Diverging hydrological sensitivity among tropical basins

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ABSTRACT The three tropical basins each have unique roles in the global climate system. The main mechanism by which tropical oceans affect remote climate is the latent heating of local


precipitation. Here we report major differences in hydrological sensitivity (precipitation change per unit surface warming) among tropical basins. Specifically, the Pacific hydrological


sensitivity is several times as large as that of the Indian basin, while the Atlantic hydrological sensitivity is negative. This results from a thermodynamic amplification of the existing


spatial unevenness in relative humidity, with the wettest basin getting wetter and the driest basin getting drier. The diverging basin hydrological sensitivity is accompanied by an


interbasin repartitioning of latent heating and convective mass fluxes, with far-reaching implications on rainfall and surface temperature over tropical and mid-latitude lands. These results


indicate that the previously unrecognized interbasin differences in hydrological sensitivity may contribute substantially to the geographic pattern of anthropogenic climate change. Access


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26 October 2020 DATA AVAILABILITY Model output and observation data can be accessed at the following websites: CMIP6, https://esgf-node.llnl.gov/projects/cmip6/; observed SST,


https://pcmdi.llnl.gov/mips/amip/; GPCP, https://psl.noaa.gov/data/gridded/data.gpcp.html; CMAP, https://www.psl.noaa.gov//data/gridded/data.cmap.html; TRMM,


https://disc.gsfc.nasa.gov/datasets/TRMM_3B43_7/summary; ERA5, https://cds.climate.copernicus.eu/cdsapp#!/home; NCEP/DOE-II, https://psl.noaa.gov/data/gridded/data.ncep.reanalysis2.html;


JRA-55, https://jra.kishou.go.jp/JRA-55/index_en.html. CODE AVAILABILITY The CESM model code is publicly available at https://www2.cesm.ucar.edu/models/cesm1.2/. Scripts for the analysis and


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https://doi.org/10.5281/zenodo.10729735 (2024). Download references ACKNOWLEDGEMENTS We thank I. Simpson and M. Ting for helping with the CAM5 and stationary wave model simulations and J.


Lynch-Stieglitz for helping with the writing of the manuscript. J.H. is supported by the National Science Foundation (NSF) grant no. AGS-2047270 and B.F. is supported by NSF grant no.


AGS-2217619. We acknowledge the World Climate Research Programme’s Working Group on Coupled Modelling, which is responsible for CMIP and we thank the climate modelling groups for producing


and making available their model output. For CMIP, the US Department of Energy’s Program for Climate Model Diagnosis and Intercomparison provides coordinating support and led development of


software infrastructure in partnership with the Global Organization for Earth System Science Portals. We acknowledge the CESM Large Ensemble Community Project and supercomputing resources


provided by NSF, the National Center for Atmospheric Research (NCAR) and Yellowstone. We thank the Physical Sciences Laboratory (PSL) of the National Oceanic and Atmospheric Administration


and the Goddard Earth Sciences Data and Information Services Center for providing precipitation observations. We thank the Copernicus Programme, PSL and NCAR for providing the reanalysis


data. AUTHOR INFORMATION AUTHORS AND AFFILIATIONS * School of Earth and Atmospheric Sciences, Georgia Institute of Technology, Atlanta, GA, USA Jie He & Kezhou Lu * Department of


Geosciences, Mississippi State University, Mississippi State, MS, USA Boniface Fosu * Northern Gulf Institute, Mississippi State University, Mississippi State, MS, USA Boniface Fosu *


Department of Geosciences, Princeton University, Princeton, NJ, USA Stephan A. Fueglistaler Authors * Jie He View author publications You can also search for this author inPubMed Google


Scholar * Kezhou Lu View author publications You can also search for this author inPubMed Google Scholar * Boniface Fosu View author publications You can also search for this author inPubMed


