Abstract
The Pacific–South America (PSA) teleconnection pattern triggered by the El Niño/Southern Oscillation (ENSO) is suggested to be moving eastward and intensifying under global warming. However, the underlying mechanism is not completely understood. Previous studies have proposed that the movement of the PSA teleconnection pattern is attributable to the eastward shift of the tropical Pacific ENSO-driven rainfall anomalies in response to the projected El Niño-like sea surface temperature (SST) warming pattern. In this study, we found that with uniform warming, models will also simulate an eastward movement of the PSA teleconnection pattern, without the impact of the uneven SST warming pattern. Further investigation reveals that future changes in the climatology of the atmospheric circulation, particularly the movement of the exit region of the subtropical jet stream, can also contribute to the eastward shift of the PSA teleconnection pattern by modifying the conversion of mean kinetic energy to eddy kinetic energy.
Introduction
The El Niño/Southern Oscillation (ENSO), as the primary interannual air-sea coupled mode in the tropical Pacific, has significant effects on the global climate variability (Hoerling et al., 1997; Horel and Wallace 1981; Hu et al., 2021; Liu and Alexander 2007; Trenberth et al., 1998; Xie et al., 2016; Straus and Shukla 2002; Yang et al., 2018; Sun et al., 2019; Sun et al., 2022). The ENSO has a three-pronged effect on the climate variability in the extratropics of the Southern Hemisphere. To begin, El Niño events warm the tropical atmosphere at all longitudes, resulting in the strengthening and equatorward movement of the subtropical jet stream (STJ) and descending branches of the Hadley circulation (Rind et al., 2001; Seager et al., 2003; Lu et al., 2008). Second, ENSO can affect the Southern Hemisphere Annular Mode by influencing the propagation and intensity of transient eddies (Fogt et al., 2011; L'Heureux and Thompson 2006; Lau and Lau 1992; Lau et al., 2005; Seager et al., 2003). Third, the ENSO signal is capable of propagating to mid- and high-latitudes, as well as to Antarctica, via stationary waves generated by the anomalous tropical convection in the tropical Pacific (Held et al., 2002; Schneider et al., 2012). In the Southern Hemisphere, the ENSO teleconnection resembles the Pacific–South American (PSA) wave train characterized by alternating pressure centers east of New Zealand, near the Amundsen Sea and South America, curving poleward and eastward toward Antarctica, highly impacting the depth of the Amundsen Sea Low (Karoly 1989; Mo and Higgins 1998; Mo and Paegle 2001; Schneider et al., 2012). The variability of the Amundsen Sea Low could further modulate the temperature and sea ice anomalies over Antarctica (Yuan and Martinson 2000; Yuan 2004; Li et al., 2015; Wang et al., 2020; Wang et al., 2022).
The PSA teleconnection pattern triggered by ENSO events is strongly seasonally dependent and is zonally asymmetric during El Niño and La Niña years (Jin and Kirtman 2009; Hitchman and Rogal 2010; Ding et al., 2012; Schneider et al., 2012; Li et al., 2021). The seasonality of the PSA being more pronounced in austral winter and spring is primarily attributable to the seasonal variation in the STJ. A stronger and more equatorward STJ in austral winter and spring favors the formation of the Rossby wave source (Sardeshmukh and Hoskins 1988) in the subtropical Pacific, resulting in a more pronounced PSA teleconnection pattern (Jin and Kirtman 2009; Scott Yiu and Maycock, 2019). The asymmetric impacts between the warm and cold phase of ENSO, which exhibit a more eastward PSA wave train during El Niño than La Niña, can be attributable to the shift of the anomalous tropical convection and the discrepancy of the STJ (Hoerling et al., 1997; Wang et al., 2021; Wang et al., 2022).
