremes. In this study, a statistical framework is introduced which defines its extremes as individual events with a beginning and an ending. By applying this methodological approach over Czechia, we can see that ExEvEs tend to form clusters of heightened evaporation lasting several days. In summer, these events are linked to sunny, dry conditions, while in winter, they are driven by wet weather and longwave radiation. Since 1981, the frequency and intensity of ExEvEs in Czechia have risen sharply, much more dramatically than overall evaporation. This increase has significant effects on the amount and speed of water exchange between land and atmosphere. The proposed framework provides a systematic way to identify, study, and understand evaporation extremes, shedding light on their causes, effects, and seasonal patterns.


Geometry of the Juno I57 and I58 encounter. The top diagram shows the I57 and I58 trajectories as viewed from Earth. The bottom panels show the cross‐cut as viewed from the north pole for I57 and the south pole for I58. The solid black lines show Juno's trajectory, the light gray lines are radio ray paths through the Alfvén wing, teal lines indicate the times the ray path was affected by the Alfvén wing. In a majority of I57, the occultation begins at the transmit position (Juno's position) within the northern Alfvén wing at a closest distance of 1,225 km from the surface of Io. On I58, Juno is occulted by the entire southern Alfvén wing, but much closer to the surface of Io (radio link at 223 km).
Diagram of the two inversion methods (left: horizontal tubes model, right: ray tracing using concentric cylinders) adopted to do the inversion to electron density, using the I57 trajectory as an example.
Radio occultation observations of the Alfvén wing radio occultation with Juno. The left side are the results from I57 and the right side are the results from I58. The vertical lines marked “ingress” and “egress” show the points where the radio signal was affected by the modeled Alfvén wing defined the text; the middle “center” line marks the time the signal crossed the center of the modeled Alfvén wing axis. The top row (a, b) is the measured differential frequency residual after calibration, overlaid with a 10‐s average. The middle row (c, d) is the Total Electron Content. The bottom row (e, f) is the estimated electron densities using the two methods (Horizontal Tubes and Cylindrical Ray Tracing). The uncertainties, dominated by the sensitivity to the chosen modeled Alfven wing paramers, are the shaded regions in panels (e, f). A gap of ±500 km around the center of the Alfvén wing exists for the ray tracing method due to geometry restrictions, see text for details. Overlaid is the measurements of in‐situ electron densities from the Juno/Waves instrument collected during I57 (Sulaiman et al., 2024), note no density measurements of the Alfvén wing were made with Juno/Waves on I58 because the spacecraft flew outside the Alfvén wing during I58.
Electron Density in Io's Alfvén Wing Observed Via Radio Occultation With Juno

D. R. Buccino

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A. Caruso

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D. Coffin

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[...]

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S. Bolton

Juno performed close flybys of the innermost Galilean moon, Io, in December 2023 (I57) and February 2024 (I58). During these flybys, the radio link connecting the Juno spacecraft to Earth observing stations of NASA's Deep Space Network (DSN) propagated through the Alfvén wing, a magnetospheric feature in which plasma is produced between Io and Jupiter. The radio link is sensitive to the elevated electron densities in the Alfvén wing. A direct measurement of the total electron content was made by a linear combination of Juno's X‐band and Ka‐band downlink frequencies. Two different approaches were used in inverting the measurements into electron densities which assume different electron density distributions within the Alfvén wing. The maximum electron densities estimated in the Alfvén wing were 20,500–27,000 cm⁻³ on I57, in the northern Alfvén wing, and 15,300–31,000 cm⁻³ on I58, in the southern Alfvén wing.


(a) Binary image (black regions refer to the solid phase and white regions indicate the void space) of the non‐eroded (NE) porous medium with a dimension of 7.1×5.3 $1\times 5.3$ mm representing the heterogeneous geometry of real porous medium, adopted from Fakhari et al. (2018). The result of erosion is shown in panels (b) and (c), respectively, showing a zoom‐in into samples M109 (mechanical) and C30 (chemical), both of similar mean pore size, with gray indicating eroded areas. Panel (d) shows the distribution of pore sizes for samples NE, M109, and C30, normalized by the domain length.
Impact of erosion type and flow regime on dispersion coefficients, obtained from numerical simulations. (a) Dispersion coefficient D $D$, normalized by Dm ${D}_{m}$ versus Pe $\mathrm{P}\mathrm{e}$ for different samples. We note that for purely advective transport, normalized D∼Pe1 $D\sim \ {\text{Pe}}^{1}$ (b) Dispersion coefficient D $D$, normalized by λNEuinlet ${\lambda }_{\mathrm{N}\mathrm{E}}{u}_{\text{inlet}}$ versus Pe $\mathrm{P}\mathrm{e}$ to characterize dispersion in terms of its advective part. We note that for purely diffusive transport (i.e., Pe≲ $\mathrm{P}\mathrm{e}\lesssim $0.1) normalized D∼Pe−1 $D\sim \ {\mathrm{P}\mathrm{e}}^{-1}$ (c) The ratio of dispersion coefficients to that in the Non‐Eroded sample. For both cases, dispersion decreases with the erosion at high Pe $\text{Pe}$, while erosion promotes dispersion at low Pe $\mathrm{P}\mathrm{e}$. Vertical dashed lines mark the values of Pe $\mathrm{P}\mathrm{e}$ for which Residence Time Distribution is plotted in Figure 4. Porosities ϕ $\phi $ of the samples are shown for reference. χ $\chi $ refers to calculated tortuosity.
Solute concentration fields from numerical simulation (a) and experiment (b) for mechanically eroded sample M136 at Pe=1.33 $\mathrm{P}\mathrm{e}=1.33$, used for validation of simulation. Colormap corresponds to concentration ranging from 0 to Cinlet ${C}_{\text{inlet}}$. The constructed numerical domain (a) for the validation of the experiment resembles the microfluidic device (b), matching the input and outlet cavities of the micromodel. Experimentally measured concentration map in samples M109 at Pe=1.3 $\mathrm{P}\mathrm{e}=1.3$ (c) and Pe=13 $\mathrm{P}\mathrm{e}=13$ (d) and in M136 at Pe=1.3 $\mathrm{P}\mathrm{e}=1.3$ (e) and Pe=13 $\mathrm{P}\mathrm{e}=13$ (f). Reducing Pe $\mathrm{P}\mathrm{e}$ dampens fingering and eliminates the sharp transversal concentration difference among pores.
Numerically obtained Residence Time Distribution (RTD) for Non‐Eroded, M109, and C30 samples at three different values of Pe $\mathrm{P}\mathrm{e}$, marked in Figure 2. χ $\chi $ is the tortuosity (of velocity streamlines) and L $L$ is the domains' length. At small Pe $\mathrm{P}\mathrm{e}$, diffusion forces dominate the transport, and RTD curves show a non‐Fickian trend with an early breakthrough time and severe tailing. Increasing the value of Pe $\mathrm{P}\mathrm{e}$ shifts transport from the non‐Fickian toward an approximately Fickian regime at Pe $\mathrm{P}\mathrm{e}$ = 5.2. For the highest Pe $\mathrm{P}\mathrm{e}$ the multi‐modal distribution of pore sizes in sample M109 makes the transport regime non‐Fickian with a non‐Gaussian distribution of RTD, caused by the notable diffusive mass flux between high‐ and low‐velocity pathways.
Effect of Pe $\mathrm{P}\mathrm{e}$ on numerically obtained solute migration profile for samples (top) M109, and (bottom) C30. From left to right, panels show Pe $\mathrm{P}\mathrm{e}$ = 0.052, Pe $\mathrm{P}\mathrm{e}$ = 5.2, and Pe $\mathrm{P}\mathrm{e}$ = 520. Compare the concentration in low‐velocity zones for sample M109 at Pe = 0.052 (C/C0≈ $C/{C}_{0}\approx $0.9), Pe = 5.2 (C/C0≈ $C/{C}_{0}\approx $0.5) and Pe = 520 (C/C0≈ $C/{C}_{0}\approx $0.1), highlighted with squares for a few zones. Arrows refer to the formed tailing in the concentration profile. Colorbar shows non‐dimensionalized concentration CC0 $\frac{C}{{C}_{0}}$.
Non‐Monotonic Impact of Erosion on Solute Dispersion in Porous Media

