Paul R. Holland’s research while affiliated with British Antarctic Survey and other places

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Publications (189)


Iceberg grounding enhances the release of freshwater on the Antarctic continental shelf
  • Preprint

May 2025

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8 Reads

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Figure 2. Region names and numbers used in data products for each ice sheet. The Greenland regions from Mouginot and Rignot (2019) and Antarctic regions from The IMBIE team (2018).
Figure 3. Time series of Greenland a) ice discharge, and b) ice discharge anomaly (w.r.t. 1850-1900) (right) from flux-gates ∼5 km upstream
Figure 4. Maps showing the annual average weighting function for iceberg melt rates as a function of their source region. Similar maps with monthly resolution are also available.
Figure 5. Maps showing the annual average weighting function for iceberg melt rates as a function of their source region. Similar maps with monthly resolution are also available.
Datasets and protocols for including anomalous freshwater from melting ice sheets in climate simulations
  • Preprint
  • File available

May 2025

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112 Reads

Anomalous freshwater fluxes from the Greenland and Antarctic ice sheets and ice shelves are impacting the surrounding oceans and we need to be able to account for these effects in climate model simulations over the historical period and beyond. In previous phases of the Coupled Model Intercomparison Project (CMIP), models mostly either assumed that the ice sheets were in mass balance, or that discharge from the ice sheets was constant, but in neither case was the observed increasing discharge properly accounted for. In this paper, we present an updateable dataset of absolute and anomalous freshwater mass fluxes from both ice sheets. These fluxes can be implemented in historical climate simulations as a forcing for models that do not (yet) include interactive ice sheets, or used to evaluate models that do. We also make recommendations for how climatological and anomalous fluxes can be implemented in climate models that may have different approaches to interactions with the ice sheets. These forcings are available for CMIP7 simulations and should lead to more robust and coherent simulation of sea surface temperature, sea ice and regional sea level trends in the recent historical period, and improve the credibility of projections.

