There are different drivers that may influence decadal-multidecadal changes in large scale oceanic circulations over the North Atlantic (Fig. 1). These include: 1) natural internal variability in the atmosphere (e.g., Wunsch 1999; Feldstein 2000; Eden and Willebrand 2001) and ocean (Sévellec and Fedorov 2013; Moat et al. 2024), 2) internal coupled ocean–atmosphere processes (Delworth et al. 1993; Dong and Sutton 2005; Omrani et al. 2014; Ortega et al. 2015; Lai et al. 2022), 3) responses to external forcings, such as anthropogenic forcings in greenhouse gas forcing (Gregory et al. 2005; Delworth and Dixon 2006; Graff and LaCasce 2012; Lee et al. 2021) and aerosol emissions (Delworth and Dixon 2006; Bellomo et al. 2018; Menary et al. 2020; Hassan et al. 2021; Robson et al. 2022), and 4) responses to external natural forcings, such as the changes of solar radiation (Mignot et al. 2011; Menary et al. 2014; Ye et al. 2023a) and volcanic eruptions (Swingedouw et al. 2017; Marshall et al. 2022; Paik et al. 2023).
3.2.1 Internal Variability
Ocean-only experiments suggest that decadal-multidecadal AMOC variability in the North Atlantic primarily results from buoyancy forcing over subpolar regions (Eden and Willebrand 2001; Marshall et al. 2001; Böning et al. 2006; Robson et al. 2012; Yeager and Danabasoglu 2014). Many previous coupled atmosphere-ocean model simulations with constant forcings have also exhibited substantial multidecadal variations in AMOC and have associated this variability with the internal interactions of ocean currents or with coupled interactions between different components of the coupled system (e.g., ice, ocean, and atmosphere) in the North Atlantic region (Delworth et al. 1993; Vellinga and Wu 2004; Dong and Sutton 2005; Jungclaus et al. 2005; Park and Latif 2008; Delworth and Zeng 2012; Menary et al. 2015; Ortega et al. 2015; Wills et al. 2019; Jiang et al. 2021; Jackson et al. 2022; Lai et al. 2022; Meccia et al. 2023). In many of the studies the propagation of freshwater from the Arctic (e.g., Jungclaus et al. 2005; Jiang et al. 2021) or salinity anomalies from the south (Delworth et al. 1993; Vellinga and Wu 2004), and the dominant timescales are set by advective processes, such as the spin-up/spin-down of the North Atlantic SPG circulation or the accumulation of high-/low-density water in deep water formation regions. However, many studies also indicate an important role for atmospheric circulation changes due to ocean-atmosphere coupling (e.g., Omrani et al. 2022; Lai et al. 2022). Some studies also suggest that Rossby wave adjustment, with little or no influence of the atmosphere, can be the dominant driver of decadal timescale AMOC variability, especially within the subpolar latitudes (Sevelec and Fedorov 2013; Muir and Fedorov 2017).
3.2.2 Anthropogenic forcings
3.2.2.1 The response to greenhouse gas forcing
There is general agreement that increasing concentrations of greenhouse gases act to weaken the AMOC in climate models (Gregory et al. 2005; Delworth and Dixon 2006; Stouffer et al. 2006; Caesar et al. 2018; Thornalley et al. 2018; Menary et al. 2020; Eyring et al. 2021). Weakening of the AMOC under greenhouse gas forcing results from both reduced heat loss to the atmosphere and increasing freshwater fluxes at high latitudes, both leading to lighter surface waters and lighter surface waters may lead to a reduction of deep convection in sinking regions and thus impact the strength of the AMOC (e.g., Gregory et al. 2005; Manabe and Stouffer 1994; Stouffer et al. 2006; Eyring et al. 2021). Advection of heat and salinity anomalies into the North Atlantic deep convection region can also affect the AMOC. For instance, studies have also attributed a weakening of the AMOC in GCMs to Arctic sea ice loss (Sévellec et al. 2017) and subsurface warming of the North Atlantic (Haskins et al. 2020; Levang and Schmitt 2020), which both increase ocean stratification and inhibit deep convection. However, the amount, the rate and the effects of this decline are highly uncertain across models (Gregory et al. 2005; Collins et al. 2013; Weijer et al. 2020; Bellomo et al. 2021; Gulev et al. 2021; Lee et al. 2021; Fox-Kemper et al. 2021). The response to decreasing greenhouse gas concentrations has recently been examined (Schwinger et al. 2022). Overshoot scenarios show reduction of AMOC and subsequent recovery (see Section 3.4.2). However the AMOC response depends strongly on peak GHG concentrations and the rate at which they are then removed.
