Rune Graversen’s research while affiliated with UiT The Arctic University of Norway and other places

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Publications (30)


Normalized pulse functions representing global‐mean surface temperature response to SO2 ${\text{SO}}_{2}$. The black line is the pulse function from OB16, gray lines show the eight pulse functions from the CESM2 simulations listed in Table 1, while the red line highlights one gray line in each of the subfigures. Numbers in parenthesis give the normalization constant.
Same as in Figure 1, but for pulse functions representing ERF response to SO2 ${\text{SO}}_{2}$.
Annual means of the fraction of the sea surface covered by sea ice for the CESM2 simulations. Solid lines are single‐eruption experiments, and short dashed lines are double‐eruption experiments using 2‐year separation between eruptions, while long dashed lines are double eruptions with 4‐year eruption separation. Gray shading represents one and two standard deviations from the mean of a control run.
Reconstruction of AOD (top), ERF (middle), and global‐mean surface temperature (bottom) time series for the CESM2 simulations S400‐2SEP (left column) and S400‐4SEP (right column). Black, solid lines are original simulation output, orange is reconstructed using φS400 ${\varphi }^{\mathrm{S}400}$, and purple (brown) is reconstructed using φS400‐2SEP ${\varphi }^{\mathrm{S}400\mbox{-}2\text{SEP}}$ φS400‐4SEP $\left({\varphi }^{\mathrm{S}400\mbox{-}4\text{SEP}}\right)$.
As Figure 4, but for the CESM2 simulations S26‐2SEP (left columns) and S26‐4SEP (right column).

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Nonparametric Estimation of Temperature Response to Volcanic Forcing
  • Article
  • Publisher preview available

May 2025

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5 Reads

Eirik Rolland Enger

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Rune Graversen

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Audun Theodorsen

Large volcanic eruptions strongly influence the internal variability of the climate system. Reliable estimates of the volcanic eruption response as simulated by climate models are needed to reconstruct past climate variability. Yet, the ability of models to represent the response to both single‐eruption events and a combination of eruptions remains uncertain. We use the Community Earth System Model version 2 along with the Whole Atmosphere Community Climate Model version 6, known as CESM2(WACCM6), to study the global‐mean surface temperature (GMST) response to idealized single volcano eruptions at the equator, ranging in size from Mt. Pinatubo‐type events to supereruptions. Additionally, we simulate the GMST response to double‐eruption events with eruption separations of a few years. For large idealized eruptions, we demonstrate that double‐eruption events separated by 4 years combine linearly in terms of GMST response. In addition, the temporal development is similar across all single volcanic eruptions injecting at least 400 Tg SO2 (SO2)\left({\mathrm{S}\mathrm{O}}_{2}\right) into the atmosphere. Because only a few eruptions in the past millennium occurred within 4 years of a previous eruption, we assume that the historical record can be represented as a superposition of single‐eruption events. Hence, we employ a deconvolution method to estimate a nonparametric historical GMST response pulse function for volcanic eruptions, based on climate simulation data from 850 to 1850 taken from a previous study. By applying the estimated GMST response pulse function, we can reconstruct most of the underlying historical GMST signal. Furthermore, the GMST response is significantly perturbed for at least 7 years following eruptions.

