Many studies have evaluated the performance of multiple global climate models (GCMs) from a temporal or spatial perspective at finer resolution, but no study has evaluated the performance of individual GCMs at different resolutions and before and after bias correction from both temporal and spatial perspectives. The goal of this study is to evaluate the performance of 21 Coupled Model Inter-comparison Project 6 (CMIP6) GCMs at the raw (coarser) and downscaled (finer) resolutions and after bias correction in relation to their skills in the simulation of daily precipitation and maximum and minimum temperatures over China for the period 1961–2014 using state-of-the-art temporal and spatial metrics, Kolmogorov–Smirnov statistic and SPAtial EFficiency. The results indicated some differences in the ranks of GCMs between temporal and spatial metrics at different resolutions. The overall ranking shows that the simulations at the raw resolution of GCMs are more similar to the observations than the simulations after inverse distance weighted interpolation in SPAtial EFficiency. Three variables from bias-corrected GCMs ranked from 1 to 21 show similar good performance in spatial patterns but the poorest trend in empirical Cumulative Distribution Functions (ECDFs) except daily precipitation.

  • Evaluation of the performance of GCMs for daily precipitation and maximum and minimum temperatures based on spatio-temporal assessment metrics.

  • Evaluation of the performance of GCMs at coarse and finer resolutions and those after bias correction.

The Intergovernmental Panel on Climate Change (IPCC) states that human activity has caused global warming of 1.0 °C over the past 100 years and is likely to reach 1.5 °C between 2030 and 2052 (Masson-Delmotte et al. 2018). Climatic extremes such as temperature and precipitation extremes are sensitive to climate warming (Fischer et al. 2014; Ji & Kang 2015; Kharin et al. 2018; Lorenz et al. 2019), and these extremes are often associated with profound effects on ecosystems (Terando et al. 2012; Wheeler & Von Braun 2013; Gu et al. 2020; Zhang et al. 2022). It is necessary to get reliable future climate change information to mitigate the adverse impacts of climate change.

The state-of-the-art GCM simulations from Coupled Model Inter-comparison Project Phase 6 (CMIP6) are expected to improve the representation of the Earth's climate system developed by different institutions around the world (Eyring et al. 2016). The quantification of climate change impacts is often achieved by using global climate model (GCM) simulations with downscaling or bias correction techniques (Cook et al. 2020; Hirabayashi et al. 2021; Xu et al. 2021; Adib & Harun 2022).

Some studies evaluated the performance of variables in GCMs according to their performance over historical periods, using various methods such as the reliability ensemble averaging method (Giorgi & Mearns 2003), relative entropy (Shukla et al. 2006), Bayesian approach (Min & Hense 2006), probability density function (Perkins et al. 2007), hierarchical ANOVA models (Sansom et al. 2013), clustering (Knutti et al. 2013), correlation (Jiang et al. 2015; Xuan et al. 2017), symmetrical uncertainty (Salman et al. 2018), multiple spatial metrics (Ahmed et al. 2019) and Taylor diagram (Ngoma et al. 2020). Furthermore, the performance of GCMs is evaluated at different temporal scales, daily (Perkins et al. 2007), monthly (Srinivasa Raju et al. 2017), seasonal (Ngoma et al. 2020) and annual scales (Murphy et al. 2004). In addition to temporal scales, a number of studies ranked GCMs re-gridded based on spatial average or all the grid covering the study area (Salman et al. 2018; Abbasian et al. 2019).

Ojha et al. (2014) applied a variable convergence score to evaluate 10 atmospheric variables associated with downscaling precipitation and found higher consistency across GCMs for pressure and temperature, and lower consistency for precipitation and related variables in India. Abbasian et al. (2019) used performance criteria including mean deviation, RMSE, NSE, r, Kolmogorov–Smirnov (KS) statistic, Sen's slope estimator and Taylor diagram to evaluate precipitation and temperature, and found that most GCMs perform well in simulating the annual and seasonal temperature but poorly in simulating precipitation, especially at the seasonal scale over Iran. Cui et al. (2021) re-gridded daily temperature and precipitation for the period 1961–2012 in 29 GCMs from CMIP6 with bilinear interpolation and found good performance in simulating the sign of the trends in extreme indices but underestimated their magnitudes and misrepresent spatial patterns. Yang et al. (2021) compared temperature and precipitation in 20 GCMs from CMIP6 with gridded observation data for the period 1995–2014 and found that CMIP6 models show a good ability to capture the climatological distributions of temperature and precipitation, with better performance for temperature than precipitation over China.