February 2025

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10 Reads

Ali Saeibehrouzi

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Soroush Abolfathi

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Petr Denissenko

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Ran Holtzman

Plain Language Summary Quantifying the dispersion coefficient is one of the most fundamental aspects of transport in porous materials with direct application in energy storage/recovery, or pollutant/nutrient transport in subsurface media. Dispersion arises from the availability of variable flow paths, resulting in a spectrum of transient times that solute particles can experience for transport through porous media. Porous media are often heterogeneous structures with irregular flow paths, making the prediction of solute spreading challenging. In nature, a common phenomenon that impacts the geometry of media is erosion. We analyze solute spreading under single‐phase conditions in media with different degree/type of erosion. We found a non‐monotonic erosion‐dispersion relation. Depending on the transport regime, our investigation shows that erosion can either enhance solute spreading (for diffusion‐dominated transport) or limit it (for advection‐dominated transport). While mechanical erosion through particle migration creates media with a multi‐modal variation in pore size distribution, chemical erosion, which involves particle shrinkage, primarily widens pore spaces without significantly altering the initial pore size distribution. These findings mark a crucial advancement in predicting the fate of injected or released solute species into natural porous media, particularly in the context of ongoing changes in pore space properties driven by erosion.


Spatial distribution of MSEs, seismic array, pumping wells, hydrologic observation wells, and the fault system. (a) Map view. Dots, relocated MSE epicenters colored by event depths (Depth is denoted as H, defined as elevation above the WGS84 geoid); purple triangles, hydrologic observation wells; lines, surface fault traces with tick marks representing dip directions; background image, topography. Other symbols are labeled in the legend. Faults include: RFF, Range Front Fault; NF, Nightingale Fault; FF, Fan Fault; AF, Antithetic Fault; SEF, San Emidio Fault; BBF, Basin Bounding Fault; PF, Piedmont Fault; NWF, NW Fault. (b) East–West cross‐section of the geologic and temperature models by Folsom et al. (2020) at 4,472.9 km Northing. West‐dipping lines, fault traces at depth. Iso‐temperature contours are shown. Geologic units: QTa, Alluvium; QTas, silicified sediments; Ts, tilted and indurated Late Miocene siltstones; Tpb', upper basaltic andesite; Tpts, lower tuffs; Tpts', upper tuffs and tuffaceous sediments; TrJn, Nightingale.
Temporal evolution of plant operations, microseismicity, and fluid pressure throughout the seismic array deployment. Time is relative to the start of shutdown (UTC 13:00 on 18 April 2022). The shutdown period is shaded in dark gray. (a) Pumping rates at production (75B‐16, 25A‐21, 76–16) and injection (53–21, 43–21, 42–21) wells. (b) Microseismicity. Black bars show the number of events per hour (left vertical axis) for the events with magnitude > −0.6. Dots represent event magnitudes (right vertical axis), with those above −0.6 colored red and those below −0.6 colored blue. (c) Distance of MSEs (dots) to the nearest production well as a function of time. Curves show r=Dt $r=\sqrt{D\hspace*{.5em}t}$ with different diffusivity D $D$ values. A zoom‐in view of this panel for the shutdown period is shown in Figure S19 of Supporting Information S1. (d) Fluid pressure changes measured at 11 hydrologic observation wells. Well locations are shown in Figure 1a.
Vertical cross‐sections of event relocations (black dots) and the Vp model along four profiles that are approximately perpendicular to the main fault strikes. (a) Map of the four profiles (white lines). (b, d, f, h) Vp model. (c, e, g, i) Vp model perturbation (in percent) relative to the depth‐averaged 1‐D model. The vertical axis H is defined as elevation above the WGS84 geoid. MSEs within 0.3 km of each cross‐section are shown. Fault traces at the surface and at depth are showed as colored lines, as labeled in the legend. In the cross‐sections, the white‐to‐red and white‐to‐blue lines denote the depth trajectories of the production and injection wells, respectively, with the red and blue parts at the bottom representing the perforated segments. Note that the injection well trajectories shown in panels (f–i) are very shallow. White dashed curves generally outline the well‐resolved parts of the Vp model based on the checkerboard resolution test.
Diagram of induced seismicity due to Pp ${P}_{p}$ diffusion (red arrow) within the reservoir developed along the permeable fault zone (dashed rectangle) during production cessation. The background image is the vertical cross‐section of the Vp model and seismicity from Figure 3f.
Microseismicity Modulation Due To Changes in Geothermal Production at San Emidio, Nevada, USA

February 2025

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1 Read

Hao Guo

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Clifford Thurber

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Erin Cunningham

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[...]

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Kurt L. Feigl

Plain Language Summary Seismic events in the shallow subsurface can be caused by industrial activities, such as pumping operations in geothermal power plants. In recent years, it has been recognized that brief pauses in geothermal production are associated with increased seismicity, a phenomenon that was rarely reported before. The San Emidio geothermal field in Nevada, USA is a natural experiment site to study this phenomenon. In April 2022, a planned power plant shutdown at San Emidio was monitored using dense seismic and hydrologic instrumentation, providing an excellent opportunity to understand its underlying mechanisms. Using data from the dense seismic array with state‐of‐the‐art seismic detection, location, and tomography techniques, we developed a microseismic event catalog with high‐precision event locations and a high‐resolution three‐dimensional P‐wave seismic velocity model. Our results, combined with hydrologic data, support the hypothesis that the cessation of production rapidly increased fluid pressures along pre‐existing fault zones, activating critically stressed fault patches and fractures and producing microseismicity.