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Timeline of the simulations run with CESM2 (WACCM6). Black, filled dots mark a volcanic eruption event, while gray stippled lines mark their timing annotated by the simulation year and the month, Y‐MM. Ensemble names are listed on the left‐hand side, with simulations within an ensemble having the same color. All eruptions occurred on the 15th day of a month. All simulations start in preindustrial 1850 conditions and were run in both CoupledAO and FixedSST_SI settings at least until the start of simulation year 21.
SAOD (a), ERF (b), and global mean surface temperature (c) response time series to the four tropical volcanic eruption cases, S26, S400, S1629, and S3000 (specified only in legend (a)). S3000 contains two ensemble members, while the others have four. Each time series is normalized to the peak value C $C$, with values of C $C$ given in the legend. Black lines indicate the mean across the ensembles after aligning eruption times as shown in Figure 1, while shading marks one standard deviation from the mean.
ERF as a function of SAOD. Symbols, as indicated in the legend, are indicating annual means over the whole time series of simulations shown in Figure 1. For comparison, annual means of the data from the HadCM3 simulation by Gregory et al. (2016, G16 as gray crosses), and the estimated peak values of the Mt. Pinatubo (black star) and Mt. Tambora (black plus) eruptions are also shown. Red circles labeled C2W Peaks* indicate peak values from the CESM2 (WACCM6) simulations, computed from 12‐month running means over the ensemble means. An asterisk (∗) $(\ast )$ indicates peak values (as opposed to annual means). The gray line is the same regression fit to G16 as in Gregory et al. (2016, their Figure 4). (a) and (b) have different SAOD intervals on the x $x$‐axis, where (b) is zooming in on the smallest SAOD values.
(a): Seasonal means of the ratio of ERF to SAOD as a function of time after eruption. Straight lines indicate linear regression fits and are described in Table 2, while shaded regions are the standard deviation of the ensembles for each season. Regression fits and shadings are made for the prepeak (left) and postpeak (right) periods. (b) Same as in (a), but for the underlying SAOD and ERF time series having been scaled to have peak values at unity. Shown are data from Table 1, along with tropical eruptions from M20. Values from each ensemble member are omitted for clarity, but we note that S26 includes some outliers at positive ratios after the start of the second posteruption year.
Peak values of (a) SAOD, (b) ERF, and (c) global mean surface temperature (GMST) as a function of injected SO2 ${\text{SO}}_{2}$. (d) ERF and (e) GMST as a function of SAOD. (f) GMST as a function of ERF. ERF and GMST values are absolute values. Blue diamonds labeled STrop represent tropical cases (S26, S400, S1629, and S3000), while the brown three‐branched twig signifies the high‐latitude S1629N case. T10 (a–f), M14 (a–f), B20 (a–f), OB16 (b, c, and f), E13 (a), M20 (a–f), J05 (a–f), McG24 (b, c, and f), Os20 (a, c, and e), and R09 (c) are data from previous studies; P and T indicate Mt. Pinatubo and Mt. Tambora estimates, respectively, based on observations, and the stippled gray line represents a two‐thirds power‐law relationship between SAOD and SO2 ${\text{SO}}_{2}$ as suggested by Crowley and Unterman (2013). aRF rather than ERF was estimated from atmosphere‐ocean coupled model simulations. Label background colors indicate data from similar models (Table C1).
Saturation in Forcing Efficiency and Temperature Response of Large Volcanic Eruptions

Volcanic eruptions cause climate cooling due to the reflection of solar radiation by emitted and subsequently produced aerosols. The climate effect of an eruption may last for about a decade and is nonlinearly tied to the amount of injected SO2 SO2{\text{SO}}_{2} from the eruption. We investigate the climatic effects of volcanic eruptions, ranging from Mt. Pinatubo‐sized events to supereruptions. The study is based on ensemble simulations in the Community Earth System Model Version 2 (CESM2) climate model applying the Whole Atmosphere Community Climate Model Version 6 (WACCM6) atmosphere model, using a coupled ocean and fixed sea surface temperature setting. Our analysis focuses on the impact of different levels of SO2 SO2{\text{SO}}_{2} injections on stratospheric aerosol optical depth (SAOD), effective radiative forcing (ERF), and global mean surface temperature (GMST) anomalies. We uncover a notable time‐dependent decrease in aerosol forcing efficiency (ERF normalized by SAOD) for all eruption SO2 SO2{\text{SO}}_{2} levels during the first posteruption year. In addition, it is revealed that the largest eruptions investigated in this study, including several previous supereruption simulations, provide peak ERF anomalies bounded at −65Wm−2 65Wm2{-}65\,\mathrm{W}\,{\mathrm{m}}^{-2}. Further, a close linear relationship between peak GMST and ERF effectively bounds the GMST anomaly to, at most, approximately −10K 10K{-}10\,\mathrm{K}. This is consistent across several previous studies using different climate models.