Accordingly, this study focuses on the assessment of the performance of daily precipitation and maximum and minimum temperatures from GCMs in temporal and spatial aspects from 1961 to 2014 in mainland China. Before the application of climate variables, spatio-temporal indicators are usually used to evaluate the temperature and precipitation of climate patterns after interpolation (Abbasian et al. 2019; Ahmed et al. 2019). When climate variables are applied to the impact study of climate change, it needs to be interpolated first. The use of spatial and temporal indicators to evaluate the performance of climate variables from GCM and primary climate variables input into the hydrological model is important for the reprocessing of the climate variables output from the climate model into the hydrological model. However, seldom do studies focus on the performance of climate variables at the scale of raw GCMs. Through the spatio-temporal analysis of the climate variables before and after interpolation and after deviation correction, the performance of precipitation and temperature from the raw climate model to the input of the hydrological model was evaluated in this study. The rest of the paper is arranged as follows: Section 2 presents the study area and datasets, and Section 3 presents a brief introduction to the methodology, including the temporal and spatial metrics, interpolation and bias correction methods. Section 4 presents the results, followed by the discussion and conclusion in Section 5. The spatial and temporal evaluation methods and the evaluation results of corrected climate variables from raw, interpolated and bias-corrected GCM could be helpful in the selection of GCMs in hydrologic impact studies, and this would be applied to the study of the hydrological response in climate change.

Study region and data

This study used a gridded meteorological dataset () over China for the period of 1961–2014. This dataset contains three climate variables, including daily precipitation, and daily minimum and maximum temperatures, which are downloaded from the China Meteorological Data Sharing Service System (http://www.cma.gov.cn/) to represent the observed data. This gridded dataset came from 2472 in situ observation gauge stations across China and was interpolated using the thin plate spline method of GTOPO30 (Global 30 Arc-Second Elevation) data sampling (Zhang et al. 2015). This dataset can well simulate the daily precipitation and temperature of the historical period in China and is often used as observational data (Wan et al. 2021; Yin et al. 2021).

The elevation data of the mainland of China were from the Resources and Environment Science and Data Center (https://www.resdc.cn/Datalist1.aspx?FieldTyepID=9,13). Also, the observed daily maximum and minimum temperatures and precipitation in the grid of China were used (see Figure 1).
Figure 1

The elevation map of China and the location of the grid points (back dots) at finer resolution used in this study.

Figure 1

The elevation map of China and the location of the grid points (back dots) at finer resolution used in this study.

Close modal

GCM temperature and precipitation data

Daily precipitation and maximum and minimum temperatures in 21 GCMs (Table 1) extracted from the CMIP6 data center (https://esgf-node.llnl.gov/projects/cmip6/) were selected from 1961 to 2014 in GCMs.