Under global warming, Pacific–North American (PNA) and the PSA teleconnection pattern triggered by ENSO events are both projected to move eastward and intensify (Zhou et al., 2014; Cai et al., 2021). Previous studies have proposed that the movement of the teleconnection pattern is attributable to the eastward shift of the ENSO-driven rainfall anomalies over the tropical Pacific in response to the projected El Niño-like warming pattern (Zhou et al., 2014; Cai et al., 2021; Hu et al., 2021). As a result of the overall reduction of the tropical circulations due to the increased static stability in the tropics under greenhouse warming, the tropical Pacific sea surface temperature (SST) change features an El Niño-like warming pattern (Held and Soden 2006; Huang and Xie 2015; Yeh et al., 2018). The background warming pattern, in turn, results in the intensification and the eastward movement of the ENSO-driven rainfall anomalies in the tropical Pacific (Power et al., 2013; Huang and Xie 2015). In response to the changes in the ENSO-driven rainfall anomalies, the extratropical Rossby wave trains, as the PSA and PNA teleconnection pattern, are projected to shift eastward and strengthen in previous studies (Cai et al., 2021; Zhou et al., 2014; Yeh et al., 2018).
In addition to tropical heating anomalies, the PSA teleconnection pattern is modulated by the extratropical circulation (Meehl et al., 2007; Muller and Roeckner 2008). Several early (Simmons et al., 1983; Ting and Yu 1998) and recent studies (Wang et al., 2021; Wang et al., 2022) have suggested that the STJ is critical in determining the position of extratropical ENSO teleconnections. Here, we showed that the eastward shift of the PSA teleconnection pattern is presented even without the impact of the uneven SST warming pattern, in which the future change of climatological circulation plays an important role.
The remainder of this study is organized as follows: Section 2 introduces data and methods. Section 3 presents the results involving the changes in the teleconnection pattern and the underlying mechanisms. Section 4 provides a summary.
Data and Methods
a. Reanalysis and model data
To investigate the future change of the ENSO-triggered PSA teleconnection pattern under global warming, a set of atmospheric-only experiments from the phase 6 of the Coupled Model Intercomparison Project (CMIP6) is utilized. The experiments, namely, AMIP, AMIP-p4K with uniform warming, and AMIP-future4K with patterned warming, are simulated by the atmospheric general circulation models. AMIP is forced by the observed monthly sea ice and SST; the latter two are forced by the observed SST anomalies and the uniform SST, and patterned climatological SST obtained from CMIP5 ensemble mean SST changes at 4 × CO2, respectively. The details of the models are listed in Table 1.
TABLE 1
| Model | Institute |
|---|---|
| BCC-CSM2-MR | Beijing Climate Center, China |
| CanESM5 | Canadian Centre for Climate Modelling and Analysis, Canada |
| CESM2 | National Center for Atmospheric Research, USA |
| CNRM-CM6-1 | Centre National de Recherches Meteorologiques, France |
| GFDL-CM4 | National Oceanic and Atmospheric Administration, Geophysical Fluid Dynamics Laboratory, USA |
| IPSL-CM6A-LR | L’Institut Pierre-Simon Laplace, France |
| MRI-ESM2-0 | Meteorological Research Institute, Japan |
| MIROC6 | The University of Tokyo, National Institute for Environment Studies, and Japan Agency for Marine-Earth Science and Technology, Japan |
AMIP models from CMIP6 used in this study.
In this study, the July–August (JJA) mean geopotential height is derived from the European Centre for Medium-Range Weather Forecasts Interim Reanalysis (ERAI;
Berrisford et al., 2011) at a resolution of 2.5° × 2.5° from 1979 to 2014. The Niño 3.4 index is from the climate prediction center of NOAA (
https://www.cpc.ncep.noaa.gov/), and the principal component of the first empirical orthogonal functional mode of the SST over the tropical Pacific (120°E–80°W, 15°S–15°N) is defined as the Niño index in the AMIP simulations. Regression analysis is used, and the statistical significance of this study is evaluated by the two-tailed Student’s t-test.
b. Linearized Baroclinic Model (LBM)
The LBM used in this study is based upon the primitive equations linearized at a given state with a horizontal resolution of T42 and 20 sigma levels and schemes for horizontal and vertical diffusion, Rayleigh friction, and Newtonian damping. This model is widely used and has an irreplaceable role in the study of climate dynamics (
Xie et al., 2009;
Hu et al., 2019). More details of the model are presented in
Watanabe and Kimoto (2000). To produce a stable atmospheric response to the heating forcing, the model is integrated for 50 days, and the average from the 20th to 50th day is used for analysis.