Figure 1. AOD (a), RF (b) and temperature response (c) time series to the four tropical volcanic eruption cases, C2W↓, C2W−, C2W↑, and C2W↑↑. The time series have been normalised to have peak values at unity, where C is the normalisation constant. Black lines indicate the median across the ensembles, while shading marks the 5th and 95th percentiles.
Figure 2. RF as a function of AOD, yearly means. Data from the five simulations listed in table 1 (C2W↓, C2W−, C2W↑, C2WN↑, and C2W↑↑) are shown along with the data from the HadCM3 sstPiHistVol simulation by Gregory et al. (2016) (grey crosses, G16). Also shown are the estimated peak values of the Mt. Pinatubo (black star) and Mt. Tambora (black plus) eruptions. The peak values from the C2W simulations are shown as red circles. Additionally in (a) the simulated super-volcano of Jones et al. (2005) (pink square) is shown. All peak values (as opposed to annual means) have an asterisk ( * ) in their label. The grey lines are the same regression fits as in Gregory et al. (2016, Fig. 4), where the solid line is the fit to G16. (b): Zooming in on the smallest AOD values.
Figure 3. (a): The ratio of RF to AOD, with time-after-eruption on the horizontal axis. Straight lines indicate linear regression fits and are described in table 2, while shaded regions are the standard deviation across the ensembles for each season. Regression fits and shadings are made for the pre-peak and post-peak periods. (b): Same as in (a), but where the underlying AOD and RF time series have been scaled to have peak values at unity. Shown are data from table 1 along with tropical eruptions from M20.
Figure 4. (a) AOD, (b) RF, and (c) temperature anomaly as a function of injected SO2. (d) RF and (e) temperature anomaly as a function of AOD. (f) Temperature anomaly as a function of RF. Blue diamonds labelled C2WTrop represent tropical cases (C2W↓, C2W−, C2W↑, C2W↑↑), the brown three-branched twig signifies the C2WN↑ case, and green downward triangles denote OB16 data from Otto-Bliesner et al. (2016). The red thin diamonds labelled M20 display the Marshall and Smith (2020) data. Black star and plus indicate Mt. Pinatubo and Mt. Tambora estimates based on observations. The pink square labelled J05 refers to the one-hundred times Mt. Pinatubo super-volcano from Jones et al. (2005), and the pink disk labelled T10 represents the YTT super-volcano from Timmreck et al. (2010). The pink dashed line labelled N15 is from Niemeier and Timmreck (2015), indicating the function in Eq. 1.
Radiative forcing by super-volcano eruptions

March 2024

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61 Reads

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1 Citation

We investigate the climatic effects of volcanic eruptions spanning from Mt.\ Pinatubo-sized events to super-volcanoes. The study is based on ensemble simulations in the Community Earth System Model Version 2 (CESM2) climate model using the Whole Atmosphere Community Climate Model Version 6 (WACCM6) atmosphere model. Our analysis focuses on the impact of different \ce{SO2}-amount injections on stratospheric aerosol optical depth (AOD), effective radiative forcing (RF), and global temperature anomalies. Unlike the traditional linear models used for smaller eruptions, our results reveal a non-linear relationship between RF and AOD for larger eruptions. We also uncover a notable time-dependent decrease in aerosol forcing efficiency across all eruption magnitudes during the first post-eruption year. In addition, the study reveals that larger as compared to medium-sized eruption events produce a delayed and sharper peak in AOD, and a longer-lasting temperature response while the time evolution of RF remains similar between the two eruption types. When including the results of previous studies, we find that relating \ce{SO2} to any other parameter is inconsistent across models compared to the relationships between AOD, RF, and temperature anomaly. Thus, we expect the largest uncertainty in model codes to relate to the chemistry and physics of \ce{SO2} evolution. Finally, we find that the peak RF approaches a limiting value, and that the peak temperature response follows linearly, effectively bounding the temperature anomaly to at most \sim\SI{-12}{\kelvin}.