Table 1

CMIP6 GCMs considered in this study

CountryModeling centerModel nameResolution in degree
(lon. × lat.)
China Beijing Climate Center BCC-CSM2-MR 1.125° × 1.1213° 
Institute of Atmospheric Physics, Chinese Academy of Sciences FGOALS-g3 2° × 2.2785° 
Canada Canadian Center for Climate Modelling and Analysis CanESM5 2.8125° × 2.7893° 
France Centre National de Recherches Météorologiques, Centre Européen de Recherche et de Formation Avancée en Calcul Scientifique CNRM-CM6-1 1.4063° × 1.4004° 
CNRM-ESM2-1 
Institut Pierre-Simon Laplace IPSL-CM6A-LR 2.5° × 1.2676° 
Australian Collaboration for Australian Weather and Climate Research ACCESS-ESM1-5 1.8750° × 1.25° 
ACCESS-CM2 1.8750° × 1.25° 
Netherlands–Ireland EC-EARTH consortium published at Irish Centre for High-End Computing EC-Earth3 0.7031° × 0.7017° 
EC-Earth3-Veg 
Russia Russian Academy of Sciences, Institute of Numerical Mathematics INM-CM4-8 2° × 1.5° 
INM-CM5-0 
Japan Atmosphere and Ocean Research Institute (The University of Tokyo), National Institute for Environmental Studies and Japan Agency for Marine-Earth Science and Technology MIROC6 1.4063° × 1.4004° 
MIROC-ES2L 2.8125° × 2.7893° 
Meteorological Research Institute MRI-ESM2-0 1.1250° × 1.1213° 
UK Met Office Hadley Centre HadGEM3-GC31-LL 1.8750° × 1.25° 
UKESM1-0-LL 
Germany Max Planck Institute for Meteorology MPI-ESM1-2-HR 0.9375° × 0.9349° 
MPI-ESM1-2-LR 1.875° × 1.8647° 
Norway Bjerknes Centre for Climate Research, Norwegian Meteorological Institute NorESM2-MM 1.25° × 0.9424° 
USA Geophysical Fluid Dynamics Laboratory GFDL-ESM4 1.25° × 1° 
CountryModeling centerModel nameResolution in degree
(lon. × lat.)
China Beijing Climate Center BCC-CSM2-MR 1.125° × 1.1213° 
Institute of Atmospheric Physics, Chinese Academy of Sciences FGOALS-g3 2° × 2.2785° 
Canada Canadian Center for Climate Modelling and Analysis CanESM5 2.8125° × 2.7893° 
France Centre National de Recherches Météorologiques, Centre Européen de Recherche et de Formation Avancée en Calcul Scientifique CNRM-CM6-1 1.4063° × 1.4004° 
CNRM-ESM2-1 
Institut Pierre-Simon Laplace IPSL-CM6A-LR 2.5° × 1.2676° 
Australian Collaboration for Australian Weather and Climate Research ACCESS-ESM1-5 1.8750° × 1.25° 
ACCESS-CM2 1.8750° × 1.25° 
Netherlands–Ireland EC-EARTH consortium published at Irish Centre for High-End Computing EC-Earth3 0.7031° × 0.7017° 
EC-Earth3-Veg 
Russia Russian Academy of Sciences, Institute of Numerical Mathematics INM-CM4-8 2° × 1.5° 
INM-CM5-0 
Japan Atmosphere and Ocean Research Institute (The University of Tokyo), National Institute for Environmental Studies and Japan Agency for Marine-Earth Science and Technology MIROC6 1.4063° × 1.4004° 
MIROC-ES2L 2.8125° × 2.7893° 
Meteorological Research Institute MRI-ESM2-0 1.1250° × 1.1213° 
UK Met Office Hadley Centre HadGEM3-GC31-LL 1.8750° × 1.25° 
UKESM1-0-LL 
Germany Max Planck Institute for Meteorology MPI-ESM1-2-HR 0.9375° × 0.9349° 
MPI-ESM1-2-LR 1.875° × 1.8647° 
Norway Bjerknes Centre for Climate Research, Norwegian Meteorological Institute NorESM2-MM 1.25° × 0.9424° 
USA Geophysical Fluid Dynamics Laboratory GFDL-ESM4 1.25° × 1° 

In this study, GCMs for daily precipitation and maximum and minimum temperatures were first ranked separately (individual ranking) using temporal and spatial performance measures, KS statistic and spatial metrics (SPAtial Efficiency (SPAEF)). The bias correction method was used for the GCMs and ranked as below. The procedure used for the research is outlined as follows:

  • The resolution of observation is at finer resolution, and the observed daily precipitation and maximum and minimum temperatures for the period 1961–2014 are remapped to the original grid of the GCM-simulated resolution by the mean grid method for the observation at coarser resolution. The data from raw GCMs are interpolated to finer resolution with inverse distance weighted interpolation (Shepard 1968).

  • KS statistic and spatial metrics (SPAEF) are individually applied to daily precipitation and maximum and minimum temperatures for the period 1961–2014 at both finer and coarser resolution.

  • The goodness-of-fit (GOF) estimated by KS and SPAEF for daily precipitation, and maximum and minimum temperatures is used to rank the GCMs separately at both finer and coarser resolution.

  • The bias correction method is used for the GCMs at finer resolution, and the ranks are used for them and the difference between GCMs in different resolution and metrics are compared.

Assessment metrics

The temporal (KS) and spatial metrics (SPAEF) were individually applied from 1961 to 2014 to daily precipitation and maximum and minimum temperatures, respectively. Later, the GOF values of each day were temporally averaged to obtain a value for the entire study area. The details of the two metrics are given in the following.