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Map of the Amundsen Sea Sector showing ice shelf basal melting and the active subglacial lakes network
a Map showing the location of ice drainage basins, ice shelves, Thwaites’s subglacial hydrology, polynya, and hydrographic moorings in front of Pine Island ice shelf. Basemap is a MODIS image acquired on the 5th of January 2014 during the polynya formation. The ice shelf colours display the amplitude of basal melt change during 2013–2014 coincident with the basal melt pulse at Thwaites, the ice shelf extent corresponds to the minimum for the 2011–2021 period accounting for calving front and grounding line variation³⁶. Inset shows sector location within the Antarctic Ice Sheet (b) Mean basal melt rate under Thwaites Eastern Ice Shelf (TEIS) and near the grounding line of Thwaites Western Ice Tongue (TWITgl) between 2010 and 2020, the area of thinning and retreat at the grounding line is labelled “2013 ungrounding”; c Sensitivity of the grounded ice to changes in the Thwaites floating ice (see Methods)⁶⁴. Source data are provided as a Source Data file.
Relative timing between lake discharge, ice shelf thinning and basal melt increase, and grounded ice thinning
a timeline of events and location of main features, subglacial network at the proximity of the grounding line is shown in grey; b time-series of elevation change anomaly from the 2011–2020 mean rate of elevation change for the Thwaites Eastern Ice Shelf (TEIS) and near the grounding line of Thwaites Western Ice Tongue (TWITgl), the elevation change is shown in Fig. S6; c mean elevation change over the area of the 2013 ungrounding (dashed line) and regression analysis over the period of increased thinning (solid lines) the breakpoint is determined to be April 2013 (see Methods); d Total volume change of the seven active subglacial lakes (curves) and equivalent rates of subglacial discharge (green shading); e Change in thermocline depth from two hydrographic moorings in front of the Pine Island glacier (Fig. 1a), and basal melt rate variability under Pine Island and Thwaites (average for TEIS and TWITgl) ice shelves during the Thwaites’ lake drainage and grounding line thinning and retreat. The vertical lilac shading across all five plots marks the onset of lake drainage taking place sometimes between January and April 201336,39. Source data are provided as a Source Data file.
Correlation between subglacial flux, ice shelf basal melting, and ocean conditions
a Correlation between timeseries of Thermocline depth (Therm. D.), Subglacial flux (SGL flux), Thwaites basal melt anomaly (T. m.a.), and Pine Island Glacier basal melt anomaly (PIG m.a.) as shown in Fig. 2 of the main manuscript. Numbers in insets give the values of the Pearson correlation coefficients. P values suggest that the Thwaites basal melt anomaly and the Subglacial flux timeseries (Pearson correlation coefficient of 0.60) have a significant correlation (P value of 7e⁻⁹). Basal melt anomalies under PIG and Thwaites are weakly correlated over the entire period and with a P value of 6e⁻³. b A lag analysis suggests increased correlation between the subglacial flux and Thwaites’ basal melt rates shifted backward in time by three months, the Pearson correlation increases from 0.60 to 0.77 with a P value of 5e⁻¹⁶ (top right plot). Accounting for a three-month lag (Fig. S10), the relationship between Thwaites‘ basal melt and the subglacial flux is well approximated by a power law (dashed line) of exponent 0.52 (95% confidence interval [0.29 0.75]). Source data are provided as a Source Data file.
Modelled additional ice shelf melt from subglacial discharge
Predicted additional basal melt rate due to subglacial discharge (modelled: red; power law approximation (m°=3.78F0.54)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(\dot{m}=3.78{F}^{0.54})$$\end{document}: blue; subglacial flux multiple F\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$F$$\end{document} is the subglacial flux used divided by 80 m³ s⁻¹, the background subglacial discharge rate for the main drainage network, subglacial flux multiple of 8 corresponds to the order of magnitude of the combined peak discharge of all seven Thwaites lakes in 2013. Source data are provided as a Source Data file.
Schematic of proposed succession of events during the 2013–2014 period under Thwaites Glacier
Schematic diagram of impact of subglacial lake discharge on ocean melting and ice shelf, sea-ice, and grounding line change.
The influence of subglacial lake discharge on Thwaites Glacier ice-shelf melting and grounding-line retreat

March 2025

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80 Reads

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2 Citations

The retreat of the Antarctic Ice Sheet is conventionally attributed to increased ocean melting of ice shelves, potentially enhanced by internal instability from grounding lines near retrograde bed slopes. Ocean melting is enhanced by increased intrusion of modified Circumpolar Deep Water (mCDW) into ice shelf cavities. Upwelling from the release of subglacial meltwater can enhance mCDW’s melting ability, though its efficacy is not well understood and is not represented in current ice sheet loss projections. Here we quantify this process during an exceptional subglacial lake drainage event under Thwaites Glacier. We found that the buoyant plume from the subglacial discharge temporarily doubled the rate of ocean melting under Thwaites, thinning the ice shelf. These events likely contributed to Thwaites’ rapid thinning and grounding line retreat during that period. However, simulations and observations indicate that a steady subglacial water release would more efficiently enhance basal melt rates at Thwaites, with melt rate increasing like the square root of the subglacial discharge. Thus, it remains unclear whether increased subglacial flooding events provide a stabilizing influence on West Antarctic ice loss by reducing the impact of subglacial water on ocean melting, or a destabilizing influence by triggering rapid changes at the grounding zone.


Observationally constrained estimates of the annual Arctic sea-ice volume budget 2010–2022

