Abstract
High Mountain Asia (HMA) has experienced a spatial imbalance in water resources in recent decades, partly because of a dipolar pattern of precipitation changes known as South Drying–North Wetting1. These changes can be influenced by both human activities and internal climate variability2,3. Although climate projections indicate a future widespread wetting trend over HMA1,4, the timing and mechanism of the transition from a dipolar to a monopolar pattern remain unknown. Here we demonstrate that the observed dipolar precipitation change in HMA during summer is primarily driven by westerly- and monsoon-associated precipitation patterns. The weakening of the Asian westerly jet, caused by the uneven emission of anthropogenic aerosols, favoured a dipolar precipitation trend from 1951 to 2020. Moreover, the phase transition of the Interdecadal Pacific Oscillation induces an out-of-phase precipitation change between the core region of the South Asian monsoon and southeastern HMA. Under medium- or high-emission scenarios, corresponding to a global warming of 0.6–1.1 °C compared with the present, the dipolar pattern is projected to shift to a monopolar wetting trend in the 2040s. This shift in precipitation patterns is mainly attributed to the intensified jet stream resulting from reduced emissions of anthropogenic aerosols. These findings underscore the importance of considering the impact of aerosol emission reduction in future social planning by policymakers.
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Data availability
The large-ensemble simulations and multimodel simulations are publicly available from the Earth System Grid Federation (https://esgf-node.llnl.gov/search/cmip6/). The GPCC data are available from the National Oceanic and Atmospheric Administration (NOAA) Physical Sciences Laboratory (https://psl.noaa.gov/data/gridded/data.gpcc.html). The CRU data are available from the CEDA Archive (https://catalogue.ceda.ac.uk/). The CN05.1 data are provided by the Climate Change Research Center, Chinese Academy of Sciences (https://ccrc.iap.ac.cn/resource/detail?id=228). The APHRODITE data are available from APHRODITE’s water resources (http://aphrodite.st.hirosaki-u.ac.jp/products.html). The GPM IMERG v.06B final run can be obtained from NASA (https://gpm.nasa.gov/data/imerg). HAR v.2 is available from Fachgebiet Klimatologie (https://www.klima.tu-berlin.de/index.php?show=daten_har2&lan=de). The JRA-55 reanalysis products can be downloaded from the NCAR Research Data Archive (https://rda.ucar.edu/datasets/ds628-1/). The ERA-5 reanalysis products are available from the Climate Data Store (https://cds.climate.copernicus.eu/cdsapp#!/dataset/reanalysis-era5-land-monthly-means?tab=form). The ERSST data were provided by the NOAA National Centers for Environmental Information (https://www.ncei.noaa.gov/products/extended-reconstructed-sst). Source data are provided with this paper.
Code availability
The data in this study are analysed with the NCAR Command Language (NCL) and Scilab. All the maps are generated using NCL. The core codes of the optimal fingerprint method are provided by ref. 72. Other key codes are publicly available from Harvard Dataverse (https://doi.org/10.7910/DVN/VKXNNW).
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Acknowledgements
This work is jointly supported by the National Natural Science Foundation of China (grant no. 41988101), the second Tibetan Plateau Scientific Expedition and Research (STEP) programme (grant no. 2019QZKK0102), and the Strategic Priority Research Program of the Chinese Academy of Sciences (grant no. XDA20060102). J.J. is supported by the National Natural Science Foundation of China (grant no. 42205034) and the Special Research Assistant Project of the Chinese Academy of Sciences. F.S. is supported by the National Natural Science Foundation of China (grant no. 42175029). Y.Q. acknowledges support by the US Department of Energy (DOE), Office of Science and Office of Biological and Environmental Research (BER), as part of the Earth and Environmental System Modeling programme. The Pacific Northwest National Laboratory (PNNL) is operated for the DOE by the Battelle Memorial Institute under contract DE-AC05-76RLO1830. We also acknowledge support from the Jiangsu Collaborative Innovation Center for Climate Change.
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T.Z. conceived and designed the study, with support from J.J. and Y.Q. J.J. conducted the analysis and drafted the manuscript. T.Z., Y.Q., C.L., F.S., H.L., X.C., W.Z. and Z.C. provided comments and revised the manuscript. Y.Q., C.L. and H.L. edited the paper. All the authors contributed to the scientific interpretation of the results.