KS statistic

We take the KS test (Massey 1951) as a measure to determine the ability of the GCMs to represent the probability density functions (PDFs) of the observed variables (cma precipitation and maximum and minimum temperatures). The KS measures the maximum vertical distance between the cumulative distribution functions (CDFs) of the simulated models and the observation, which is sensitive to the median, variance and shape of the CDFs. Its value ranges between 0 and 1, and the value closer to 0 refers to a better agreement between the simulated and observed daily precipitation and maximum and minimum temperature. Also, the statistic can be expressed as follows:
(1)
where and are the CDFs of the observations and simulations, respectively. The empirical CDFs (ECDFs) and boxplots of the simulations and observations are presented for a better comparison of observations and GCMs (see Figure 2).
Figure 2

The ECDFs and boxplots of daily precipitation from cma and the GCM simulations.

Figure 2

The ECDFs and boxplots of daily precipitation from cma and the GCM simulations.

Close modal

SPAEF metric

SPAEF (Demirel et al. 2018), which considers three statistical measures, Pearson correlation, coefficient of variation and histogram overlap, in the assessment of GCMs, is a robust spatial performance metric. The SPAEF values between observed and GCMs were calculated using Equation (2). In Equation (2), α is the Pearson correlation coefficient between observed and GCM-simulated daily precipitation and maximum and minimum temperature, is the spatial variability, and is the overlap between the histograms of observed and GCM-simulated daily precipitation and maximum and minimum temperature:
(2)
Equations (3) and (4) show the calculations for and , respectively. In Equation (3), and refer to the standard deviations of the simulated and observed data and and refer to the mean values of the simulated and observed data, respectively;
(3)
In Equation (4), K, L and N refer to the histogram values of observations, the simulations and the number of bins in a histogram;
(4)

The values of SPAEF are between −∞ and 1, where a value closer to 1 indicates a higher spatial similarity between the observations and GCM simulations (Koch et al. 2018).

We ranked the GCMs at the resolution of raw GCMs (coarser resolution) and observation data (finer resolution), with the relative error in the daily precipitation and maximum and minimum temperatures.

Bias correction method

One multivariate bias correction method (two-stage quantile mapping, TSQM), which combines a single-variable bias correction method with a distribution-free shuffle approach (Guo et al. 2019), is used to correct daily precipitation and maximum and minimum temperatures in GCMs at finer resolution. The TSQM method (Guo et al. 2019) involves two steps: firstly, the daily bias correction (DBC) method (Chen et al. 2013) is used to correct biases for the three climate variables separately, and then, a distribution-free shuffle approach is used to construct the inter-variable correlations by rearranging the sequences of bias-corrected series. Also, the DBC method involves two steps: firstly, the biases in precipitation occurrence are corrected by determining the precipitation threshold for simulated precipitation amounts, and then, the biases in temperature (or wet-day precipitation amounts) between the reference simulation and observation, and the same biases are removed for the future simulation.

Performance of precipitation

SPAEF and KS between observed (cma) and GCM-simulated daily mean precipitation, maximum and minimum temperatures in China at the coarse and finer resolutions and after bias correction were estimated for the period 1961–2014. Table 2 shows the GOF values that depict the performance of each GCM in simulating cma mean daily precipitation. In Table 2, the ranks of GCMs corresponding to SPAEF and KS are shown with brackets. The GOF values near 1(0) refer to better performance of the GCM of interest in SPAEF (KS). For example, ACCESS-ESM1-5 has a GOF value of 0.979 for SPAEF and is, hence, regarded as the best GCM, whereas MIROC-ES2L can be regarded as the poorest GCM, which has a GOF value of 0.862 in terms of SPAEF. Also, CNRM-ESM2-1 is regarded as the best GCM with a GOF value close to 0, and FGOALS-g3 is the poorest one with a GOF value close to −0.002 in terms of KS at coarse resolution. The GOF values and ranks at finer resolution and that after bias correction can also be interpreted in the same manner.