c. Kinetic energy conversion
As stated by Kosaka and Nakamura (2006), the barotropic growth of the local kinetic energy associated with perturbations from the basic state is given by
Here, and are the anomalous zonal and meridional winds, respectively. and denote the zonal and meridional climatological winds, respectively. KEH is horizontal perturbed kinetic energy, and CK (the sum of CKx and CKy) is the conversion of local kinetic energy from the basic state to atmospheric anomalies.
Results
a. Evaluation of the AMIP simulations of the ENSO-triggered PSA teleconnection pattern.
The atmospheric anomalies triggered by ENSO during austral winter are depicted in
Figure 1in observations and AMIP. In the tropical Pacific, the anomalous convective heating excites a Gill-like response (
Figure 1A). The extratropical teleconnection pattern resembles the PSA wave train, characterized by an anomalous low-pressure center east of New Zealand, a high-pressure anomaly near the Amundsen Sea in the Pacific sector. The structure of the atmospheric responses to ENSO in the AMIP is comparable to that observed with a pattern correlation coefficient between atmospheric anomalies in ERAI and AMIP (0–90°S; 0–360°) of up to 0.79. The resemblance shows that the AMIP models are capable of simulating the ENSO teleconnection in the Southern Hemisphere. It should be noted that the intensity of the PSA teleconnection pattern in AMIP is weaker than observed, suggesting that there may be some common bias in AMIP models, but this inaccuracy does not affect our conclusions as we mainly made comparisons between different AMIP experiments. As a result, it is feasible to undertake subsequent investigations using these simulations.
b. Results in AMIP-p4K and AMIP-future4K
FIGURE 1
Figure 2A presents the ENSO-driven rainfall anomalies in the tropical Pacific in AMIP. Positive responses are distributed in the eastern and central Pacific, whereas negative responses are found on the north flank of the equatorial eastern Pacific which is mainly contributed by the anomalous dry advection (Su and Neelin 2002). In comparison to AMIP, ENSO-driven precipitation anomalies increase in the central and eastern Pacific in the AMIP-future4K and decrease in the western tropical Pacific, resulting in an overall eastward shift and amplification of the precipitation anomalies in the tropical Pacific (Figure 2C). The changes between AMIP-future4K and AMIP are consistent with prior results based on the future simulations in CMIP5/6, which suggest that the El Niño-like warming pattern leads to an eastward shift and intensification of ENSO convective anomalies in the tropical Pacific (Huang and Xie 2015).
FIGURE 2
Compared with the PSA teleconnection pattern in AMIP, the experimental result from AMIP-future4K displays a more eastward and more intense PSA teleconnection pattern (Figures 2B,D). The concurrent intensification and the eastward movement of the ENSO-driven rainfall anomalies in the tropical Pacific and the PSA teleconnection pattern in AMIP-future4K are consistent with earlier studies (Zhou et al., 2014; Cai et al., 2021). When only the climatological SST differs between AMIP and AMIP-future4K, this discrepancy brings several additional changes, including changes in the water vapor, the position of ENSO-driven precipitation anomalies, and the background atmospheric circulation. Previous studies have suggested that all these factors may have an effect on the ENSO teleconnection pattern (Held and Soden 2006; Huang and Xie 2015; Hu et al., 2021).
To disentangle the above factors and examine the causal relationship between each factor and the future changes in the PSA teleconnection pattern, the AMIP-p4K experiment is further introduced for comparison. AMIP-p4K results show a minor increase in ENSO-driven rainfall anomalies over the northeastern tropical Pacific and a decrease in the central and southwestern Pacific relative to that in the AMIP experiment (Figure 2E). The amplitude of ENSO-driven rainfall anomalies over the tropical Pacific in AMIP-p4K is significantly smaller than that in AMIP-future4K and is insufficient to cause the eastward shift and intensification of ENSO-driven precipitation anomalies relative to that in AMIP.