Number of dTw days (daily max Tw > 31°C) per year (June–May) in climatology (CLIM), and the anomalous dTw days in the EP Niño composite (EP—CLIM), and the CP Niño composite (CP—CLIM) under the GWTs (1.5, 2, 3, and 4°C) for (a) West Africa, (b) South Asia, (c) East Asia, (d) the Middle East, and (e) Mainland Southeast Asia. Stippling shows where differences are statistically significant at the 90th percentile for more than half of the models based on a 1,000‐member bootstrap ensemble per GCM.
Percentage of total land area experiencing at least 1 day with dTw at each location under the four GWTs. Shades of gray, red, and green represent the seasons during climatological, EP, and CP Niño years, respectively. The lightest (darkest) shade indicates JJA (MAM) season. Seasonal error bars for each El Niño flavor represent one standard deviation determined from the multi‐model ensemble. Red (Green) dashed lines represent the annual total difference between EP (CP) Niño years at a given GWT and the climatology under the next higher GWT.
Population (in millions; following 2050 SSP2 population projections) exposed to at least 1 day with dTw per year (daily max Tw > 31°C) at each location under the four GWTs. Black lines represent the climatology, with the red line indicating EP years and the green line representing CP years. Error bars represent one standard deviation determined from the multi‐model ensemble. Red (Green) dashed lines represent the difference between EP (CP) Niño years at a given GWT and the climatology under the next higher GWT.
El Niño Enhances Exposure to Humid Heat Extremes With Regionally Varying Impacts During Eastern Versus Central Pacific Events

February 2025

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5 Reads

Zachary M. Menzo

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Christina Karamperidou

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Qinqin Kong

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Matthew Huber

Plain Language Summary Humid heat extremes, characterized by high wet bulb temperature (Tw), pose health risks even to young, healthy individuals. While strong El Niño events are known to affect extreme Tw days, the impact of different El Niño types (Central Pacific and Eastern Pacific) has not been well studied. Using historical data and future climate projections, we examined how these El Niño types affect the frequency and spatial extent of dangerous Tw. Our analysis shows that under future warming, Eastern Pacific and Central Pacific El Niño events drive distinctly different, regionally varying patterns of dangerous Tw, yet both significantly increase the affected population and area impacted by humid heat extremes at all global warming levels. Even at low global warming levels, during El Niño events, the population exposed to dangerous Tw is expected to be equal to that exposed regularly when the mean warming is more than four times higher. This highlights the need to consider El Niño diversity in assessing the additional heat stress in heavily populated regions as the planet warms and approaches the critical threshold of heat stress.


Q‐flux forcings applied to a slab‐ocean coupled climate model (left panel; unit of W m⁻²) and the responses of surface temperature (middle left; unit of K), 850‐hPa vertical motion (middle right; unit of Pa s⁻¹), convective precipitation (right panel; unit of mm day⁻¹), averaged during the extended winter months across four major western boundary currents in both hemispheres. The results correspond to the difference between the anomalies obtained in the +2σ $\sigma $ and −2σ $\sigma $ perturbation experiments. Black curves highlight the latitudes with the maximum surface temperature responses. Stippled areas represent regions where results are statistically significant at the 95% level, determined by a two‐sided student's t‐test. Green boxes denote the WBC boundaries.
Responses of zonal‐mean vertical motion (left panel shading; unit of Pa s⁻¹) and condensational heating (right panel; unit of K day⁻¹) to Q‐flux forcings, averaged during the extended winter months across four major western boundary currents in both hemispheres. Stippled areas represent regions where results are statistically significant at the 95% level, determined by a two‐sided student's t‐test.
As in Figure 1, but for the responses of sea‐level pressure (left panel; unit of hPa) and 300 hPa geopotential height (right panel; unit of gpm) to Q‐flux forcings.
Influence of Anomalous Ocean Heat Transport on the Extratropical Atmospheric Circulation in a High‐Resolution Slab‐Ocean Coupled Model

Lantao Sun

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Casey Patrizio

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David W. J. Thompson

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James W. Hurrell

Plain Language Summary We study how ocean heat transport (OHT) influences the atmospheric circulation in the major western boundary currents (WBCs) of both hemispheres, including the Gulf Stream, Kuroshio‐Oyashio Extension, Brazil‐Malvinas Confluence, and Agulhas Currents. We find that the heating due to anomalous ocean heat transport causes air to rise on the equatorward side of the largest surface heating in all WBC regions. The regions of rising air are also associated with more intense convective precipitation. The effect is strongest in the Northern Hemisphere (NH) where the atmospheric response extends to the upper troposphere, leading to significant heating and atmospheric circulation anomalies aloft. The findings highlight the robustness of the atmospheric response to ocean dynamical processes in the western boundary currents, although differences in the hemispheric responses are noteworthy. In the NH WBCs, the atmospheric response to OHT anomalies is balanced primarily through vertical air movement, whereas in the Southern Hemisphere, the response is balanced primarily by low‐level horizontal temperature advection.


(a) GNSS buoy array, GNSS land sites, and Surface Water and Ocean Topography (SWOT) swath track (total width 120 km) during the Fast Sampling Phase (FSP), (b) power spectral density of the mean GNSS and ACCESS‐C wet path delay estimates, (c) Magnitude squared coherence between GNSS and ACCESS‐C (d) Semivariogram for GNSS, ACCESS‐C and ECMWF from the SWOT product. Results from GNSS and ACCESS‐C are averages using coincident hourly data from all nine GNSS buoy locations, and results from ECMWF are averages using daily FSP data from the nine sites.
Surface Water and Ocean Topography (SWOT) swath segments for the four different regions showing power spectral density of residual wet path delay (WPD) from ACCESS‐C minus ECMWF, the SWOT error budget for WPD (black) and sea surface height (red). The regions shown are (a) Carpentaria, pass 006, (b) Davies Reef, pass 019, (c) Albany, pass 008 and 021, and (d) Bass Strait, pass 006 and 019. The Australian North West Shelf region is not covered by ACCESS‐C and so is not included in this analysis.
Residual differences between the Surface Water and Ocean Topography radiometer and the ACCESS‐C and GNSS buoy array in Bass Strait (fast sampling phase, cycles 476 to 577), highlighting the impact of land contamination on the approach to coast. The median radiometer minus ACCESS‐C differences across all cycles is indicated by the orange line, with the residuals from each cycle indicated by the underlying heatmap (showing residual count per bin). The boxplots show radiometer minus GNSS buoy residuals, with the boxes extending from the first to third quantile of the data, the whiskers extending to 1.5 multiplied by the interquartile range, and the central line showing the median values (n = 89 for each box). Distance to coast is from the radiometer measurement (not buoy location). No valid radiometer measurements are available for the most southerly buoy hence this is excluded.
Case studies showing wet path delay features in Bass Strait and Carpentaria. (a)–(c) Bass Strait case, pass 006, cycle 486, 2023‐04‐10 01:02, (a) Sentinel 3A radiance Oa12 “clouds” band, 2023‐04‐09 23:05, (b) Surface Water and Ocean Topography (SWOT) radar backscatter, (c) SWOT sea surface height anomaly (SSHA), (d)‐(f) Carpentaria case, pass 006, cycle 529, 2023‐05‐22 18:11, (d) ACCESS‐C wet troposphere, (e) SWOT radar backscatter, (f) SWOT SSHA. Black dashed lines in each are the SWOT swath extents, black circles in panels (a)–(c) are the GNSS buoy array, and black arrows in panels (d)–(f) indicate the frontal feature captured in each data set.
Small Scale Variability in the Wet Troposphere Impacts the Interpretation of SWOT Satellite Observations

February 2025

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4 Reads

Andrea Hay

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Christopher Watson

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Benoit Legresy

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[...]