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Extended data figures and tables
Extended Data Fig. 1 Long-term changes in summer precipitation in and around HMA.
a-f, The linear trends of summer precipitation (mm·month−1·decade−1) in and around HMA derived from the GPCC (a), CRU (b), CN05.1 (c), APHRO (d), JRA-55 (e) and ERA-5 data (f). The stippling indicates that the trend is significant at the 10% level according to the Mann-Kendall test; numbers denote the periods used to calculate the trends. The boundaries of HMA are identified as an isoline of 2500 m according to Global Multi-resolution Terrain Elevation Data 201052. g, h, Time series of 9-year running mean precipitation anomalies (mm·month−1) relative to a period from 1995–2014 over northern HMA (g, northern box in a) and southeastern HMA (h, southern box in a) derived from GPCC (black), CRU (gray), CN05.1 (orange), APHRO (blue), GPM (red, 2000–2020) and HAR data (purple, 1980–2020).
Extended Data Fig. 2 The two leading modes of summer precipitation over HMA.
a-f, The two leading modes (EOF1 and EOF2) based on an EOF analysis of the 9-year running mean of summer precipitation (mm·month−1) in and around HMA derived from GPCC (a, b), CRU (c, d) and APHRO data (e, f). Numbers denote the corresponding explained variances. The boundaries of HMA are identified as an isoline of 2500 m according to Global Multi-resolution Terrain Elevation Data 201052. g, h, The corresponding time series of the two leading modes (PC1 and PC2) derived from GPCC (black), CRU (red) and APHRO data (blue).
Extended Data Fig. 3 The mechanisms of the long-term trend in the westerly associated precipitation pattern over HMA in summer.
a-b, The linear trends of the moisture budget terms (mm·month−1·decade−1) associated with the first mode averaged over northern (a) and southeastern (b) HMA from 1958-2020. c-g, Linear trends of the vertical advection term (c, mm·month−1·decade−1), vertical velocity (d, Pa·s−1·decade−1, negative values denote upward motion), geostrophic relative vorticity (e, shading in units of 10−6·s−1·decade−1), and horizontal wind at 500 hPa (f, vector in units of m·s−1·decade−1) associated with the first mode from 1958 to 2020. The vector in e denotes the climatological (1995–2014) horizontal wind (m·s−1) at 500 hPa; the shading in f denotes the climatological temperature (K) at 500 hPa. g, Climatological zonal wind at 200 hPa. The box denotes the core zone of the subtropical westerly jet (SWJ). Above results are derived from JRA-55. The boundaries of HMA are identified as an isoline of 2500 m according to Global Multi-resolution Terrain Elevation Data 201052. h, Time series of 9-year running mean location (°; black) and strength (m·s−1; blue) of the jet axis derived from JRA-55 (solid lines) and ERA-5 (dashed lines). The latitude position with maximal wind speed averaged over 40° ~ 120°E denotes the location of the jet axis.
Extended Data Fig. 4 Long-term changes in SWJ over HMA under different external forcings.
a, The linear trends of the SWJ strength index (m·s−1·decade−1; see Methods) derived from JRA-55 (1958–2020) and ERA-5 (1959–2020) associated with the first mode and the multimodel ensemble mean under ALL, NAT, GHG and AA forcings (1951–2020). Error bars denote the 25–75% range of all models (n = 10). b-e, The linear trends of zonal wind at 200 hPa (b, c, m·s−1·decade−1) and tropospheric temperature (d, e, K·decade−1) from 1951 to 2020 under GHG (b, d) and AA (c, e) forcings derived from the multimodel average of 10 CMIP6 models. The stippling indicates that the trend is significant at the 10% level according to the Mann-Kendall test. The blue contours denote the climatological zonal wind (m·s−1) at 200 hPa from 1995–2014. f, g, The meridional gradient of the temperature trend in d and e. The boundaries of HMA are identified as an isoline of 2500 m according to Global Multi-resolution Terrain Elevation Data 201052.
