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Supplement of Atmos. Chem. Phys., 18, 17489 17496, 2018 https://doi.org/10.5194/acp-18-17489-2018-supplement Author(s) 2018. This work is distributed under the Creative Commons Attribution 4.0 License. Supplement of Insignificant effect of climate change on winter haze pollution in Beijing Lu Shen et al. Correspondence to: Lu Shen (lshen@fas.harvard.edu) The copyright of individual parts of the supplement might differ from the CC BY 4.0 License.

Table S1. Correlations of the 2010-2017 PM 2.5 concentrations in Beijing in winter with an array of first principal components (PC1s) constructed using different combinations of meteorological variables and the predicted trends of winter PM 2.5 implied by these PC1s. Experiment # Variables Correlation of PC1 with PM 2.5 (DJF, 2010-2017) Predicted PM 2.5 Trend (DJF, 1973-2017, µg m -3 a -1 ) Predicted PM 2.5 Trend (DJF, 1993-2017, µg m -3 a -1 ) 1 RH, V850 0.90-0.12 (p=0.63) 0.001 (p=0.99) 2 RH, WS 0.88-0.20 (p=0.37) -0.64 (p=0.19) 3 RH, δu500 0.85 0.12 (p=0.59) 0.034 (p=0.93) 4 RH, V850, WS a 0.90-0.21 (p=0.31) -0.50 (p=0.27) 5 RH, V850, 0.91 NA b -0.46 (p=0.33) 6 7 δt 925-1000hPa RH, V850, WS, δt 925-1000hPa, δu500 RH, V850, WS, δt 925-1000hPa 0.90 NA -0.65 (p=0.13) 0.92 NA -0.78 (p=0.10) Average -0.08 (p=0.71) -0.43 (p=0.33) a WS is for surface wind speed. b Missing data because the observed δt 925-1000hPa from radiosonde is available only after 1993. 2

Table S2. Models from the Coupled Model Intercomparison Project Phase 5 (CMIP5) used for this study. Model Name Institute ACCESS1.0 a,b Commonwealth Scientific and Industrial Research Organization (CSIRO) and Bureau of Meteorology (BOM), Australia ACCESS1.3 a,b BCC-CSM1-1 a,b BNU-ESM a,b CanESM2 a,b CCSM4 a CESM1-CAM5 a CMCC-CM a CMCC-CMS a,b CNRM-CM5 a,b CSIRO-MK3-6-0 a,b FIO-ESM a GFDL-CM3 a,b GFDL-ESM2M a,b GFDL-ESM2G a,b GISS-E2-H a GISS-E2-R a HadGEM2-AO a HadGEM2-CC a,b HadGEM2-ES a INMCM4 a,b IPSL-CM5A-LR a,b IPSL-CM5A-MR a,b IPSL-CM5B-LR a,b MIROC-ESM a,b MIROC-ESM- CHEM a,b CSIRO and BOM, Australia Beijing Climate Center, China Meteorological Administration College of Global Change and Earth System Science, Beijing Normal University Canadian Centre for Climate Modelling and Analysis National Center for Atmospheric Research Community Earth System Model Contributors Centro Euro-Mediterraneo per i Cambiamenti Climatici Centro Euro-Mediterraneo per i Cambiamenti Climatici Centre National de Recherches Météorologiques / Centre Européen de Recherche et Formation Avancée en Calcul Scientifique Commonwealth Scientific and Industrial Research Organization in collaboration with Queensland Climate Change Centre of Excellence The First Institute of Oceanography, SOA, China NOAA Geophysical Fluid Dynamics Laboratory NOAA Geophysical Fluid Dynamics Laboratory NOAA Geophysical Fluid Dynamics Laboratory NASA Goddard Institute for Space Studies NASA Goddard Institute for Space Studies Met Office Hadley Centre (additional HadGEM2-ES realizations contributed by Instituto Nacional de Pesquisas Espaciais) Met Office Hadley Centre (additional HadGEM2-ES realizations contributed by Instituto Nacional de Pesquisas Espaciais) Met Office Hadley Centre (additional HadGEM2-ES realizations contributed by Instituto Nacional de Pesquisas Espaciais) Institute for Numerical Mathematics Institut Pierre-Simon Laplace Institut Pierre-Simon Laplace Institut Pierre-Simon Laplace Japan Agency for Marine-Earth Science and Technology, Atmosphere and Ocean Research Institute (The University of Tokyo), and National Institute for Environmental Studies Japan Agency for Marine-Earth Science and Technology, Atmosphere and Ocean Research Institute (The University of Tokyo), and National Institute for Environmental Studies 3

Atmosphere and Ocean Research Institute (The University of Tokyo), MIROC5 a,b National Institute for Environmental Studies, and Japan Agency for Marine-Earth Science and Technology MPI-ESM-LR a Max-Planck-Institut für Meteorologie (Max Planck Institute for Meteorology) MPI-ESM-MR a,b Max-Planck-Institut für Meteorologie (Max Planck Institute for Meteorology) MRI-CGCM3 a,b Meteorological Research Institute NORESM1-M a Norwegian Climate Centre NORESM1-ME a Norwegian Climate Centre a The 32 models, each with monthly archives of meteorology. b The 21 models, each with daily archives of meteorology. 4

%a -1 Fig. S1. Slopes of winter RH with reconstructed wintertime PM 2.5 concentrations in Beijing during 1973-2016 in (a) gridded global land and surface humidity dataset (HadISDH, https://www.metoffice.gov.uk/hadobs/hadisdh/) and (b) NCEP renanlysis. (c) Timeseries of mean DJF RH in Beijing from HadISDH and NCEP reanalysis. Because RH in the NCEP reanalysis is biased high, we reduce its magnitude by 23% in the plot. Fig. S2. (a) Same as Fig. 1a, but for the zonal wind speed at 500 hpa. We define δu500 as the difference between the mean zonal wind speed in the box north of Beijing (95 E-130 E, 47.5 N- 55 N) and that in the box south of Beijing (120 E-145 E, 27.5 N-35 N). (b) Relationship of V850 and δu500 during winter months of 1973-2017, with the correlation coefficient shown inset. 5