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Jack Beardsley

Plain Language Summary The new Surface Water and Ocean Topography (SWOT) mission is the first satellite altimeter to observe changes in the height of the sea surface over broad swaths at high resolution. To obtain high accuracy measurements various corrections are needed for the raw radar measurements. One of the required corrections accounts for the water vapor in the atmosphere which delays the radar signal. Although SWOT sea surface measurements are at high resolution, the correction available for the water vapor in the atmosphere is at a lower resolution, which could possibly affect interpretation of SWOT observations. Here we use a high‐resolution atmospheric model and a set of GNSS buoys to investigate the variations of atmospheric water vapor over shorter distances in Australian coastal waters. We find that the variation is higher than the SWOT error budget and that a higher‐resolution correction for moisture in the atmosphere is often needed to ensure the correct interpretation of SWOT observations.


Map of the study area (55–80°W, 57–70°S) with subregions Drake Passage (yellow), Northern Shelf (red), Mid Shelf (green), and Southern Shelf (cyan), showing (a) bathymetry, (b) mean satellite‐derived Chl‐a 1997–2022, and (c) ship track locations for underway pCO2 data 2000–2020.
Seasonal cycles of Chl‐a, ∆pCO2, and pCO2sur with thermal and non‐thermal components 2000–2020 showing Chl‐a (a–d), ∆pCO2 (e–h), and pCO2sur (i–l) for the Drake Passage (a, e and i), Northern Shelf (b, f and j), Mid Shelf (c, g and k), and Southern Shelf (d,h,l) subregions. (See Figure S3 in Supporting Information S1 for ∆pCO2 as in e‐h with regionally scaled y‐axes). Error bars represent ±1 standard deviation.
Seasonal Variability of Surface Ocean Carbon Uptake and Chlorophyll‐a Concentration in the West Antarctic Peninsula Over Two Decades

February 2025

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17 Reads

Jessica S. Turner

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David R. Munro

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Amanda Fay

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[...]

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Heidi Dierssen

The Southern Ocean plays a vital role in global CO2 uptake, but the magnitude and even the sign of the flux remain uncertain, and the influence of phytoplankton phenology is underexplored. This study focuses on the West Antarctic Peninsula, a region experiencing rapid climate change, to examine shifts in seasonal carbon uptake. Using 20 years of in situ air‐sea CO2 flux and satellite‐derived Chlorophyll‐a, we observe that the seasonal cycles of both air‐sea CO2 flux and Chlorophyll‐a intensify poleward. The amplitude of the seasonal cycle of the non‐thermal component of surface ocean pCO2 increases with increasing latitude, while the amplitude of the thermal component remains relatively stable. Pronounced biological uptake occurs over the shelf in austral summer despite reduced CO2 solubility in warmer waters, which typically limits carbon uptake through physical processes. These findings underscore the prominence of biological mechanisms in regulating carbon fluxes in this rapidly changing region.


(a) Position of three spacecraft THEMIS A, D, and E, four spacecraft MMS and four spacecraft Cluster at 19:10:00UT in the geocentric solar magnetospheric (GSM) coordinate system. The four spacecraft MMS and Cluster 3 and 4 are close to each other on this spatial scale and are represented by only one point. (b) The Cooling analysis of the Flux Transfer Event motion from a predicted sub‐solar magnetic reconnection X‐line, which shows the YZ plane viewed from the sun. (c) and (d) TH‐A and TH‐D magnetic field components. (e) TH‐D ion energy flux spectrogram. (f–g and h–i) Magnetic field and ion energy spectrogram of TH‐E and MMS1, respectively. (j) and (k) Cluster C4 magnetic field in GSM coordinate system and H+ energy flux spectrogram. All the vectors of THEMIS and MMS are presented in boundary normal coordinate system LMN, where N is the magnetopause normal. Relative to GSM coordinates, L = (−0.15, −0.10, 0.97), M = (0.52, −0.83, 0), and N = (0.83, 0.52, 0.18) for THEMIS; L = (−0.21, −0.20, 0.91), M = (0.65, −0.69, 0), and N = (0.69, 0.65, 0.30) for MMS. The center of FTE1 and FTE2 are denoted by vertical dashed black and blue lines, respectively.
The panels show the magnetic field, electron spectrograms of energy flux and high energy (>1 keV) pitch angle distribution of TH‐A, TH‐E, and MMS1, respectively.
Schematic diagram of FTE1 which captures the 3‐D geometric structure, orientation and trajectory of the Flux Transfer Events (FTEs) across the magnetopause. The light blue solid lines represent the magnetic field lines of the magnetosphere (MSP); the green solid lines represent the interplanetary magnetic field; the green dashed lines represent the predicted reconnection X‐lines; the blue and red solid lines represent the open field lines connecting magnetosheath (MSH) to the northern hemisphere and the closed field lines connecting the northern and southern hemispheres in FTE, respectively.
Global Three‐Dimensional Structure of Flux Transfer Events: THEMIS‐MMS‐Cluster Coordinated Observation

February 2025

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3 Reads

T. Yang

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X.‐C. Dong

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M. W. Dunlop

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[...]

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J.‐B. Cao

We present consecutive observations of Flux Transfer Events (FTEs) on 10 November 2020, using MMS, THEMIS and Cluster spacecraft located at different magnetopause locations. Two typical scale FTE signatures are successively observed by low‐latitude THEMIS, mid‐latitude MMS and high latitude Cluster, reflecting their global spatial scale characteristics. Multi‐spacecraft observation also revealed the complete 3‐D structure of the FTEs, with azimuthal extended section, magnetosheath and magnetospheric arm. The simultaneous existence of different magnetic field line topologies during the FTEs indicates the generation mechanism of multiple X‐line reconnection. Successive observations with intervals of several minutes revealed some evolutionary features of FTEs, including an increase in size and flux, and disappearance of the magnetic dip region on both sides. Our observations give a complete 3‐D picture of FTEs on a global scale, which can improve our understanding of the transient magnetic reconnection and solar wind‐magnetosphere interaction at the magnetopause.


Location of the Zuoqiupu ice core drill site. The cyan square marks the drill site. The background color represents the spatial distribution of annual mean Aerosol Optical Depth (AOD) for 2010 (Hsu, 2013). Circles, scaled by glacier area, indicate negative (pink) and positive (blue) glacier elevation change rates between 2000 and 2019 (Hugonnet et al., 2021). The dashed rectangles mark the region (65–110°E, 10–30°N) from which the time series of mean SPEI (Standardized Precipitation‐Evapotranspiration Index) is calculated (see Figure 3).
Time series of ƒbiomass (fractional contribution of biomass burning) in the Zuoqiupu ice core (1959–2012). The time series shows annual ƒbiomass values derived from radiocarbon content of black carbon. The horizontal purple dashed lines indicate the decadal mean levels.
(left) EEMD components (c1–c5) of ƒbiomass (fractional contribution of biomass burning), the sum of c1–c3, and the annual ƒbiomass series. (right) Linkages between ƒbiomass from the Zuoqiupu ice core, South Asian wildfire‐emitted black carbon (WF‐BC), and climate oscillations (1959–2012). (a) MEI (Multivariate ENSO Index), (b) EEMD‐detrended ƒbiomass (sum_c1–c3) anomaly, (c) detrended WF‐BC anomaly in South Asia, (d) SPEI (Standardized Precipitation‐Evapotranspiration Index) (annual mean from the region in Figure 1), and (e) detrended Pacific Walker circulation (PWC) index anomaly (1959–2012). Y‐axes for SPEI and PWC are reversed. MEI, WF‐BC, SPEI, and PWC are 5‐year running means, and ƒbiomass (sum_c1–c3) is a 3‐year running mean. Red asterisks mark simultaneous peaks across the series.
Black carbon (BC) deposition flux and source apportionment from fossil fuel versus biomass combustion before and after 1990. The pie charts, scaled by BC deposition flux, show the contributions of fossil fuel (brown) and biomass burning (green). The average deposition flux increased from 9.0 ± 3.4 mg m⁻² year⁻¹ before 1990 to 14.5 ± 4.0 mg m⁻² year⁻¹ after 1990. Before 1990, fossil fuel combustion contributed 76% of BC, while biomass burning accounted for 24%. After 1990, fossil fuel's contribution dropped to 70%, and biomass burning rose to 30%, mainly due to more climate‐driven wildfires.
Radiocarbon Fingerprinting Black Carbon Source History in the Himalayas

February 2025

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2 Reads

Mo Wang

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Hailong Wang

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Baiqing Xu

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[...]