3.2.2.2 The response to aerosol forcing
Many studies have highlighted that AAer forcing can have a large impact on the North Atlantic, and AAer forcing has been shown to strengthen the AMOC in climate models (Cai et al. 2006; Delworth and Dixon 2006; Undorf et al. 2018a, b; Andrews et al. 2020; Menary et al. 2020; Hassan et al. 2021; Robson et al. 2022). Menary et al. (2020) showed that the multimodel mean AMOC increased significantly over 1850–1985 in historical simulations of CMIP6 models. Furthermore, Menary et al. (2020) attributed the AMOC increase to stronger AAer forcing in CMIP6 compared to CMIP5, primarily due to the inclusion of aerosol–cloud interactions in more models although increases in the temporal variability of CMIP6 emissions may also play a role (Needham et al. 2024). Hassan et al. (2021) showed that CMIP6 AAer simulations yield robust AMOC strengthening (weakening) in response to increasing (decreasing) anthropogenic aerosols during 1900–2020. They argued that AMOC multi-decadal variability is initiated by North Atlantic aerosol optical thickness perturbations to net surface shortwave radiation, sea surface temperature, and hence sea surface density. Robson et al. (2022) analyzed CMIP6 historical simulations in order to understand the processes leading to the anthropogenic aerosol AAer forced increase in AMOC over the period 1850–1985. They split models between “strong” or “weak” sensitivity to AAer forcing and explained differences of AMOC response. They showed that in both strong and weak changes in AAer effects on AMOC are via changes in downwelling surface shortwave radiation over the subpolar North Atlantic (SPNA), similar to Hassan et al. (2021). However, in models with a strong sensitivity turbulent heat loss over the SPNA is significantly larger because the air advected over the ocean is colder and drier, in turn because of greater AAer-forced cooling over the continents upwind, especially North America. Robson et al. (2022) also argued that the strengthening of the AMOC also feeds back on itself positively in two distinct ways: by raising the sea surface temperature and hence further increasing turbulent heat loss in the SPNA, and by increasing the sea surface density across it due to increased northward transport of saline water.
After 1985, the role of AAer forcings on AMOC is less clear. This lack of clarity is partly due to the fact that greenhouse gases are also contributing to a simulated decline. However, the changes in AAer emissions becomes much more complex, with large regional changes but small changes in global mean emissions (Kang et al. 2021). Furthermore, there is some evidence that the response of AMOC to AAer emissions from different regions may be non-linear (e.g., Liu et al. 2024).
3.2.3. Natural forcings
The oceanic response to solar forcing associated with the 11-year solar cycle could be amplified by ocean-atmosphere coupling the North Atlantic Ocean (Gray et al. 2013; Scaife et al. 2013; Andrews et al. 2015; Ye et al 2023a). Andrews et al. (2015) and Gray et al. (2016) showed that the accumulated solar energy in the mixed layer of the North Atlantic could generate a response lag of 3–4 years of surface atmospheric pressure to the decadal solar cycle, which in turn could affect AMOC. For example, Ye et al. (2023a) assessed the influence of varied total solar irradiance (TSI) due to the effects of solar activity on AMOC based on an Earth System model with intermediate complexity and the results showed a significant and stable negative correlation between TSI and AMOC on a multidecadal timescale. However, there is a growing debate regarding the influence of solar activity on AMOC change (Ye et al. 2023a).