Table 2

GOF values and ranks of raw, interpolated and bias-corrected GCMs for daily precipitation

Model nameRaw
Interpolated
Bias-corrected
SPAEFKSSPAEFKSSPAEFKS
BCC-CSM2-MR 0.94(14) –0.001(17) 0.613(18) 0.249(5) 0.903(16) 0.014(18) 
FGOALS-g3 0.944(10) −0.002(21) 0.571(20) 0.101(1) 0.907(11) −0.001(2) 
CanESM5 0.87(20) 0.001(19) 0.728(9) 0.351(11) 0.907(10) 0.003(7) 
CNRM-CM6-1 0.944(11) −0.001(9) 0.776(4) 0.346(10) 0.918(6) −0.002(5) 
CNRM-ESM2-1 0.952(9) 0(1) 0.762(6) 0.325(9) 0.922(2) −0.002(6) 
IPSL-CM6A-LR 0.954(8) 0.001(18) 0.661(17) 0.229(4) 0.901(19) 0.005(11) 
ACCESS-ESM1-5 0.979(1) −0.001(13) 0.748(7) 0.791(18) 0.901(18) −0.012(16) 
ACCESS-CM2 0.932(16) 0.001(15) 0.744(8) 0.517(16) 0.907(12) 0.007(13) 
EC-Earth3 0.973(5) 0.001(8) 0.779(3) 0.176(2) 0.919(4) 0.02(20) 
EC-Earth3-Veg 0.977(4) 0.001(11) 0.798(1) 0.178(3) 0.925(1) 0.001(3) 
INM-CM4-8 0.943(12) 0.001(6) 0.709(11) 0.915(21) 0.918(5) −0.008(14) 
INM-CM5-0 0.902(19) 0(2) 0.688(15) 0.882(20) 0.906(14) −0.004(8) 
MIROC6 0.955(7) 0.001(16) 0.693(14) 0.638(17) 0.903(15) −0.002(4) 
MIROC-ES2L 0.862(21) −0.001(3) 0.488(21) 0.831(19) 0.916(7) −0.013(17) 
MRI-ESM2-0 0.957(6) −0.001(10) 0.7(12) 0.252(6) 0.895(21) −0.017(19) 
HadGEM3-GC31-LL 0.93(18) 0.001(7) 0.797(2) 0.499(15) 0.9(20) 0.007(12) 
UKESM1-0-LL 0.932(17) −0.001(5) 0.767(5) 0.46(14) 0.912(8) 0(1) 
MPI-ESM1-2-HR 0.978(3) −0.001(4) 0.722(10) 0.282(7) 0.919(3) −0.005(9) 
MPI-ESM1-2-LR 0.935(15) −0.002(20) 0.578(19) 0.425(13) 0.902(17) −0.01(15) 
NorESM2-MM 0.941(13) −0.001(12) 0.665(16) 0.374(12) 0.909(9) 0.005(10) 
GFDL-ESM4 0.979(2) −0.001(14) 0.694(13) 0.313(8) 0.906(13) −0.034(21) 
Model nameRaw
Interpolated
Bias-corrected
SPAEFKSSPAEFKSSPAEFKS
BCC-CSM2-MR 0.94(14) –0.001(17) 0.613(18) 0.249(5) 0.903(16) 0.014(18) 
FGOALS-g3 0.944(10) −0.002(21) 0.571(20) 0.101(1) 0.907(11) −0.001(2) 
CanESM5 0.87(20) 0.001(19) 0.728(9) 0.351(11) 0.907(10) 0.003(7) 
CNRM-CM6-1 0.944(11) −0.001(9) 0.776(4) 0.346(10) 0.918(6) −0.002(5) 
CNRM-ESM2-1 0.952(9) 0(1) 0.762(6) 0.325(9) 0.922(2) −0.002(6) 
IPSL-CM6A-LR 0.954(8) 0.001(18) 0.661(17) 0.229(4) 0.901(19) 0.005(11) 
ACCESS-ESM1-5 0.979(1) −0.001(13) 0.748(7) 0.791(18) 0.901(18) −0.012(16) 
ACCESS-CM2 0.932(16) 0.001(15) 0.744(8) 0.517(16) 0.907(12) 0.007(13) 
EC-Earth3 0.973(5) 0.001(8) 0.779(3) 0.176(2) 0.919(4) 0.02(20) 
EC-Earth3-Veg 0.977(4) 0.001(11) 0.798(1) 0.178(3) 0.925(1) 0.001(3) 
INM-CM4-8 0.943(12) 0.001(6) 0.709(11) 0.915(21) 0.918(5) −0.008(14) 
INM-CM5-0 0.902(19) 0(2) 0.688(15) 0.882(20) 0.906(14) −0.004(8) 
MIROC6 0.955(7) 0.001(16) 0.693(14) 0.638(17) 0.903(15) −0.002(4) 
MIROC-ES2L 0.862(21) −0.001(3) 0.488(21) 0.831(19) 0.916(7) −0.013(17) 
MRI-ESM2-0 0.957(6) −0.001(10) 0.7(12) 0.252(6) 0.895(21) −0.017(19) 
HadGEM3-GC31-LL 0.93(18) 0.001(7) 0.797(2) 0.499(15) 0.9(20) 0.007(12) 
UKESM1-0-LL 0.932(17) −0.001(5) 0.767(5) 0.46(14) 0.912(8) 0(1) 
MPI-ESM1-2-HR 0.978(3) −0.001(4) 0.722(10) 0.282(7) 0.919(3) −0.005(9) 
MPI-ESM1-2-LR 0.935(15) −0.002(20) 0.578(19) 0.425(13) 0.902(17) −0.01(15) 
NorESM2-MM 0.941(13) −0.001(12) 0.665(16) 0.374(12) 0.909(9) 0.005(10) 
GFDL-ESM4 0.979(2) −0.001(14) 0.694(13) 0.313(8) 0.906(13) −0.034(21) 