On the impact of net-zero forcing Q-flux change

February 2024

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43 Reads

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1 Citation

Climate Dynamics

Numerical climate model simulations suggest that global warming is enhanced or hampered by the spatial pattern of the warming itself. This phenomenon is known as the “pattern effect” and has in recent years become the most promising explanation for the change over time of climate sensitivity in climate models. Under historical global warming, different patterns of surface-temperature change have emerged, notably a yet unexplained cooling in the Southern Ocean and the East Pacific. Historical climate model simulations notoriously fail to reproduce this cooling, which may contribute to the deviation of the simulated global-mean warming from the observed record. Here we qualitatively investigate the potential impact of historical and other surface-temperature pattern changes by changing the ocean heat transport convergence (Q-flux) in a slab-ocean model. The Q-flux changes are always implemented such that in the global mean they impose no net forcing. Consistent with earlier studies we find that the impact of a negative Q-flux change in the Southern Ocean has a stronger effect than in other regions because of a feedback loop between sea-surface temperatures (SSTs) and clouds in the Southern Ocean and the stably stratified regions in the tropics. The SST-cloud feedback loop facilitates the expansion of the Antarctic sea ice, indeed taking the model into a Snowball-Earth state. The intensity of this effect is found to be model dependent, especially due to differences in the cloud parametrisation. In experiments with deactivated sea ice the impact of the negative Q-flux change is much weaker.


Bringing it all together: Science and modelling priorities to support international climate policy

February 2024

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428 Reads

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3 Citations

Colin Gareth Jones

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Ben B B Booth

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[...]

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Sönke Zaehle

We review how the international modelling community, encompassing Integrated Assessment models, global and regional Earth system and climate models, and impact models, have worked together over the past few decades, to advance understanding of Earth system change and its impacts on society and the environment, and support international climate policy. We then recommend a number of priority research areas for the coming ~6 years (i.e. until ~2030), a timescale that matches a number of newly starting international modelling activities and encompasses the IPCC 7th Assessment Report (AR7) and the 2nd UNFCCC Global Stocktake. Progress in these areas will significantly advance our understanding of Earth system change and its impacts and increase the quality and utility of science support to climate policy. We emphasize the need for continued improvement in our understanding of, and ability to simulate, the coupled Earth system and the impacts of Earth system change. There is an urgent need to investigate plausible pathways and emission scenarios that realize the Paris Climate Targets, including pathways that overshoot the 1.5 °C and 2 °C targets, before later returning to them. Earth System models (ESMs) need to be capable of thoroughly assessing such warming overshoots, in particular, the efficacy of negative CO2 emission actions in reducing atmospheric CO2 and driving global cooling. An improved assessment of the long-term consequences of stabilizing climate at 1.5 °C or 2 °C above pre-industrial temperatures is also required. We recommend ESMs run overshoot scenarios in CO2-emission mode, to more fully represent coupled climate - carbon cycle feedbacks. Regional downscaling and impact models should also use forcing data from these simulations, so impact and regional climate projections are as realistic as possible. An accurate simulation of the observed record remains a key requirement of models, as does accurate simulation of key metrics, such as the Effective Climate Sensitivity. For adaptation, improved guidance on potential changes in climate extremes and the modes of variability these extremes develop in, is a key demand. Such improvements will most likely be realized through a combination of increased model resolution and improvement of key parameterizations. We propose a deeper collaboration across modelling efforts targeting increased process realism and coupling, enhanced model resolution, parameterization improvement, and data-driven Machine Learning methods. With respect to sampling future uncertainty, increased collaboration between approaches that emphasize large model ensembles and those focussed on statistical emulation is required. We recommend increased attention is paid to High Impact Low Likelihood (HILL) outcomes. In particular, the risk and consequences of exceeding critical tipping points during a warming overshoot. For a comprehensive assessment of the impacts of Earth system change, including impacts arising directly from specific mitigation actions, it is important detailed, disaggregated information from the Integrated Assessment Models (IAMs) used to generate future scenarios is available to impact models. Conversely, methods need to be developed to incorporate potential future societal responses to the impacts of Earth system change into scenario development. Finally, the new models, simulations, data, and scientific advances, proposed in this article will not be possible without long-term development and maintenance of a robust, globally connected infrastructure ecosystem. This system must be easily accessible and useable across all modelling communities and across the world, allowing the global research community to be fully engaged in developing and delivering new scientific knowledge to support international climate policy.