By further comparing the circulation changes in AMIP-p4K and AMIP-future4K, we found that the El Niño-like warming pattern significantly intensifies the PSA wave train (Figures 2D,F). Corresponding to more intense precipitation anomalies in AMIP-future4K with the El Niño-like warming pattern, the strength of the PSA teleconnection pattern is significantly stronger than that in AMIP, whereas the PSA teleconnection pattern in AMIP-p4K is comparable to that in AMIP. The result demonstrates that the future climatological warming pattern contributes to the intensification of the ENSO-triggered PSA teleconnection pattern.
In terms of the movement of the PSA teleconnection pattern, despite the substantial difference in the climatological SST between the two experiments, the PSA teleconnection pattern shifts a comparable distance. This finding suggests that the causal link between the movement of the ENSO-driven rainfall anomalies in the tropical Pacific and the shift of the PSA wave train may be insufficiently robust, and other causes may potentially contribute to the shift of the PSA teleconnection pattern.
The STJ is critical in the development of the subtropical disturbance via barotropic energy conversion (Simmons et al., 1983), acting as an anchor for the location of the ex-tropical wave train triggered by the tropical heating (Ting and Yu 1998). The variation of the STJ plays an important role in the asymmetric impacts of ENSO on the PSA teleconnection pattern by altering the barotropic energy conversion (Wang et al., 2021). In the following study, the movement of the PSA teleconnection pattern under global warming is investigated from the perspective of energy conversion.
Figure 3 presents the climatological zonal winds and the CK in three experiments. In AMIP, the positive CK at the exit of the STJ is consistent with the position of the atmospheric anomaly east of New Zealand (Figures 2B, 3A), indicating the importance of the CK in the development of the disturbance. The majority of the positive CK at the exit of the STJ is contributed by CKx (Figures 3A,B). According to Eq. 1, the zonally elongated (u’>v’) atmospheric anomaly east of New Zealand is eager to extract barotropic energy (CKx) from the basic mean flow (Figure 3A) and develops at the exit region of the STJ where the mean zonal flow is confluent (; Figure 4A).
FIGURE 3
FIGURE 4
In AMIP-future4K, the exit region of the STJ with substantial confluence shifts eastward at about 10° longitudes (Figure 4B). As the exit region of the STJ moves eastward (see the navy and red solid circles in Figure 4B), the strong positive CK favorable to the development of atmospheric anomalies move eastward in lockstep (see the navy and red solid circles in Figure 3B). Similar to AMIP-future4K, the eastward shift of the PSA teleconnection pattern in AMIP-p4K is accompanied by the movement of the STJ exit and the positive CK in the subtropical Pacific (Figures 3C, 4C).
The aforementioned result illustrates that the movement of the climatological STJ exit region contributes to the shift of the PSA teleconnection pattern. To further confirm the effect of STJ changes on the PSA teleconnection pattern, a set of LBM experiments are utilized for investigation, following Wang et al. (2022). The first LBM experiment (EXP1) is forced by the heating source centered at 150°W (Figures 5A,B) and the JJA climatological mean flow. The prescribed heating source has a cosine elliptical pattern, with a peak of −3 K day−1 at the 0.45 sigma level. The horizontal distribution and the vertical profile of the heating source are presented in Figures 5A,B, respectively. The second experiment (EXP2) utilizes the same heating source but shifts the mean flow 20° longitude westward, mimicking the movement of the STJ exit region. In EXP1, the atmospheric response to the tropical heating in the subtropical Pacific is centered at the exit of the STJ, where the climatological zonal flow is significantly confluent (Figures 5C,D). Similar to the experimental results in AMIP experiments, the strong positive CK which contributes to the development of the disturbance is detected at the exit of the STJ in EXP1. However, in EXP2, with the same tropical heating source, the strong positive CK in the mid-latitudes moves westward, paralleling the change of the exit of the climatological STJ (Figure 5D). The consistent movement of the positive CK and disturbance in the subtropical Pacific (Figures 5E,F) demonstrate that the movement of the STJ exit region causes a shift in the position of the PSA teleconnection pattern by modifying the conversion of mean kinetic energy to eddy kinetic energy.