Note: Numbers within brackets represent the rank of GCMs.

Table 2 shows the ranks attained by GCMs corresponding to temporal and spatial metrics for daily precipitation at coarse and finer resolutions and those after bias correction. The daily precipitation from raw GCM and that after bias correction perform better than that of interpolated GCM, the maximum SPAEF is 0.979, 0.925 and 0.798, and KS is 0, 0 and 0.101 for raw, bias-corrected and interpolated GCMs, separately. For example, BCC-CSM2-MR attained ranks 14, 18 and 16 for SPAEF but 17, 5 and 18 for KS at coarse and finer resolutions and after bias correction. MIROC-ES2L secured rank 21 for SPAEF in both coarse and finer resolutions but 7 after bias correction. The SPAEF for GCMs at coarse resolution is the largest one, and the KS for GCMs is the smallest one in the coarse resolution for daily precipitation.

Figure 2 illustrates the ranks of daily precipitation at coarse and finer resolutions and those after bias correction based on KS. The daily precipitation after bias correction shows the best in the ECDFs, while daily precipitation in the raw GCMs and that after interpolation overestimate the precipitation. Also, the boxplots also show that the mean of daily precipitation from bias-corrected GCMs shows the best performance than that from raw and interpolated GCM.

The spatial patterns of mean daily precipitation simulated by the GCMs ranked 1 and 21 were compared with the spatial pattern of cma precipitation at coarse and finer resolutions and those after bias correction and are presented in Figure 3. In Figure 3, it was seen that the GCMs that attained rank 1 (the best-performing GCM) showed spatial patterns more similar to those of cma precipitation than that attained rank 21. Figure 3 clearly shows that GCMs that attained rank 21 overestimated the precipitation over a large region at coarse and finer resolutions in the study area. The mean daily precipitation of GCMs after bias correction shows the best performance than that of raw and interpolated GCMs.
Figure 3

Spatial patterns of mean daily precipitation from 1961 to 2014 of the GCM ranked 1, ranked 21 and cma.

Figure 3

Spatial patterns of mean daily precipitation from 1961 to 2014 of the GCM ranked 1, ranked 21 and cma.

Close modal

Performance of maximum temperature

Table 3 illustrates the ranks of daily maximum temperature at coarse and finer resolutions and those after bias correction based on the temporal and spatial metrics. The GOFs are the largest for SPAEF and the smallest for KS in raw GCMs in comparison with the GCMs interpolated and that after bias correction. For instance, CNRM-ESM2-1 has a GOF value of 0.985 for SPAEF and is hence regarded as the best GCM in terms of SPAEF in raw GCMs, whereas MRI-ESM2-0 and EC-Earth3 are the best GCMs for finer resolution and that after bias correction with the GOF values of 0.463 and 0.89. On the other hand, MIROC-ES2L, HadGEM3-GC31-LL and INM-CM5-0 can be regarded as the poorest GCM, which have GOF values of 0.764, −4.146 and −0.181, respectively, in terms of SPAEF in coarse and finer resolutions and those after bias correction. The GOF values and ranks for KS can also be interpreted in the same manner. The SPAEF for GCMs at coarse resolution is the largest one for daily maximum temperature like precipitation, but the KS for GCMs interpolated but before bias correction is the smallest one for daily maximum temperature.