Validation of a SAR-Only Wind-Vector Retrieval Against Shipborne In Situ Wind Observations in the European Arctic

January 2024

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77 Reads

IEEE Transactions on Geoscience and Remote Sensing

Space-borne synthetic aperture radar (SAR) observations provide broad coverage of high-resolution snapshots of the sea surface conditions in polar regions. However, their potential has not yet been fully harnessed for meteorological applications. For instance, standard methods for SAR wind-vector retrieval rely on wind direction inputs from numerical weather prediction models, which hampers the high-resolution capabilities of SAR wind retrievals and the use of these in data assimilation. A recently proposed SAR-only wind-vector retrieval method, that uses SAR information more exhaustively than standard methods do, is compared to in situ ship observations and is found to perform similarly to a standard method under average wind conditions at open sea. However, in coastal regions, at high wind speeds, and in complex meteorological conditions this new application outperforms the standard method. It is concluded here that wind fields obtained from the SAR-only wind-vector retrieval are suitable for data assimilation in high-resolution weather prediction models, since they can provide model-independent, high-quality, and high-resolution observational wind information. In addition, a simple interpolation technique is introduced to substitute land in the calibration procedure of the Doppler centroid anomaly for open-ocean SAR scenes.


Correlations between interannual PMT at 67.5° N and Arctic (a) temperature and (b) precipitation, and between interannual PMT at 67.5° S and Antarctic (c) temperature and (d) precipitation. Results represent annual means for present-day conditions (1981–2010), CMIP6 model-mean. The ‘hotspot’ regions denoted by green lines in (a) and (c) are defined to represent areas with relatively high positive correlation between PMT and temperature. Stippled regions indicate where the correlations are significant (see Methods).
Correlations between (a) interannual PMT at 67.5° N and Arctic sea level pressure, and (b) interannual PMT at 67.5° S and Antarctic sea level pressure. Results represent annual means for present-day conditions (1981–2010), CMIP6 model-mean.
Correlation of (a) interannual PMT at 67.5° N and surface air temperature (DJF mean) in the Arctic hotspot region (see figure 1), and (b) interannual PMT at 67.5° S and surface air temperature (DJF mean) in the Antarctic hotspot region (see figure 1). Blue bars represent CMIP6 models (blue dashed line: model mean), purple bars reanalyses data (purple dashed line: reanalyses mean). Results are for present-day (1981–2010).
Fraction of hotspot temperature (N or S) and polar (67.5°–90° N or °S) precipitation variability explained by PMT variability over time. Winter (DJF or JJA) data is used in moving 30 year windows. Evaluated as the ratio of regressions between interannual PMT and temperature or precipitation times PMT, and actual temperature/precipitation anomalies. For temperature we used the hotspot regions (see figure 1) as the mean polar tempature signal is quite low due to opposing regional contributions. Black lines indicate linear trend lines from 1995 onwards (Arctic and Antarctic PMT-PR regressions have an R ² of 0.98 and 0.95, respectively, for a p-value < 0.05). For the Arctic, 2 models did not have a negative trend; all negative trends were significant. For Antarctica, 3 models did not have a negative trend; of all negative trends, 3 were not significant (p-value > 0.05).
Regional polar warming linked to poleward moisture transport variability

September 2023

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130 Reads

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1 Citation

Polar warming, ice melt and strong precipitation events are strongly affected by episodic poleward advection of warm and moist air1,2, which, in turn, is linked to variability in poleward moisture transport (PMT)3. However, processes governing regional impacts of PMT as well as long-term trends remain largely unknown. Here we use an ensemble of state-of-the-art global climate models in standardized scenario simulations (1850–2100) to show that both the Arctic and the Antarctic exhibit distinct geographical patterns of PMT-related warming. Specifically, years with high PMT experience considerable warming over subarctic Eurasia and West-Antarctica4, whereas precipitation is distributed more evenly over the polar regions. The warming patterns indicate preferred routes of atmospheric rivers1, which may regionally enhance atmospheric moisture content, cloud cover, and downward longwave radiative heating in years with comparatively high PMT5. Trend-analyses reveal that the link between PMT-variability and regional precipitation patterns will weaken in both polar regions. Even though uncertainties associated with intermodel differences are considerable, the advection of warm and moist air associated with PMT-variability is likely to increasingly cause mild conditions in both polar regions, which in the Arctic will reinforce sea-ice melt. Similarly, the results suggest that warm years in West-Antarctica disproportionally contribute to ice sheet melt6, enhancing the risk of ice-sheet instabilities causing accelerated and sudden sea-level rise.