February 2025

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51 Reads

Annals of Glaciology

Sea-ice floating in the Arctic ocean is a constantly moving, growing and melting layer. The seasonal cycle of sea-ice volume has an average amplitude of 10000km310\,000\,\mathrm{km}^3 or 9 trillion tonnes of sea ice. The role of dynamic redistribution of sea ice is observable during winter growth by the incorporation of satellite remote sensing of ice thickness, concentration and drift. Recent advances in the processing of CryoSat-2 radar altimetry data have allowed for the retrieval of summer sea-ice thickness. This allows for a full year of a purely remote sensing-derived ice volume budget analysis. Here, we present the closed volume budget of Arctic sea ice over the period October 2010–May 2022 revealing the key contributions to summer melt and minimum sea-ice volume and extent. We show the importance of ice drift to the inter-annual variability in Arctic sea-ice volume and the regional distribution of sea ice. The estimates of specific areas of sea-ice growth and melt provide key information on sea-ice over-production, the excess volume of ice growth compared to melt. The statistical accuracy of each key region of the Arctic is presented, revealing the current accuracy of knowledge of Arctic sea-ice volume from observational sources.


Spatio-temporal melt and basal channel evolution on Pine Island Glacier ice shelf from CryoSat-2

February 2025

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50 Reads

Ice shelves buttress the grounded ice sheet, restraining its flow into the ocean. Mass loss from these ice shelves occurs primarily through ocean-induced basal melting, with the highest melt rates occurring in regions that host basal channels – elongated, kilometre-wide zones of relatively thin ice. While some models suggest that basal channels could mitigate overall ice shelf melt rates, channels have also been linked to basal and surface crevassing, leaving their cumulative impact on ice-shelf stability uncertain. Due to their relatively small spatial scale and the limitations of previous satellite datasets, our understanding of how channelised melting evolves over time remains limited. In this study, we present a novel approach that uses CryoSat-2 radar altimetry data to calculate ice shelf basal melt rates, demonstrated here as a case study over Pine Island Glacier (PIG) ice shelf. Our method generates monthly Digital Elevation Models (DEMs) and melt maps with a 250 m spatial resolution. The data show that near the grounding line, basal melting preferentially melts a channel's western flank 50 % more than its eastern flank. Additionally, we find that the main channelised geometries on PIG are inherited upstream of the grounding line and play a role in forming ice shelf pinning points. These observations highlight the importance of channels under ice shelves, emphasising the need to investigate them further and consider their impacts on observations and models that do not resolve them.


(a–c) Linear trends in annual mean SIA in satellite observations (red) and CMIP6 models (blue histogram) and Gaussian fit to CMIP6 distribution (black) for the periods (a) 1979–2005, (b) 1979–2013 and (c) 1979–2023. The dashed vertical line indicates zero trend, and the blue line indicates the multi-model mean. (d) The probability of observing a trend at least as large as observed (a one-tailed test) under the null hypothesis that observations are taken from the same population as the CMIP6 multi-model ensemble, for varying end dates and either a fixed start date of 1979 as in panels (a) and (b) (crosses) or fixed trend length of 35 years (dots); pval stands for p value.
Contributions to the p value shown in Fig. 1d. (a) Observed trend, with NSIDC Sea Ice Index v3.0 in black as in the main text and other datasets as indicated. (b) Mean of modelled trends, (c) standard deviation of modelled trends and (d) p value (pval; as main text Fig. 1d but with alternative observational estimates (Dörr et al., 2021)).
The role of ice-free conditions in explaining model spread (a and b) and result sensitivity to ensemble treatment (c and d). (a) Scatterplot of summer (February) sea ice climatology for 1979–2023 against the annual mean trend over 1979–2023. (b) As (a) but for annual mean climatology against the trend, with a cutoff threshold (a quarter of the observed climatology) to exclude MIROC models indicated by a dashed grey line. Panels (a) and (b) show a maximum of six ensemble members per model. (c) As Fig. 1d but excluding MIROC models. (d) As Fig. 1d but the mean of p values (pval) from 10 000 resamples each using one random ensemble member from each model.
Brief communication: New perspectives on the skill of modelled sea ice trends in light of recent Antarctic sea ice loss

December 2024

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14 Reads

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2 Citations

Most climate models do not reproduce the 1979–2014 increase in Antarctic sea ice cover. This was a contributing factor in successive Intergovernmental Panel on Climate Change reports allocating low confidence to model projections of sea ice over the 21st century. We show that recent rapid declines bring observed sea ice area trends back into line with the models and confirm that discrepancies exist for earlier periods. This demonstrates that models exhibit different skill for different timescales and periods. We discuss possible interpretations of this linear trend assessment given the abrupt nature of recent changes and discuss the implications for future research.