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Jun Li

Black carbon (BC) is considered as an important contributor to the Himalayan glaciers melt in the past few decades. However, the long‐term source apportionment of BC remains unclear. Here we present the first radiocarbon (¹⁴C)‐based annual variation of BC source apportionment in an ice core spanning the period of 1959–2012 drilled from the Southeastern Tibetan Plateau, a receptor site of South Asia outflow. We find fossil fuel combustion is a major contribution (73% ± 5%), yet the biomass burning fraction (ƒbiomass) has grown from 24% ± 4% to 30% ± 4% since 1990. Intriguingly, we further find the ƒbiomass demonstrating a robust correlation with South Asian wildfires linked to climate oscillations. Thus, for mitigating BC impacts on Himalayan glaciers, South Asia's transition from fossil fuels to clean energy is a more efficient and urgent strategy than reducing residential biomass burning.


Example of a triplet of images of a snow aggregate, collected by a MASC. The best fitted ellipse of each image is drawn in green, with the major axis defining the apparent orientation with respect to the horizontal.
Evaluation of the retrieval of orientation that could be achieved with a triplet of MASC images, conducted using simulated data (ellipsoids in the left column, simulated snowflakes in the right column). (a and c) Distribution of orientation value, both reference and reconstructed. (b and d) Letter‐value plots for the error distribution of the orientation (in absolute value, not sign dependent). The simulations are conducted on 10,000 ellipsoids of various geometry as well as on 10,000 aggregates.
Histogram of the distribution of orientation value for all data (412,150 particles, top) and data stratified according to the instrumental setup (bottom) either being unsheltered (274,839 particles) or deployed within a double‐fence inter‐comparison reference (DFIR, 137,311 particles). The dotted lines illustrate the shape of a Gaussian curve having the same mean and standard deviation as the observed data, and are given to provide a visual comparison of the difference with respect to a Gaussian shape (it is not a fit of the histogram). Orientation values are estimated as the sign‐preserving mean of the three MASC views.
Evolution of the standard deviation of the distribution of orientation values at various wind speed levels and stratified according to the instrumental setup. The bottom panel shows the number of observations falling into each bin of wind speed.
Violin plot (distribution) of orientation values stratified according to different hydrometeor types. The data correspond to observations collected within a DFIR (Figure 4), for low horizontal wind (about 47,000 observations for wind <4 ${< } 4$ ms−1 ${\text{ms}}^{-1}$) and high horizontal wind (about 36,000 observations for wind >8 ${ >} 8$ ms−1 ${\text{ms}}^{-1}$). Data are stratified in two classes of axis ratio (a_r) limited by the median axis ratio value of the entire population. The number of observations in each distribution ranges between a minimum of 500 (planar crystals, low axis ratio, low wind) and a maximum of about 15,000 (aggregates, low axis ratio, low wind).
Observation of the Orientation of Snow Hydrometeors at Sheltered and Unsheltered Sites

February 2025

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3 Reads

J. Grazioli

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M. Condolf

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Y.‐A. Roulet

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[...]

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A. Berne

Knowledge about orientation of falling snow is still poorly documented with field measurements despite its importance, for example, in the interpretation of remote sensing data. This study investigates the orientation of snow hydrometeors using data from a Multi‐Angle Snowflake Camera. We explore the impact of different observational setups (sheltered vs. unsheltered), wind speed, hydrometeor type, and axis ratio on the orientation distributions. Numerical simulations are used to select the best orientation estimator and to understand the reason behind contrasting results reported in past literature. We find that previously reported non‐zero median orientations are likely artifacts due to averaging absolute values of orientations from the three individual cameras. Observed orientations generally follow a symmetrical distribution around 0° {}^{\circ}, with broader distributions observed at unsheltered sites and/or high wind conditions. Observed distributions may vary significantly from those assumed in previous studies, highlighting the need for further research on hydrometeor orientations under varying environmental conditions.


Seismic rupture propagating through a strike‐slip fault (symmetrically) surrounded by a more compliant damage zone of thickness 2H $2H$. The geometry of the problem and its two end‐member situations involve (a) crack‐like rupture for homogeneous elastic properties between the damage zone and the wall rock; (b) pulse‐like rupture for large elastic contrast between the compliant damage zone and the stiffer wall rock. The red curves represent instantaneous slip rate in each case, as derived from a two‐dimensional elastodynamics model. The top and bottom color maps represent respectively the near‐tip profiles of shear stress and velocity shown with the same scaling for the two end‐members. More details on the simulated problem and conditions are provided in Section 3.1 and Figure S2 in Supporting Information S1.
Sketch illustrating the proposed minimal elastodynamic model. A strip of low seismic velocity damage zone of thickness 2H $2H$ surrounds a fault, situated within a stiffer wall rock. Due to the symmetry of the problem, only the upper half of the system is modeled. Rupture style is controlled by ζ¯ $\bar{\zeta }$, a non‐dimensional parameter that compares the relative stiffness of the wall rock k¯ $\bar{k}$, the radiation damping η¯ $\bar{\eta }$, and the prestress τ¯k ${\bar{\tau }}_{k}$. In the overdamped regime, ζ¯>1 $\bar{\zeta } > 1$, slip rate decays in the wake of the rupture toward finite positive values leading to a crack‐like rupture. In the underdamped regime, ζ¯<1 $\bar{\zeta }< 1$, the harmonic vibration of the compliant damage zone leads to transient negative slip rates, which promote self‐healing pulse‐like rupture.
Phase diagram predicting the propensity of damaged faults to rupture with crack‐like versus pulse‐like dynamics tested against two‐dimensional elastodynamics simulations. (a) Phase diagram comparing the steady‐state regime (Equation 8) predicted by the minimal model—depicted by the background color map—to the behavior observed in full‐field simulations. The latter are depicted by symbols that are either blue crosses if the average slip rate u¯˙ $\dot{\bar{u}}$ observed in the wake of the rupture changes sign (underdamped regime) or red pluses otherwise (overdamped regime). The bi‐color spheres highlight cases near the critical damping ratio whose classification is not obvious and/or depends on the nucleation conditions. Representative ranges for the estimated Δv ${\Delta }v$ of natural faults zones are shown for San Andreas (Huang et al., 2014; Lewis & Ben‐Zion, 2010; Li et al., 2006), Little Lake (Zhou et al., 2022) and North Anatolian (Ben‐Zion et al., 2003a; Huang et al., 2014) faults. Two examples of the slip rate profile observed in the numerical simulations for the underdamped and overdamped regimes are shown respectively in panels (b) and (c) in comparison with the one‐dimensional theory—corresponding to Equation (S31) in Supporting Information S1. The red and blue lines in panels (b) and (c) correspond to the profiles of slip rate averaged across the damage zone observed at different times in the two‐dimensional simulations, respectively for no healing and instantaneous healing conditions. See the main text for further explanations.
A Minimal Model Illuminates the Physics of Pulse‐Like Seismic Rupture and Oscillatory Slip Rates in Damaged Faults