 Google Scholar * Stephan A. Fueglistaler View author publications You can also search for this author inPubMed Google Scholar CONTRIBUTIONS J.H. designed the study and led the writing of


the manuscript. J.H. analysed the diverging basin hydrological sensitivity. K.L. conducted and analysed the diabatic heating experiments. B.F. and S.A.F. contributed to the analysis. All


authors contributed to scientific interpretation and the writing of the manuscript. CORRESPONDING AUTHOR Correspondence to Jie He. ETHICS DECLARATIONS COMPETING INTERESTS The authors declare


no competing interests. PEER REVIEW PEER REVIEW INFORMATION _Nature Climate Change_ thanks Ji Nie and the other, anonymous, reviewer(s) for their contribution to the peer review of this


work. ADDITIONAL INFORMATION PUBLISHER’S NOTE Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations. EXTENDED DATA EXTENDED


DATA FIG. 1 INTERBASIN DIFFERENCES IN INDIVIDUAL MODELS. Basin SST change (A), HS (B–D) and percentage change in convective mass flux (E) from the ssp585 multimodel mean (MMM) and individual


models. EXTENDED DATA FIG. 2 IMPACTS OF OCEANIC PRECIPITATION CHANGES ON LAND TEMPERATURE. Land surface temperature response in amipTRP (A), amipTRPadj (B) and the difference between


amipTRP and amipTRPadj (C). Regions where responses are significantly above internal variability (Method) are stippled. EXTENDED DATA FIG. 3 RELATION BETWEEN HYDROLOGICAL SENSITIVITY


METRICS. Intermodel relationship between interbasin discrepancies in A-B) HSmean% and basin mean HSlocal% and C-D) HSmean% and basin mean HSlocal. Intermodel correlation coefficient (R) and


the two-tailed probability value based on the Student’s t-test (p) are shown in texts. EXTENDED DATA FIG. 4 TEMPERATURE CONTRIBUTIONS TO MOIST STATIC ENERGY CHANGES. Multimodel mean present


and future MSE0rel (A) and relative low-level temperature (T0rel, B) averaged for 0.1 °C SSTrel bins for individual basins. Low-level temperature (T0) is defined as the pressure weighted air


temperature averaged between 1000 hPa and 850 hPa. T0rel is defined as T0 minus by the tropical mean T0. SSTrel bins that account for less than 0.5% of the total basin area are shown in


semitransparent colours. EXTENDED DATA FIG. 5 MECHANISMS FOR REGIONAL HYDROLOGICAL SENSITIVITY. Multimodel mean HSlocal% (A, B), MSE0rel change (C, D), RH0 change (E, F) and TRP0 change (G,


H) from the amipUniform and amipAll simulations. EXTENDED DATA FIG. 6 THERMODYNAMIC ORIGINS OF DIVERGING BASIN HYDROLOGICAL SENSITIVITY. Intermodel relationship between interbasin


differences in precipitation-weighted basin mean thermodynamic TRP0 change and those in basin mean precipitation change. Panel A shows the differences between the Pacific and Indian basins


and panel B shows the differences between the Pacific and Atlantic basins. Intermodel correlation coefficient (R) and the two-tailed probability value based on the Student’s t-test (p) are


shown in texts. SUPPLEMENTARY INFORMATION SUPPLEMENTARY INFORMATION Supplementary Figs. 1–8, Texts 1 and 2 and Table 1. RIGHTS AND PERMISSIONS Springer Nature or its licensor (e.g. a society


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of this article is solely governed by the terms of such publishing agreement and applicable law. Reprints and permissions ABOUT THIS ARTICLE CITE THIS ARTICLE He, J., Lu, K., Fosu, B. _et


al._ Diverging hydrological sensitivity among tropical basins. _Nat. Clim. Chang._ 14, 623–628 (2024). https://doi.org/10.1038/s41558-024-01982-8 Download citation * Received: 06 September


2023 * Accepted: 18 March 2024 * Published: 09 April 2024 * Issue Date: June 2024 * DOI: https://doi.org/10.1038/s41558-024-01982-8 SHARE THIS ARTICLE Anyone you share the following link


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