Emerging signals of climate change from the equator to the poles: new insights into a warming world

October 2024

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398 Reads

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13 Citations

The reality of human-induced climate change is unequivocal and exerts an ever-increasing global impact. Access to the latest scientific information on current climate change and projection of future trends is important for planning adaptation measures and for informing international efforts to reduce emissions of greenhouse gases (GHGs). Identification of hazards and risks may be used to assess vulnerability, determine limits to adaptation, and enhance resilience to climate change. This article highlights how recent research programs are continuing to elucidate current processes and advance projections across major climate systems and identifies remaining knowledge gaps. Key findings include projected future increases in monsoon rainfall, resulting from a changing balance between the rainfall-reducing effect of aerosols and rainfall-increasing GHGs; a strengthening of the storm track in the North Atlantic; an increase in the fraction of precipitation that falls as rain at both poles; an increase in the frequency and severity of El Niño Southern Oscillation (ENSO) events, along with changes in ENSO teleconnections to North America and Europe; and an increase in the frequency of hazardous hot-humid extremes. These changes have the potential to increase risks to both human and natural systems. Nevertheless, these risks may be reduced via urgent, science-led adaptation and resilience measures and by reductions in GHGs.


Chlorophyll Production in the Amundsen Sea Boosts Heat Flux to Atmosphere and Weakens Heat Flux to Ice Shelves

September 2024

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46 Reads

The Amundsen Sea in West Antarctica features rapidly thinning ice shelves, large polynyas, and sizable spring phytoplankton blooms. Although considerable effort has gone into characterizing heat fluxes between the Amundsen Sea, its associated ice shelves, and the overlying atmosphere, the effect of the phytoplankton blooms on the distribution of heat remains poorly understood. In this modeling study, we implement a feedback from biogeochemistry onto physics into MITgcm‐BLING and use it to show that high levels of chlorophyll—concentrated in the Amundsen Sea Polynya and the Pine Island Polynya—have the potential to increase springtime surface warming in polynyas by steepening the attenuation profile of solar radiation with depth. The chlorophyll‐associated warm anomaly (on average between +0.2° {}^{\circ}C and +0.3° {}^{\circ}C) at the surface is quickly dissipated to the atmosphere, by increases in longwave, latent and sensible heat loss from open water areas. Outside of the coastal polynyas, the summertime warm anomaly leads to an average sea ice thinning of 1.7 cm across the region, and stimulates up to 20% additional seasonal melting near the fronts of ice shelves. The accompanying cold anomaly, caused by shading of deeper waters, persists year‐round and affects a decrease in the volume of Circumpolar Deep Water on the continental shelf. This cooling ultimately leads to an average sea ice thickening of 3.5 cm and, together with associated changes to circulation, reduces basal melting of Amundsen Sea ice shelves by approximately 7% relative to the model scenario with no phytoplankton bloom.