(a) PM 2.5 vs. NCEP V850 (b) PM 2.5 vs. obs surface wind (c) PM 2.5 vs. obs RH V850 (m/s) -6-5 -4-3 -2-1 R=0.81 Wind (m/s) 2.5 3.0 3.5 4.0 R=-0.80 RH (%) 30 40 50 60 R=0.78 50 100 150 200 PM 2.5 (µg/m3) 50 100 150 200 PM 2.5 (µg/m3) 50 100 150 200 PM 2.5 (µg/m3) (d) PM 2.5 vs. obs δt (1000-925 hpa) (e) PM 2.5 vs. NCEP δu500 ΔT (K) 2.0 3.0 4.0 R=0.70 Wind (m/s) -35-25 -15 R=0.64 50 100 150 200 PM 2.5 (µg/m3) 50 100 150 200 PM 2.5 (µg/m3) Fig. S3. Relationships of DJF monthly PM 2.5 concentrations with local and regional variables: (a) V850, (b) observed surface wind speed, (c) observed surface relative humidity, (d) potential temperature gradient between 925 and 1000 hpa, and (e) δu500. The correlation coefficients are shown inset. Definitions of V850 and δu500 are found in Fig. 1a and Fig. S3a. DJF PC1s using different meteorological variables PC1-2 -1 0 1 2 p = 0.50 1980 1990 2000 2010 Fig. S4. Timeseries of PC1s calculated from seven different combinations of meteorological variables (dashed color lines). Details of these combinations are described in Table S1. The thick black line refers to the ensemble mean PC1. Shaded area denotes one standard deviation across ensemble members. The linear trend (blue line) of ensemble mean PC1 during 1993-2017 is insignificant (p = 0.50). 6

(a) Site distribution (b) DJF surface wind speed Wind speed (m/s) 1.5 2.5 3.5 4.5 13 obs sites in NCP Beijing obs site Beijing grid in NCEP (-2 m/s) 1980 1990 2000 2010 Fig. S5. (a) The geographical distribution of the 13 observation sites from the GSOD network used here. The Beijing site is highlighted. (b) Timeseries of 1973-2017 mean surface wind speed in winter at the Beijing site, the 13 sites in the North China Plain, and NCEP reanalysis. Because wind speed in the NCEP reanalysis is biased high in Beijing, we reduce its magnitude by 2 m s -1 in the plot. 7

Fig. S6. (a) Observed trend of potential temperature gradient between 925 and 1000 hpa during the winters of 1993-2017. The sites with significant trend (p<=0.1) are circled. (b) Same as (a), but for the NCEP reanalysis. Gridboxes with significant trend (p<=0.1) are stippled. Panels (d-f) are same as (a-c), but for the trend of potential temperature gradient between 850 and 925 hpa. 8

Fig. S7. Slopes of sea surface temperatures (SSTs) in the preceding months with DJF PC1 in Beijing during 1973-2017. Gridboxes with statistically significant correlations (p<0.1) are stippled. 9

Fig. S8. Slopes of sea surface temperatures (SSTs) in the preceding months with DJF PC1 in Beijing during 1973-2017. Only regions with significant slopes are shown. The wind anomalies at 850 hpa relative to the 1973-2017 mean are overlaid. K 10

Fig. S9. (a) Correlations of DJF mean relative humidity in Beijing with DJF SSTs during 1973-2017. The black rectangle denotes the domain of Indian Ocean. (b) Correlations of mean SSTs in the Indian Ocean with relative humidity in East Asia. Only regions with significant correlations (p<0.1) are shown. All data are detrended by subtracting the 7-year moving average. The relative humidity is obtained from gridded global land surface humidity data (HadISDH, https://www.metoffice.gov.uk/hadobs/hadisdh/). 11

DJF meteorological changes from 2000-2019 to 2080-2099 in RCP8.5 K ms -1 ms -1 ms -1 mm/day mon -1 Fig. S10. Meteorological changes in DJF from 1970-1999 to 2079-2099 in the RCP8.5 scenario. These meteorological variables include (a) potential temperature gradient between 925 and 1000 hpa, (b) zonal wind speed at 500 hpa, (c) wind speeds at 500 hpa, (d) surface wind speeds, (e) precipitation, and (f) number of stagnant days. Gridboxes where more than 70% of the models show a consistent sign of changes are stippled. For panels (a-b), we use the 32 climate models that provide monthly archives (Table S2). For panels (c-f), we use the 21 climate models that provide daily archives (Table S2). The open triangle is the location of Beijing. We classify a day as stagnant when the daily mean near-surface wind speed is less than 3.2 m s -1, daily mean midtropospheric wind speed is less than 13 m s -1, and daily accumulated precipitation is less than 1 mm (Horton et al., 2012). 12

(a) Corr V850 with U500 1.00 (b) ΔV850 by 2100s 20% (b) Δ δu500 by 2100s 20% Correlation (R) 0.75 0.50 0.25 Relative change 10% 0% -10% Relative change 10% 0% -10% 0.00-20% Fig. S11. (a) Correlation of V850 and δu500 in the winter months of 2000-2019 from an ensemble of 32 CMIP5 models. (b) The relative change of V850 from 2000-2019 to 2080-2089. (c) Same as (b) but for δu500. -20% 13