February 2025

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7 Reads

Fabian Barras

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Einat Aharonov

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François Renard

Plain Language Summary Seismic ruptures—that initiate rapid slip along tectonic faults during earthquakes—are known to propagate with two different styles; either as crack‐like ruptures, analogous to fracture in brittle materials, or as pulse‐like ruptures, where the motion of the fault resembles the crawling of a caterpillar. The reason why some seismic ruptures are predominantly pulse‐like is a central question in earthquake science that impacts our understanding of how faults operate, of how seismic ruptures move and arrest and, thereby, of what controls the size of an earthquake and the hazard that it poses. The difficulty in answering these questions often ties to the complexity of the processes involved during seismic ruptures and the limited ways to observe them at several kilometers depth. This work proposes a generic model, with a minimal number of parameters, to study and predict the style of seismic ruptures. The domain near tectonic faults often comprises densely fractured rocks, and our generic model illuminates how the reduction of stiffness in this damaged region directly impacts the seismic rupture style. Our model also predicts that slip direction could be reversed in the wake of a pulse‐like rupture, a process that can create additional damage.


Spatial distribution of NDVIMA from 2000 to 2022 and areal proportion of each normalized difference vegetation index level (a) Based on Theil‐Sen median trend analysis and Mann‐Kendall test, trends of NDVIMA over the SSH from 2000 to 2022 with the areal percentage of each trend type (b) in the whole region and subregions.
Elevation‐dependent pattern of multi‐year average normalized difference vegetation index (NDVI) and the greening rate with the relative changing rate (RCR) of NDVI at different elevation ranges. (a, b) In the whole region, (c, d) Eastern Himalaya, (e, f) Central Himalaya, and (g, h) Western Himalaya. The dashed line and dash‐dot line indicate the decline of NDVIMA values and the rising range of the greening rate at high elevation ranges, respectively. The RCR was calculated by dividing the slope of the greening rate by the NDVIMA at each elevation zone.
(a) Elevation‐dependent partial correlation coefficients of the NDVIMA with air temperature and total precipitation in different subregions. *, **, *** indicate significance at p < 0.05, p < 0.01, and p < 0.0001, respectively. (b) Spatial and temporal distributions of the partial correlation between NDVIMA and climate factors (air temperature and precipitation).
Elevation‐Dependent Vegetation Greening and Its Responses to Climate Changes in the South Slope of the Himalayas

February 2025

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19 Reads

Hamza Mukhtar

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Yujia Yang

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Mengjiao Xu

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[...]

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Wei Zhao

Plain Language Summary The South Slope of the Himalayas (SSH), known for its unique biodiversity and complex role in climate regulation, is undergoing noticeable changes in vegetation due to climate change. Due to diverse climatic environments and abrupt elevational variations, this region has different vegetation zones. However, there remains a gap in comprehensive studies addressing these changes. To fill this gap comprehensively, we utilized Normalized Vegetation Difference Index (NDVI) from 2000 to 2022 to analyze variations in naturally vegetated surface across the elevation and their correlation with climate. Our results revealed a significant increase in vegetation greenness across SSH and subregions (except Eastern Himalaya (EH)). The relative change rate (RCR) of NDVI indicated stronger vegetation growth at higher elevations from ∼2,600 to ∼5,000 m, followed by a decline in all subregions. Interestingly, further analyses revealed a warming induced vegetation growth in highland areas across the region, while lowland region faced heat stress in the Central Himalay (CH), and Western Himalaya (WH). Conversely, precipitation promoted vegetation in the middle‐elevated areas, although EH faced waterlogging stress. These contrasting responses, patterns, and trends in vegetation changes in the Himalayas highlight the need for a comprehensive understanding of specific spatial variations when devising climate change adaptation strategies.


(a) The SYM‐H and AL indices, (b) the solar wind pressure and IMF Bz in geocentric solar magnetospheric coordinates, (c, d) the phase space density (PSD) of protons with μ=10 $\mu =10$, and 50MeV/G $50\text{MeV}/\mathrm{G}$ and K=0.24G1/2RE $K=0.24{\mathrm{G}}^{1/2}{\mathrm{R}}_{\mathrm{E}}$ as a function of L∗ ${L}^{\ast }$ and time from 24th to 26th June 2017, (e) an example showing how to identify the deepening PSD minima, and (f, g) the PSD of protons as a function of L∗ ${L}^{\ast }$ for inbound/outbound passes of both Probes.
(a, b) The number of valid samples and deepening phase space density (PSD) minima, and (c) the occurrence rate as a function of μ $\mu $ and K $K$; the distribution of deepening PSD minima as a function of (d) L∗ ${L}^{\ast }$, (e) L∗−Lppall ${L}^{\ast }-{L}_{pp}^{all}$, and (f) L∗−Lpp>12 ${L}^{\ast }-{L}_{pp}^{ > 12}$, where Lppall ${L}_{pp}^{all}$ and Lpp>12 ${L}_{pp}^{ > 12}$ are the estimated plasmapause location based on the MLT‐dependent model in Liu et al. (2015); the median values of (g) L∗ ${L}^{\ast }$ of deepening PSD minima, (h) L∗−Lppall ${L}^{\ast }-{L}_{pp}^{all}$, and (i) L∗−Lpp>12 ${L}^{\ast }-{L}_{pp}^{ > 12}$ in each μ $\mu $‐K $K$ bin. In panels (d–f), the median value and quartiles are marked by red and gray dashed lines, respectively. In panels (g–i), the contours of the occurrence rate shown in panel (c) are plotted.
(a, b) The number of valid samples and deepening phase space density minima, and (c) the occurrence rate as a function of μ $\mu $ and K $K$ at different levels of geomagnetic activity.
(a, b) The number of valid samples and deepening phase space density minima, and (c) the occurrence rate as a function of μ $\mu $ and K $K$ at different levels of solar wind dynamic pressure.
The median values of (a) pitch angle, (b) kinetic energy, and (c) parallel energy in each μ $\mu $‐K $K$ bin. In panels (b, c), the white lines are the contours of the occurrence rate shown in Figure 2c.
Observations of Fast Local Loss of High‐Energy Ring Current Protons Associated With Deepening Local Minimum in Phase Space Density

February 2025

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11 Reads

Plain Language Summary Precipitation loss plays a major role in removing ions from the ring current and is a key reason why the ring current decays quickly during geomagnetic storms. Understanding the evolution of proton precipitation loss is critical to better understanding the ring current dynamics. Recent observations show the development of a notable reduction in phase space density (PSD) radial profiles, called deepening PSD minima, indicating fast local precipitation loss potentially caused by wave‐induced scattering. In this study, we present a comprehensive analysis of the evolution of ring current protons in Earth's inner magnetosphere, specifically focusing on these deepening PSD minima. Using >6 years of observations from the Van Allen Probes, we show that the overall occurrence rates of proton deepening PSD minimum peaks at ∼3%, mainly located at ∼4.5–5.0 Earth radii. The occurrence rate increases with increasing levels of geomagnetic/solar wind conditions. Theoretical calculations indicate that these protons with deepening PSD minima can resonate with electromagnetic ion cyclotron (EMIC) waves, a major type of plasma waves in Earth's magnetosphere. As a result, our study suggests that EMIC waves are the likely cause of the deepening PSD minima and contribute to the fast local loss of ring current protons.