On the Impact of Net-Zero Forcing Q-flux Change

September 2023

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70 Reads

Numerical climate model simulations suggest that global warming is enhanced or hampered by the spatial pattern of the warming itself. This phenomenon is known as the ``pattern effect'' and has in recent years become the most promising explanation for the change over time of climate sensitivity in climate models. Under historical global warming, different patterns of surface-temperature change have emerged, notably a yet unexplained cooling in the Southern Ocean and the East Pacific. Historical climate model simulations notoriously fail to reproduce this cooling, which may contribute to the deviation of the simulated global-mean warming from the observed record.Here we qualitatively investigate the potential impact of historical and other surface-temperature pattern changes by changing the ocean heat transport convergence (Q-flux) in a slab-ocean model. The Q-flux changes are always implemented such that in the global mean they impose no net forcing. Consistent with earlier studies we find that the impact of a negative Q-flux change in the Southern Ocean has a stronger effect than in other regions because of a feedback loop between sea-surface temperatures (SSTs) and clouds in the Southern Ocean and the stably stratified regions in the tropics. The SST-cloud feedback loop facilitates the expansion of the Antarctic sea ice, indeed taking the model into a Snowball-Earth state. The intensity of this effect is found to be model dependent, especially due to differences in the cloud parametrisation. In experiments with deactivated sea ice the impact of the negative Q-flux change is much weaker.


On the Control of North-Hemispheric Feedbacks by AMOC, Evidence from CMIP and Slab-Ocean Modeling

June 2023

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45 Reads

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2 Citations

The climate sensitivity of the Earth and the radiative climate feedback both change over time due to a so-called “pattern effect”, i.e., changing patterns of surface warming. This is suggested by numerical climate model experiments. The Atlantic Meridional Overturning Circulation (AMOC) influences surface warming patterns as it redistributes energy latitudinally. Thus, this ocean circulation may play an important role for climate-feedback change over time. In this study, two groups of members of the Coupled Model Intercomparison Project (CMIP) phases 5 and 6 abrupt4xCO2 experiment are distinguished: one group showing weak and the other strong feedback change over time. It is found that both groups differ significantly in the AMOC response to 4xCO 2 . Therefore, experiments with a slab-ocean model (SOM) with quadrupling of the CO 2 concentration are performed where the AMOC change is mimicked by changing the ocean heat transport. It is found that in the Northern Hemisphere extra-tropics the CMIP model group differences can be qualitatively reproduced by the SOM experiments, indicating that the AMOC plays an important role in setting the surface warming pattern. However, in the tropics and especially in the Southern Hemisphere other explanations are necessary.


Citations (18)


... Even after running the simulations for 20 years posteruption, the GMST is still decaying. This long tail in the GMST response is due to increased sea ice fractions in all of S400, S1629, and S3000 that are still outside twice the standard deviation of the control after 20 years, while the sea ice fraction in S26 is within two standard deviations of the control after about 5-10 years, see Enger et al. (2024). ...

Reference:

Saturation in Forcing Efficiency and Temperature Response of Large Volcanic Eruptions
Temperature response to volcanic forcing
  • Citing Preprint
  • October 2024

... More specifically, consistent with previous studies (e.g. Langen and Alexeev 2004, Rose et al 2013, Eiselt and Graversen 2024, the latitude at which the ocean switches from acting as a heat sink to a heat source, as well as the overall level of ocean heat transport, determines whether the growth of sea ice cover accelerates into the lower latitudes or stays restricted to the polar regions. For our simulations, we found that the semi-idealised 4×CO 2 annual-mean q-flux was suitable for sustaining stable polar ice caps. ...

On the impact of net-zero forcing Q-flux change

Climate Dynamics

... Consequently, the likelihood of temporary overshoot pathways-where global mean temperatures exceed 1.5°C before returning back to below this level-is increasing (IPCC, 2021;Schl eussner et al., 2023). The response and reversibility of the climate system under such temporary overshoots are still under-researched, limiting the scientific basis for policy making decisions regarding scenarios of global warming past 1.5°C (Jones et al., 2024;Nature Geoscience Editorial, 2023;Schleussner et al., 2024). ...