(a–b.) Time‐series of the IPO (red; in °C) and internal ASL (green; in hPa) from the natural prior‐based reconstruction using all the proxy records (i.e., all‐iCESM‐recon). (c.) Temporal evolution of the forced ASL computed as the ensemble mean of CESM1‐LE (orange; in hPa) scaled to match the observed trend over 1950–2023. (d.) Time‐series of the total ASL variability (internal plus forced; black; in hPa). All the time‐series are expressed as anomalies relative to the 1901–1930 period. Thick colored lines are moving 13‐year averages using lowess smoothing. Periods characterized by declining IPO phases are colored in red while rising IPO phases are in blue. For each period, the difference between the end and the beginning of the anomaly is displayed (based on the 13‐year averaged time‐series).
Sea‐level pressure (contours; hPa per decade) and sea surface temperature (colors; °C per decade) linear trends in all‐iCESM‐recon along with the IPO‐congruent trends and the residual trend over the 1935–1969 and 1970–2000 periods.
Time‐series of simulated ASL response to all forcing (black), greenhouse gas forcing denied (red) and stratospheric ozone depletion denied (blue) ensembles from CESM1‐LE (in hPa per decade). The linear trends of the ASL over the 1970–2000 period from the three ensembles are displayed. While the greenhouse gas forcing denied ensemble includes 20 members, the stratospheric ozone depletion denied ensemble only contains eight members. In order to take into account the different ensemble size for the trend significance, we used a bootstrapping method to calculate the p‐value of the trend for the greenhouse gas denied ensemble (10,000 iterations by randomly selecting 8 members among the 20 available members).
Composites of 30‐year trends of SST (colors) and sea‐level pressure (contours) during periods displaying 30‐year negative statistically significant (p‐value <0.05) ASL trends for the SMILEs. The forced variability (estimated as the ensemble mean) is subtracted from each member before building the composites. To increase the sample size, we include 30‐year positive statistically significant trends in the composite (and inverting their sign before combining it with the other samples). Both the relative frequency of observed declining IPO phase (in %) and the corresponding sample size are displayed on the map.
Multi‐Decadal Variability of Amundsen Sea Low Controlled by Natural Tropical and Anthropogenic Drivers

August 2024

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143 Reads

Plain Language Summary Changes in the West Antarctic Ice Sheet mass balance (i.e., the difference between the gain and loss of ice mass) are partly influenced by large‐scale winds, and in particular, a climatological low‐pressure feature located off the West Antarctic coast called the Amundsen Sea Low (ASL). Yet, although the long‐term strengthening of the ASL since the mid‐20th century has been demonstrated to be related to anthropogenic forcing, our understanding of the variability of the ASL on time‐scales of decades is poorly known. In this paper, we therefore investigate the origins of this variability since 1870, and quantify the relative contributions of human‐caused climate changes and natural variability of the climate system. For this purpose, we use several ensembles of model simulations as well as new climate reconstructions that combine paleoclimate records with model simulations using a statistical method. Our results indicate that the multi‐decadal variability of the ASL is strongly driven by tropical variability in the Indo‐Pacific through atmospheric connections between this region and the Amundsen Sea. Our reconstruction, when compared with a large ensemble of model simulations, indicates that since 1950, human‐induced climate forcing has become a dominant driver of long‐term ASL variability, contributing equally to tropical variability.



Citations (70)


... E. Alley et al., 2022a;R. B. Alley et al., 2022b;Schmidt et al., 2023;Watkins et al., 2021), which is further complicated by the complex morphology of the ice shelf base, including basal channels, fractures, and overall roughness, as well as timevarying forcing from the ice sheet (Gourmelen et al., 2025). Beyond thermodynamic effects, mechanical forces may also play a key role in ice shelf weakening. ...

Reference:

Recent Variability in Fracture Characteristics and Ice Flow of Thwaites Ice Shelf, West Antarctica
The influence of subglacial lake discharge on Thwaites Glacier ice-shelf melting and grounding-line retreat

... Furthermore, the CMIP6 Southern Ocean SST bias has been reduced by the recent cessation of observed cooling since 2015 (black curve, Figure S6 in Supporting Information S1). These recent observed changes highlight that models exhibit different skill for different timescales and periods, a particularly important consideration for the Southern Ocean (Holmes et al., 2024). ...

Brief communication: New perspectives on the skill of modelled sea ice trends in light of recent Antarctic sea ice loss

... However, for SSP370 and SSP585, SFe deposition increases up to 100% higher than present-day levels in equatorial and tropical regions, with smaller increases in high latitudes. This rise is associated with increases in water content and warmer temperatures 56,57 , which, together with high atmospheric acidity, enhance solubilization and result in greater SFe deposition 46 . ...