Volcanic eruptions may also affect the AMOC (Swingedouw et al. 2017; Marshall et al. 2022; Paik et al. 2023) and AMV. Based on a high-resolution 600-year proxy temperature record from the subtropical Atlantic, Waite et al. (2020) detected multidecadal temperature variability from the record which suggests a link between the volcanic eruption and the AMV. Using climate model simulations, Pausata et al. (2015b) found that large summer high-latitude eruptions in the Northern Hemisphere cause strong hemispheric cooling which induces an El Niño-like anomaly during the first 8–9 months after the start of the eruption in response to hemispherically asymmetric cooling. The high-latitude eruption also leads to a strengthening of the AMOC in the first 25 years after the eruption, followed by a weakening of the AMOC that lasts at least 35 years. However, the AMOC response to volcanic forcing is poorly constrained and likely to be sensitive to the period, distribution, and strength of the forcing (Mignot et al. 2011, Bilbao et al. 2024) and the background state (Zanchettin et al. 2013); For example, some models suggesting the response to volcanic forcing is a weakening (Zhong et al. 2011), some a strengthening (Stenchikov et al. 2009; Iwi et al. 2012).
3.2.4 Arctic influences on the North Atlantic
Arctic – Subarctic heat and freshwater fluxes play a central role in linking Arctic Ocean variability with the North Atlantic. On the one hand, the North Atlantic constitutes a net source of heat for the Arctic. On the other hand, the Arctic constitutes a source of freshwater for the North Atlantic. In this section, we focus on changes and driving mechanisms of freshwater fluxes from the Arctic into the North Atlantic.
Freshwater enters the Arctic Ocean as net precipitation, as river runoff from the Siberian and Alaskan-Canadian shelves, and as inflow from the Pacific through Bering Strait, and it leaves the Arctic through Davis Strait and eastern Fram Strait, both in the form of liquid freshwater and as ice (Carmack et al. 2016). For instance, over the period 1980–2000, freshwater import and export rates were approximately balanced, with estimates ranging from 7,950 ± 400 km3 yr− 1 (Serreze et al. 2006) to 8,800 ± 530 km3 yr− 1 (Haine et al. 2015) for the net import rates and from 8,720 ± 700 km3 yr− 1 (Serreze et al. 2006) to 8,700 ± 700 km3 yr− 1 (Haine et al. 2015) for the net export rates (Carmack et al. 2016).
The release of freshwater from the Arctic into the North Atlantic is not uniform but occurs in isolated time-limited events (Proshutinsky et al. 2015). Between 1950 and 2000, observations indicate four distinct, large Arctic freshwater releases into the North Atlantic. These observed, past Arctic freshwater releases are manifest as distinct periods of cold and fresh polar water in hydrographic observations from the Nordic Seas and subpolar North Atlantic (Belkin et al. 1998; Haak 2003; Belkin 2004; Sundby and Drinkwater 2007). A particularly strong freshwater event was the Great Salinity Anomaly from 1969 to 1972, which was associated with a temporary shutdown of ocean convection in the Labrador Sea, an important ocean convection region (Dickson et al. 1988; Lazier 1980). Weaker freshwater anomalies occurred in the 1980s and 1990s (Belkin et al. 1998; Belkin 2004; Sundby and Drinkwater 2007). Yet, the duration of the Arctic freshwater releases, and the exact pathways, propagation speed and arrival times in the subpolar North Atlantic and Nordic Seas differed between these freshwater releases.