Table 3

GOF values and ranks of raw, interpolated and bias-corrected GCMs for daily maximum temperature

Model nameRaw
Interpolated
Bias-corrected
SPAEFKSSPAEFKSSPAEFKS
BCC-CSM2-MR 0.939(17) −0.001(4) 0.593(17) −0.217(15) 0.924(21) −0.014(20) 
FGOALS-g3 0.983(3) 0.002(16) 0.493(18) −0.173(11) 0.932(17) −0.006(9) 
CanESM5 0.935(18) 0.002(18) 0.679(14) −0.188(13) 0.947(4) 0.015(21) 
CNRM-CM6-1 0.958(14) 0.004(21) 0.347(20) −0.315(20) 0.949(3) −0.007(10) 
CNRM-ESM2-1 0.981(4) 0.001(8) 0.48(19) −0.229(17) 0.946(6) −0.001(1) 
IPSL-CM6A-LR 0.983(2) 0.001(7) 0.243(21) −0.381(21) 0.946(5) 0.001(3) 
ACCESS-ESM1-5 0.975(8) 0.001(10) 0.707(9) −0.214(14) 0.939(10) 0.002(5) 
ACCESS-CM2 0.961(12) 0.002(17) 0.689(13) −0.231(18) 0.939(11) 0.002(4) 
EC-Earth3 0.976(7) 0.001(3) 0.625(16) −0.218(16) 0.924(20) 0.003(6) 
EC-Earth3-Veg 0.98(5) 0.003(19) 0.65(15) −0.188(12) 0.93(19) −0.008(12) 
INM-CM4-8 0.914(21) 0(1) 0.718(8) −0.06(2) 0.932(18) −0.012(16) 
INM-CM5-0 0.975(11) −0.001(2) 0.728(7) −0.086(5) 0.944(7) −0.013(17) 
MIROC6 0.917(20) 0.001(6) 0.789(2) 0.036(1) 0.94(8) −0.014(19) 
MIROC-ES2L 0.959(13) 0.001(5) 0.701(10) −0.085(4) 0.94(9) −0.011(14) 
MRI-ESM2-0 0.933(19) 0.001(12) 0.695(11) −0.17(10) 0.953(2) −0.011(13) 
HadGEM3-GC31-LL 0.985(1) 0.003(20) 0.733(6) −0.141(8) 0.932(16) −0.001(2) 
UKESM1-0-LL 0.954(15) 0.001(9) 0.762(3) −0.133(7) 0.935(14) 0.005(8) 
MPI-ESM1-2-HR 0.978(6) 0.002(15) 0.793(1) −0.104(6) 0.934(15) −0.012(15) 
MPI-ESM1-2-LR 0.975(10) 0.002(13) 0.752(4) –0.147(9) 0.957(1) −0.004(7) 
NorESM2-MM 0.948(16) 0.002(14) 0.734(5) −0.083(3) 0.936(13) 0.008(11) 
GFDL-ESM4 0.975(9) 0.001(11) 0.692(12) −0.25(19) 0.936(12) −0.013(18) 
Model nameRaw
Interpolated
Bias-corrected
SPAEFKSSPAEFKSSPAEFKS
BCC-CSM2-MR 0.939(17) −0.001(4) 0.593(17) −0.217(15) 0.924(21) −0.014(20) 
FGOALS-g3 0.983(3) 0.002(16) 0.493(18) −0.173(11) 0.932(17) −0.006(9) 
CanESM5 0.935(18) 0.002(18) 0.679(14) −0.188(13) 0.947(4) 0.015(21) 
CNRM-CM6-1 0.958(14) 0.004(21) 0.347(20) −0.315(20) 0.949(3) −0.007(10) 
CNRM-ESM2-1 0.981(4) 0.001(8) 0.48(19) −0.229(17) 0.946(6) −0.001(1) 
IPSL-CM6A-LR 0.983(2) 0.001(7) 0.243(21) −0.381(21) 0.946(5) 0.001(3) 
ACCESS-ESM1-5 0.975(8) 0.001(10) 0.707(9) −0.214(14) 0.939(10) 0.002(5) 
ACCESS-CM2 0.961(12) 0.002(17) 0.689(13) −0.231(18) 0.939(11) 0.002(4) 
EC-Earth3 0.976(7) 0.001(3) 0.625(16) −0.218(16) 0.924(20) 0.003(6) 
EC-Earth3-Veg 0.98(5) 0.003(19) 0.65(15) −0.188(12) 0.93(19) −0.008(12) 
INM-CM4-8 0.914(21) 0(1) 0.718(8) −0.06(2) 0.932(18) −0.012(16) 
INM-CM5-0 0.975(11) −0.001(2) 0.728(7) −0.086(5) 0.944(7) −0.013(17) 
MIROC6 0.917(20) 0.001(6) 0.789(2) 0.036(1) 0.94(8) −0.014(19) 
MIROC-ES2L 0.959(13) 0.001(5) 0.701(10) −0.085(4) 0.94(9) −0.011(14) 
MRI-ESM2-0 0.933(19) 0.001(12) 0.695(11) −0.17(10) 0.953(2) −0.011(13) 
HadGEM3-GC31-LL 0.985(1) 0.003(20) 0.733(6) −0.141(8) 0.932(16) −0.001(2) 
UKESM1-0-LL 0.954(15) 0.001(9) 0.762(3) −0.133(7) 0.935(14) 0.005(8) 
MPI-ESM1-2-HR 0.978(6) 0.002(15) 0.793(1) −0.104(6) 0.934(15) −0.012(15) 
MPI-ESM1-2-LR 0.975(10) 0.002(13) 0.752(4) –0.147(9) 0.957(1) −0.004(7) 
NorESM2-MM 0.948(16) 0.002(14) 0.734(5) −0.083(3) 0.936(13) 0.008(11) 
GFDL-ESM4 0.975(9) 0.001(11) 0.692(12) −0.25(19) 0.936(12) −0.013(18) 