Arctic map and sampling site. (a) Northern Hemisphere ice‐sheet extent at 13 kyr BP (Peltier et al., 2015). The orange arrows represent the possible pathway of the Younger Dryas flood, originating from Lake Agassiz (indicated by a box in this figure). Red and white arrows depict the warm Atlantic inflow to the Nordic Sea and the main bottom currents. (b) Map of sampling site. Core ARA04C/37 is marked with yellow star, while other sediment cores are shown as black dots. White arrows illustrate surface water circulation in the southern Beaufort Sea.
Younger Dryas flood signals from core JPC15 (Keigwin et al., 2018) and ARA04C/37 (Wu et al., 2020). (a) δ¹⁸O values of Neogloboquadrina pachyderma; (b) FC32 1,15, fractional abundance of C32 1,15‐diol; (c) mass accumulation rate of brGDGTs; (d) δ²H values of brassicasterol and dinosterol; and (e) long‐chain FAs.
Relationships between δ²H and sea surface salinity. (a, b) Derived relationships of δ²Hwater versus salinity in the Canadian Arctic and the Eurasian Arctic. δ²Hwater are derived from δ¹⁸O values in surface water (0–10 m) (Schmidt et al., 1999). (c) Predicted relationship of δ²Hdino versus salinity for the Beaufort Sea, based on the relationship of δ²Hwater versus salinity from the Eurasian Arctic.
Laurentide‐Greenland Ice Sheet extent and δ²H values of dinosterol and brassicaterol. (a) The extent of Laurentide‐Greenland Ice Sheet (Dalton et al., 2020). (b, c) δ²H values of dinosterol and brassicaterol in core ARA04C/37. ΔS are the relative changes in estimated salinity. (d) Lithology and sedimentary texture; gray section indicates finely laminated sediments, orange section bioturbated silty clay (Wu et al., 2022).
Quantitative Estimates of Younger Dryas Freshening From Lipid δH Analysis in the Beaufort Sea

February 2025

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91 Reads

Plain Language Summary The Younger Dryas (YD) cold event is thought to have been triggered by a weakening of the Atlantic Meridional Overturning Circulation, driven by an influx of freshwater into the North Atlantic Deep Water formation region. Determining the source, timing, and magnitude of this freshwater input is critical for understanding the associated climate change. In this study, we analyzed the hydrogen isotopic composition of various lipids in a sediment core from the Canadian Beaufort Sea to investigate these hydrological changes. Our results show that terrestrial leaf wax lipids and microalgae lipids recorded distinct freshwater signals during the YD, allowing for a better constraint on the source and magnitude of this freshening. Using an established empirical relationship between lipid hydrogen isotopes and sea surface salinity, we estimated that surface waters in the Canadian Beaufort Sea experienced a substantial salinity reduction of approximately 15–24 during the YD. This significant decrease was likely caused by a combination of a freshwater outburst and the Laurentide Ice Sheet (LIS) melting water discharge. Following the LIS retreat, the δ²Hlipid indicates that the region likely experienced a shift toward a drier climate during the mid‐to‐late Holocene (∼8–0 cal. kyr BP).


(a) Regional Kmex ${K}_{\mathit{mex}}$ index covering the full storm period and (b) the estimated variations in the horizontal component of the geomagnetic field in Mexico, ΔH ${\Delta }H$.
Observed (blue) and calculated geomagnetically induced currents (red) at three substations of the Mexican 400/230 kV power grid.
Maximum estimated geomagnetically induced currents (GIC) in all the substations considered in the 400/230 kV power grid. Magnetic observatories/stations are marked as black dots, and GIC sensor sites are marked with circles. 400/230/115 kV power lines are marked in different styles. The wind rose show the directional histogram of the induced E‐field along the central Mexican territory during the event.
The Impact of Geomagnetically Induced Currents (GIC) on the Mexican Power Grid: Numerical Modeling and Observations From the 10 May 2024, Geomagnetic Storm

February 2025

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6 Reads

This study examines the impact of the 10 May 2024, geomagnetic storm on the Mexican power grid, utilizing geomagnetically induced currents (GIC), measurements and regional magnetic field data recorded by the Laboratorio Nacional de Clima Espacial. Significant GIC were observed at three different locations within the grid. The observations were complemented with estimates for the Mexican power grid provided by a numerical model developed in late 2022. Our findings suggest that the GIC can pose a potential threat to low‐latitude power grids during extreme geomagnetic disturbances. Furthermore, the model demonstrates its potential to forecast the grid response during these events, providing critical insight into the behavior of the electrical grid during extreme space weather events.


The main pipeline and schematic depiction of Nowcastingformer encapsulate three essential components: embedding, encoder, and decoder. Diverse inputs are individually embedded through distinct branches and subsequently fused by a cross‐attention block, resulting in compressed tensor representations. These tensors undergo refinement through multiple stacked self‐attention blocks and are ultimately fed into the decoder to generate predictions.
Quantitative assessment of the performance of various models for two‐hour nowcasting with thresholds of 20, 30, and 40 dBZ, depicted as functions of lead time, with error bars representing the standard deviation (std). Panels (a1–a3) display the critical success index with corresponding error bars. Panels (b1–b3) present the Fractional Skill Score with a radius of 5 km, also accompanied by error bars. Panels (c1–c3) showcase the Probability of Detection with std error bars. Panels (d1–d2) are the Root Mean Squared Error and Mean Absolute Error, respectively, both including error bars to indicate the standard deviation.
Bar chart summarizing the distributions of importance metrics for atmospheric variables at lead times of 60 and 120 min, with results from the permutation experiment normalized by the no‐permutation metric.
A comparison between models is shown at four future time steps: the first row presents the observation, the second row displays nowcasting from pySTEPS_blending, nowcasting from the DL model, utilizing only radar reflectivity shown from the third row to the sixth row, and the seventh and eighth rows correspond to nowcasting from experiments with pre‐training and pre‐training + multi‐source, respectively. Area A and B are investigated areas.
Heatmaps obtained using IG $IG$. The heatmap of the temperature (°C) at 850 hPa level can be found in left with the trough area enclosed by a blue rectangle. The heatmap illustrating the horizontal winds at the 500 hPa level is presented in right, where blue arrows and “+” Marks indicate positive curvature.
Enhancing Nowcasting With Multi‐Resolution Inputs Using Deep Learning: Exploring Model Decision Mechanisms

February 2025

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8 Reads

Yuan Cao

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Lei Chen

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Junjing Wu

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Plain Language Summary As a sophisticated monitoring tool, weather radar occupies a pivotal position in convective nowcasting. While numerous contemporary deep learning approaches predominantly concentrate on refining network architectures using radar reflectivity as the sole input, the impact of atmospheric physical information on nowcasting remains underexplored. To incorporate the contextual backdrop of atmospheric states in nowcasting, we devise a comprehensive deep learning framework that integrates atmospheric variables across multiple levels. To enhance generalization, we employ a transfer learning strategy to extract generalized spatialtemporal features. Rather than emphasizing a specific network design, we underscore the advantages of harnessing multi‐source data and the decision mechanism of the model. By fusing atmospheric variables and radar reflectivity, and adopting a pre‐training and fine‐tuning approach, we achieve more reliable and resilient nowcasting. Overall, our successful implementation of transfer learning within this multi‐modal model offers promising insights for advancing the field of nowcasting.