Extended Data Fig. 5 Long-term changes in summer precipitation over HMA under different external forcings.
a-d, The linear trends of precipitation (mm·month−1·decade−1) from 1951 to 2020 under ALL (a), AA (b), GHG (c) and NAT (d) forcings derived from the multimodel average of 10 CMIP6 models. The stippling indicates that the trend is significant at the 10% level according to the Mann-Kendall test. The boundaries of HMA are identified as an isoline of 2500 m according to Global Multi-resolution Terrain Elevation Data 201052.
Extended Data Fig. 6 Long-term changes in summer precipitation over HMA under all external forcings for models with different horizontal resolutions.
a-b, Linear trends of precipitation (mm·month−1·decade−1) from 1951–2020 under all external forcings derived from the average of a group of CMIP6 models with resolutions lower (a) and higher (b) than 1.25° × 1.25° (Extended Data Table 1). The stippling indicates that the trend is significant at the 10% level according to the Mann-Kendall test. c, The differences in the linear trends between the models with higher and lower resolutions. The boundaries of HMA are identified as an isoline of 2500 m according to Global Multi-resolution Terrain Elevation Data 201052.
Extended Data Fig. 7 The relationship between the monsoon-associated precipitation pattern and IPO.
a, c, The correlation coefficients between the internal component of area-averaged summer (JJAS) precipitation over the South Asian monsoon core zone and the internal component of gridded precipitation from 1951–2020 in ACCESS-ESM1-5 (a) and MIROC6 (c). Boxes denote the domains of the South Asian monsoon core zone and southeastern HMA. b, d, The correlation coefficients between the corresponding time series of the monsoon-associated precipitation pattern and the internal component of sea surface temperature from 1951–2020 in ACCESS-ESM1-5 (b) and MIROC6 (d). The correlation coefficients for individual members are calculated, and the averages are shown. The stippling indicates that more than 80% of the members agree with the signal. The boundaries of HMA are identified as an isoline of 2500 m according to Global Multi-resolution Terrain Elevation Data 201052.
Extended Data Fig. 8 Future changes in precipitation over HMA.
a-f, The linear trends of precipitation (mm·month−1·decade−1) under the SSP2-4.5 (a-c) and SSP5-8.5 (d-f) scenarios from 2021-2100 derived from the ensemble mean of ACCESS-ESM1-5 (a, d) and MIROC6 (b, e) and the multimodel average of 10 CMIP6 models (c, f). The stippling indicates that the trend is significant at the 10% level according to the Mann-Kendall test. The boundaries of HMA are identified as an isoline of 2500 m according to Global Multi-resolution Terrain Elevation Data 201052.
Extended Data Fig. 9 Future changes in precipitation and the subtropical westerly jet in the summer under the SSP2-4.5 scenario.
Linear trends of precipitation (a, c, e, g; mm·month−1·decade−1) and 200 hPa zonal wind (b, d, f, h; m·s−1·decade−1) under the SSP2-4.5 (a, b), SSP2-4.5-aer (c, d), SSP2-4.5-GHG (e, f), and SSP2-4.5-nat (g, h) scenarios from 2021-2100 derived from the ensemble mean of MIROC6. The stippling indicates that the trend is significant at the 10% level according to the Mann-Kendall test. The boundaries of HMA are identified as an isoline of 2500 m according to Global Multi-resolution Terrain Elevation Data 201052.
Extended Data Fig. 10 The performance of CMIP6 models on climatological precipitation over HMA.
The climatological mean of summer precipitation (mm·month−1) in and around HMA derived from multiple observations (GPCC, CRU, APHRO and GPM) and the historical simulations of 12 CMIP6 models from 1995–2014. For the GPM, the period of 2001–2020 is used. For each model, the results of the ensemble mean are shown. Numbers denote the pattern correlation coefficients of HMA precipitation between the corresponding model and GPCC data. The boundaries of HMA are identified as an isoline of 2500 m according to Global Multi-resolution Terrain Elevation Data 201052.
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Jiang, J., Zhou, T., Qian, Y. et al. Precipitation regime changes in High Mountain Asia driven by cleaner air. Nature 623, 544–549 (2023). https://doi.org/10.1038/s41586-023-06619-y
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DOI: https://doi.org/10.1038/s41586-023-06619-y
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