Emerging signals of climate change from the equator to the poles: new insights into a warming world

... This may have accounted for the anticyclonic conditions observed in the Amundsen Sea during that period. This is in agreement with the study of O'Connor et al. (2023), which indicates that these anticyclonic conditions result from a combined effect of strong El Niño conditions and other drivers unrelated to tropical Pacific variability. Afterward, the negative IPO phase from around 1940 to the mid-1970s contributed to deepening the ASL. ...

Characteristics and rarity of the strong 1940s westerly wind event over the Amundsen Sea, West Antarctica

... Solid Earth-ice sheet-ocean-climate interactions on many time scales 40 are a major challenge for ice sheet simulations. Climate, ocean and sea-level forcings in uncoupled ice sheet models are themselves dependent on the simulated ice sheet response, yet the high computational cost of coupled models currently limits experiments to short time periods or coarse spatial resolution [65][66][67][68] . Glacial-cycle simulations with adequate representation of grounding line and ice stream dynamics still require uncoupled ice sheet models. ...

The Antarctic contribution to 21st-century sea-level rise predicted by the UK Earth System Model with an interactive ice sheet

... The speed variability is indeed superimposed on a longer-term speed-up. This may be driven by a centennial trend of ocean warming on the continental shelf (Naughten et al., 2022b), likely driven by a trend in winds over the continental shelf break (Holland et al., , 2022, or it could be driven by internal ice dynamic feedbacks (such as MISI) (Reed et al., 2024) or ice-ocean feedbacks, such as changes in cavity circulation due to ice shelf thinning and grounding line retreat (Bradley et al., 2022). ...

Anthropogenic and internal drivers of wind changes over the Amundsen Sea, West Antarctica, during the 20th and 21st centuries

... Furthermore, submarine melting in newly formed ocean cavities, at rates similar to those in the 2000s, leads to a self-reinforcing feedback, which further accelerates grounding line retreat, even without ice-shelf collapse or MICI 122 . Even when melting is reduced to zero, some catchments continue to lose mass, implying that a tipping point may already have been passed 125 . Given recent projections of rapid ocean warming of the ASE this century at triple the historical rate 51 , it seems clear that the initiation of at least partial collapse of https://doi.org/10.1038/s43247-025-02299-w ...

Coupled ice–ocean interactions during future retreat of West Antarctic ice streams in the Amundsen Sea sector

... Although these studies have shown that the variations in wind fields have influence on the baroclinic process on the Amundsen Sea slope (Dotto et al., 2020;Silvano et al., 2022), their conclusions rely on regional models and sporadic observations, and a comprehensive explanation for the undercurrent's origin and wind-driven/modulated dynamics remains elusive. In recent years, it has been discovered that ice shelf and sea ice melt also has impact on undercurrents; Haigh and Holland (2024) suggested that sea ice freshwater flux significantly correlates with undercurrent in decadal time periods; using an idealized numerical model, Si et al. (2024) proposed a mechanism of interaction between ice shelf melting and eastward undercurrents. ...

Decadal Variability of Ice‐Shelf Melting in the Amundsen Sea Driven by Sea‐Ice Freshwater Fluxes

... Increased basal melt responsible for ongoing changes in mass balance and projected future changes have been connected to increases in transport of warm, saline, modified circumpolar deep water across the continental shelf break. However, oceanic processes local to ice-shelf cavities can also affect heat transport and the efficiency of heat transfer at the ice-ocean interface (i.e., Cheng et al., 2024). ...

Ice shelf basal channel shape determines channelized ice-ocean interactions

... The processes identified here, however, could be representative of the Weddell Polynya, where open ocean deep convection sometimes occurs, if it is opened(De Lavergne et al., 2014;Rheinlaender et al., 2021;Mchedlishvili et al., 2022). Anthropogenic-driven shifts in the Amundsen Low might play a role in causing abrupt changes on the Antarctic shelves, basal melt of the West Antarctic Ice Sheet and possibly the Antarctic Slope Current(Thompson et al., 2018), open ocean sea-ice and deep mixing(Holland et al., 320 2019;Drijfhout et al., 2024b). ...

An Amundsen Sea source of decadal temperature changes on the Antarctic continental shelf

Ocean Dynamics