Summer Arctic Sea‐ice concentration (SIC) Fresh Water Mode. (a) Spatial pattern of SIC related fresh‐water forcing obtained by combining the dominant modes obtained through Empirical Orthogonal Function analysis (EOF1+EOF2+EOF3). (b) Associated time series index (PC1+PC2+PC3).
AMOC‐SST modes. The pattern of AMOC‐SST (degree) (a), AMO‐SST (degree) (c) and Trend‐SST Mode (degree) (e) together with the associated time series (b, d, f) derived with the empirical orthogonal function method applied to the North Atlantic (75°W‐20°E, 0°N‐80°N) annual SST fields (HadISST 1). In panel (b) the green line (SST Caesar) represents an atlantic meridional overturning circulation time series from (Caesar et al., 2018), highly correlated with the AMOC‐SST time series index derived here (correlation of 0.79). The red line is a linear fit of the MOC data from the RAPID 26°N array (Smeed et al., 2018).
Causality analyses: Convergent cross mapping (CCM). Panel (a) contains Time Delay CCM, that is, cross‐map skill as function of time lag for AMOC‐SST xmap Sea‐ice Concentration (SIC) (red line) with a peak of the cross‐map skill at negative lag (red vertical line). Adjacently, panel (b) displays the convergent cross‐map skill as a function of Library size, mapping from AMOC‐SST to SIC (red line). Panel (c) contains Time Delayed Convergent Cross Mapping (TDCCM) for AMO‐SST xmap SIC (blue line) with a maximum of the cross‐map skill at a slightly positive lag (blue vertical line). Complementarily, panel (d) shows the convergent cross‐map skill from AMO‐SST to SIC. Panel (e) contains the TDCCM for Trend‐SST xmap SIC (yellow line) together with its negative lag (yellow vertical line). Panel (f) shows CCM analysis for the Trend‐SST xmap SIC direction. Gray shaded areas in panels (b), (d), (f) represent statistically significance levels computed under Ebisuzaki and Swap models. Black points on each TDCCM show the statistically significant lags.
Tracing the Observed Causal Impact of Diminishing Summer Sea‐Ice Concentration on the Atlantic Meridional Overturning Circulation

February 2025

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13 Reads

Plain Language Summary A major ocean current system called the Atlantic meridional overturning circulation (AMOC) is slowing down. The AMOC plays a crucial role in regulating Earth's climate by distributing heat across the globe. While computer models suggest that the melting of Arctic sea‐ice, caused by human activities, is leading to this slowdown, there hasn't been conclusive observational evidence to confirm this link. In our study, we provide such evidence that the reduction of Arctic sea‐ice, especially during the summer months, is causing the SST fingerprint of AMOC to weaken. We analyzed data from the past century and found that this effect was particularly strong between the 1950s and 1980s, a period known for significant changes in ocean salinity called the Great Salinity Anomaly. Using advanced analytical methods, we showed that decreases in sea‐ice lead to changes in the AMOC‐SST, but with a delay of one to three decades. Our findings are important because they confirm the link between human‐induced sea‐ice loss and changes in major ocean currents. This enhances our understanding of climatic forcing factors and helps inform policy decisions aimed at mitigating these effects.


Simulation parameters: The magnetic field strength B0 $\left({B}_{0}\right)$ and magnetic flux line (white solid lines). Here, the red points represent the location where the magnetic field is minimized in each L‐shell.
Wave solutions at (a–d) L=8 $L=8$ and (e–h) L=9 $L=9$, respectively. From left to right, the electric field in the direction perpendicular to the magnetic field in the meridian plane Eη $\left({E}_{\eta }\right)$, in the azimuthal direction Eϕ $\left({E}_{\phi }\right)$, the field‐aligned Poynting flux S‖ $\left({S}_{\Vert }\right)$, and the ellipticity (ϵ) $({\epsilon})$, respectively. The electric field and the Poynting flux are normalized with respect to the maximum values of the total electric field strength Emax $\left({E}_{\text{max}}\right)$ or the total Poynting flux strength Smax $\left({S}_{\text{max}}\right)$. For Poynting flux, positive and negative values are parallel and antiparallel directions, and for the ellipticity, +1 (red color), −1 (blue), and 0 (green) indicate circularly right‐handed, left‐handed, and linear polarization, respectively.
Superposition of the wave solutions at L=8 $L=8$, 8.5, 9.0, 9.3, 9.7, and 10; (a) Normalized field‐aligned Poynting flux and (b) Ellipticity (ϵ) $({\epsilon})$. Here, the dashed lines are traces of the virtual spacecraft, and the solid pink line indicates the Shabansky orbit (c)–(e) Measured Poynting flux and ellipticity of EMIC waves generated at three virtual spacecraft. The gray shades in (c)–(e) are the source locations of L=9.7 $L=9.7$, 8.5, and 8, respectively. Here, R=r2+z2 $R=\sqrt{{r}^{2}+{z}^{2}}$ is the geocentric distance, and λ $\lambda $ is the magnetic latitude.
MMS2 EMIC wave observations from 2015‐10‐28/14:30 ‐ 17:15 UT, showing (a) normalized field‐aligned Poynting flux mirrored to the northern hemisphere and (b) Ellipticity. Quantities are shown in the same format as Figures 3c–3e, as a function of geocentric distance (R) $(R)$ and an absolute value of magnetic latitude (|λ|) $(\vert \lambda \vert )$. The wave source region inferred by Vines et al. (2019) is shown by the gray‐shaded region.
Propagation of EMIC Waves From Shabansky Orbits in the Dayside Magnetosphere

February 2025

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4 Reads

Plain Language Summary Electromagnetic ion cyclotron (EMIC) waves, with frequencies ranging from 0.1 to 5 Hz, are commonly found in Earth's magnetosphere. These waves can be detected in the outer dayside magnetosphere, where the interaction between Earth's magnetic field and the solar wind causes the magnetic field lines to compress. EMIC waves can be generated at points where the magnetic field strength becomes minimum in each magnetic field line, meaning the magnetic latitude of the source location can vary for each L‐shell. We conducted a full‐wave simulation of EMIC waves in the outer dayside magnetosphere using the Petra‐M code, incorporating a non‐dipole compressed magnetic field. Our results indicated that the direction of wave energy flow from the source varies; thus, based on a satellite's location, it can detect wave energy flowing either parallel or antiparallel to the magnetic field, which is consistent with satellite observations. We also show that EMIC waves generated in the northern hemisphere can reach both the north and the south Polar Regions. However, the wave power reaching the northern hemisphere is significantly stronger than that which reaches the southern hemisphere.


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4.6 (2023)

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38%

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9.0 (2023)

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32 days

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1.2 (2023)

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0.13397 (2023)

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