FIGURE 5
Conclusion and Discussion
In this study, the underlying mechanisms of the eastward shift and intensification of the ENSO-triggered PSA teleconnection pattern under global warming are investigated based on a set of AMIP experiments from CMIP6.
By comparing the AMIP-p4K and AMIP-future4K, it is found that the El Niño-like warming significantly intensifies the PSA wave train. Corresponding to more intense precipitation anomalies over tropical Pacific in AMIP-future4K with patterned warming, the strength of the PSA teleconnection pattern is significantly stronger than that in AMIP, whereas the PSA teleconnection pattern in AMIP-p4K with uniform warming is comparable to that in AMIP.
We found that the PSA teleconnection pattern triggered by ENSO will still shift eastward under global warming with the absence of El Niño-like SST warming. Despite the significant difference in the climatological SST between AMIP-p4K and AMIP-future4K, the PSA teleconnection pattern shifts a comparable distance in the two experiments relative to that in AMIP. Further investigation reveals that changes in the climatological STJ, particularly the movement of the exit region of the STJ, can significantly affect the position of the PSA teleconnection pattern by influencing the conversion of mean kinetic energy to eddy kinetic energy. The eastward shift of the exit region of the Pacific STJ in both experiments causes the position where the disturbance is most likely to develop to move eastward, which in turn leads to the eastward shift of the PSA teleconnection pattern. Our results, therefore, emphasize the importance of the climatological circulation change on the projected eastward shift of the PSA teleconnection pattern.
The mechanism proposed in this study complements the previous mechanism (Cai et al., 2021; Kug et al., 2010; Meehl et al., 2007; Muller and Roeckner, 2008; Zhou et al., 2014), and taken together, they may collectively contribute to the eastward shift of the PSA teleconnection pattern. This study is based on AMIP experiments which do not incorporate air–sea coupling processes; further research using the coupled model should be conducted in the future to better understand the issue and quantify the contributions of the STJ, SST warming pattern, and the CO2 direct radiation to the eastward movement and the intensification of the ENSO-triggered PSA teleconnection pattern.
Statements
Data availability statement
The data that supports the finding of this study is openly available at https://www.ecmwf.int/en/forecasts/datasets/reanalysis-datasets (ERAI; Berrisford et al., 2011), and https://esgf-node.llnl.gov/search/cmip6/ (CMIP6).
Author contributions
YW, GH, and KH conceived the study, performed the analyses, built the mechanism, and wrote the manuscript. WT, HG, KY, and HT contributed to improving the manuscript and assisted in the interpretation of the results.
Funding
The study is jointly supported by the National Key R&D Program of China (2018YFA0605904), the National Natural Science Foundation of China (42141019, 41831175, 91937302, 42175040, and 41721004), and the Youth Innovation Promotion Association of CAS (2021072).
Conflict of interest
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
Publisher’s note
All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors, and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.
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Summary
Keywords
El Niño/Southern oscillation, Global Warming, Subtropical Jet Stream, Pacific–South American teleconnection pattern, ENSO teleconnection
Citation
Wang Y, Huang G, Hu K, Tao W, Gong H, Yang K and Tang H (2022) Understanding the Eastward Shift and Intensification of the ENSO Teleconnection Over South Pacific and Antarctica Under Greenhouse Warming. Front. Earth Sci. 10:916624. doi: 10.3389/feart.2022.916624
Received
09 April 2022
Accepted
26 May 2022
Published
22 July 2022
Volume
10 - 2022
Edited by
Minghu Ding, Chinese Academy of Meteorological Sciences, China
Reviewed by
Sulan Nan, Chinese Academy of Meteorological Sciences, China
Bo Sun, Nanjing University of Information Science and Technology, China
Zhiqiang Gong, BCC, China
Updates
Copyright
© 2022 Wang, Huang, Hu, Tao, Gong, Yang and Tang.
This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: Gang Huang, hg@mail.iap.ac.cn; Kaiming Hu, hkm@mail.iap.ac.cn
This article was submitted to Atmospheric Science, a section of the journal Frontiers in Earth Science
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