Bringing it all together: Science and modelling priorities to support international climate policy

... Given the significant impact of warm-wet extremes on ice-covered regions, Yang, Hu, et al. (2024) pointed out that these areas exhibit a much higher synchrony of extreme warm and precipitation events compared to the midlatitude lands, suggesting paradigm differences of compound warm extremes between non-ice covered regions and ice-covered regions. This synchrony may arise from warm-moist air intrusions discussed by previous studies over Greenland (Barrett et al., 2020;Bintanja et al., 2023;Pettersen et al., 2022;Ward et al., 2020) and Antarctica (Gorodetskaya et al., 2023;Shields et al., 2022;Wang et al., 2023;Wille et al., 2024). ...

Regional polar warming linked to poleward moisture transport variability

... The potential for radiative feedbacks to vary over time as the SST pattern evolves can be interpreted in terms of a forced climate response. For instance, as is seen most clearly under an abrupt CO 2 doubling or quadrupling, SST patterns and thus radiative feedbacks vary as the ocean adjusts on a range of time scales Winton et al. 2010;Armour et al. 2013;Geoffroy et al. 2013;Rose et al. 2014;Rose and Rayborn 2016;Rugenstein et al. 2016;Lin et al. 2019Lin et al. , 2021Eiselt and Graversen 2023). Moreover, non-CO 2 forcing agents, such as anthropogenic aerosols, Antarctic meltwater, or volcanic eruptions, can produce time-varying SST patterns and radiative feedbacks that are distinct from those from CO 2 forcing (Shindell 2014;Gregory et al. 2016;Marvel et al. 2016;Gregory et al. 2020;Dong et al. 2022;Günther et al. 2022;Salvi et al. 2023;Zhou et al. 2023). ...

On the Control of North-Hemispheric Feedbacks by AMOC, Evidence from CMIP and Slab-Ocean Modeling
  • Citing Article
  • June 2023

... Over the Atlantic Ocean the maximum contribution is near 9 km altitude between 5 and 35°N (Figure S1a in Supporting Information S1). The difference in mass fraction between the southern and northern hemisphere is due to climatologically increased poleward transport toward the winter hemisphere (Peixoto & Oort, 1992;Stoll & Graversen, 2022). ...

The global atmospheric energy transport analysed by a wavelength-based scale separation

... In this study, we extend a high-resolution unstructured grid 3-D ocean-sea ice-ice shelf regional model setup 17,22 centred over the Petermann Ice Shelf and Petermann Fjord to include subglacial discharge at the grounding line (Fig. 1). The fjord bathymetry and the ice shelf draft are derived from BedMachine v3 8 . ...

A nested high-resolution unstructured grid 3-D ocean-sea ice-ice shelf setup for numerical investigations of the Petermann ice shelf and fjord

MethodsX

... Early work by Hasselmann et al. (1997) showed how impulse response functions could be efficiently implemented within a Structural Integrated Assessment Model (SIAM) to assess the efficacy of short-and long-term climate policies (Hasselmann, 2001;Hasselmann et al., 2003). Other work has considered the diagnosis of impulse response functions based on effective radiative forcing (ERF) through the use of parameterized relationships to develop better estimates for ERF calculations (Fredriksen et al., 2021(Fredriksen et al., , 2023. Research by Lucarini et al. (2017) and Lembo et al. (2020) has aimed to formalize the diagnosis of climate response functions through the lens of statistical mechanics, showcasing skill in predicting surface temperature fields and changes in both the Atlantic Meridional Overturning Circulation and Antarctic Circumpolar Current. ...

Estimating Radiative Forcing With a Nonconstant Feedback Parameter and Linear Response

... As a result, it is considered less accurate than other remote sensing wind retrieval technologies, e.g., scatterometry [9,10]. Secondly, Tollinger et al. criticized the limitations of established SAR wind retrieval methods and suggested a modified approach [13]. According to them, there are two factors negatively affecting the common methods: (1) the use of co-polarized backscatter signals alone (as opposed to cross-polarized), which saturate with high wind speeds; and (2) the dependence on a priori wind direction information from NWP models. ...

High-Resolution Polar Low Winds Obtained from Unsupervised SAR Wind Retrieval