Over the period 2000–2010, the Arctic has accumulated freshwater (Haine et al. 2015; Proshutinsky et al. 2019; Solomon et al. 2021; Wang et al. 2020; 2023; Wang 2021; Timmermans and Toole 2023). Most of the freshwater has been stored in the upper layers of the Arctic Ocean, particularly in the Beaufort gyre, where it is estimated that an extra 5,000 km3(25%) of freshwater has been stored in the period 2000–2010 compared to the period 1980–2000 (Haine et al. 2015). After the period 2000–2010, the Arctic freshwater storage has stabilised (Solomon et al. 2021). Moreover, a comprehensive set of observations suggests that the cold halocline layer, which caps the warm, salty Atlantic water, has significantly thinned and that further thinning may allow for an emerging freshwater release into the North Atlantic (Lin et al. 2023). The recent observed changes in the North Atlantic salinity are thought to be influenced by the freshwater excess coming from the Arctic (Holliday et al. 2020). However, so far there is only limited evidence of the Arctic freshwater fluxes impacting freshwater accumulation in the Labrador Sea and the North Atlantic (Florindo-Lopez et al. 2020)
The extended period of accumulation and increased storage of freshwater in the Arctic over the last two decades has primarily been attributed to the wind forcing (Giles et al. 2012; Haine et al. 2015; Proshutinsky and Johnson, 1997). Specifically, a more cyclonic ocean and atmospheric circulation in the Arctic have been suggested to lead to enhanced outflow of freshwater from the Beaufort Gyre into the Transpolar drift, and in the Arctic boundary currents following the shelf slopes, then further through Davis Strait and Fram Strait into the Nordic Seas and North Atlantic (Proshutinsky and Johnson 1997; Proshutinsky et al. 2019; Solomon et al. 2021). On the other hand, a more anticyclonic circulation promotes an enhanced storage of freshwater in the Beaufort Gyre, due to wind-driven Ekman transports setting up a cross-gyre pressure gradient with increased sea level in the central gyre (Proshutinsky and Johnson 1997). This accumulation can be balanced by the eddy transports releasing freshwater from the gyre (Armitage et al. 2020). This fresh water leakage from the gyre due to eddies may become larger as sea ice declines and the ocean spins up (Meneghello et al. 2018).
Over the period 2000–2015, the atmospheric and oceanic circulation in the Arctic have primarily been in a more anticyclonic regime (Armitage et al. 2017; Proshutinsky et al. 2015, 2019; Kelly et al. 2019; Regan et al. 2019). The observed changes in the Arctic surface currents for the more recent years were indicative of the Arctic ocean circulation returning to the more cyclonic state with the Beaufort Gyre shrinking back (Lin et al. 2023; Nishino et al., 2023).
While past Arctic freshwater releases constituted an integral part of the low-frequency, decadal variability (Zhang and Vallis 2006), the extent to which Arctic ice and freshwater releases act as a driver, a response or a side effect of the North Atlantic low-frequency variability is unclear. Progress is impeded by reduced spatial and temporal coverage of long-term salinity observations, as well as by freshwater biases in models (Mecking et al. 2017; Menary et al. 2015). In theory, Arctic releases of cold and fresh polar water into the subpolar region could lead to an increased meridional SST gradient and thus, an increase in atmospheric instability, triggering atmospheric feedbacks (Oltmanns et al. 2020, 2024) which give rise to predictability (Zhang and Vallis 2006). For instance, subpolar cold and freshwater anomalies are typically coupled to a positive North Atlantic Oscillation, which is associated with a stronger wind stress curl increasing the advection of cold and fresh polar water into the subpolar gyre (Häkkinen and Rhines 2004; Häkkinen et al. 2013; Holliday et al. 2020; Oltmanns et al. 2020).
In turn, changes in the North Atlantic Ocean and atmospheric circulation can feed back on processes in the Arctic by modulating ice and freshwater outflows. Specifically, observations show an increased heat transport into the Arctic due to warmer Atlantic water, resulting in a thinning of the halocline (Asbjørnsen et al. 2020; Polyakov et al. 2017, 2023; Tesi et al. 2021; Wang 2021). By integrating a two-sided coupling between the Arctic and North Atlantic into an idealised delayed, harmonic oscillator model, it is possible to reproduce the observed, multi-decadal variability of the North Atlantic Ocean (Wei and Zhang 2022). Still, the active role of the North Atlantic Ocean and atmospheric circulations in influencing the ocean and atmospheric circulations in the Arctic and hence, ice and freshwater exports are largely unknown.