Figure 4 presents the ranks of daily maximum temperature at coarse and finer resolutions and those after bias correction based on KS. The daily maximum temperature after bias correction performs the best in the mean but poorest in the trend of the ECDFs, while it is opposite for daily maximum temperature in the raw GCMs and that after interpolation. However, the boxplots also show that the mean of daily maximum temperature from bias corrected GCMs shows the best performance than that from raw and interpolated GCMs.
Figure 4

The ECDFs and boxplots of daily maximum temperature (Txm) from cma and the GCM simulations.

Figure 4

The ECDFs and boxplots of daily maximum temperature (Txm) from cma and the GCM simulations.

Close modal
Figure 5 presents the spatial patterns of mean daily maximum temperature simulated by the GCMs ranked 1 (see Figure 5(a), 5(c) and 5(f)) and 21 (see Figure 5(b), 5(d) and 5(g)), which were compared with the spatial pattern of cma maximum temperature at coarse and finer resolutions and those after bias correction. In Figure 4, it was seen that the GCMs that attained rank 1 (left list) showed spatial patterns more similar to those of cma maximum temperature than that attained rank 21 (center list). The mean daily maximum temperature of GCMs after bias correction show the best performance than raw and interpolated GCMs.
Figure 5

Spatial patterns of mean daily maximum temperature from 1961 to 2014 of the GCM ranked 1, ranked 21 and cma.

Figure 5

Spatial patterns of mean daily maximum temperature from 1961 to 2014 of the GCM ranked 1, ranked 21 and cma.

Close modal

Performance of minimum temperature

Table 4 illustrates the ranks of daily minimum temperature at coarse and finer resolutions and those after bias correction based on the temporal and spatial metrics. The GOFs are the largest for SPAEF and the smallest for KS in raw GCMs in comparison with the GCMs interpolated and that after bias correction. For instance, CNRM-ESM2-1 has a GOF value of 0.985 for SPAEF and is hence regarded as the best GCM in terms of SPAEF in raw GCMs, whereas MRI-ESM2-0 and EC-Earth3 are the best GCMs for finer resolution and that after bias correction with the GOF value of 0.463 and 0.89. On the other hand, MIROC-ES2L, HadGEM3-GC31-LL and INM-CM5-0 can be regarded as the poorest GCM, which have GOF values of 0.764, −4.146 and −0.181 in terms of SPAEF in coarse and finer resolutions and those after bias correction, whereas BCC-CSM2-MR, ACCESS-CM2 and EC-Earth3 are the best ones and HadGEM3-GC31-LL, IPSL-CM6A-LR and INM-CM5-0 are the poorest ones for coarse and finer resolutions and that after bias correction in KS. The SPAEF for GCMs at coarse resolution is the largest one, but the KS for GCMs interpolated but before bias correction is the smallest one for daily minimum temperature like daily maximum temperature.

Table 4

GOF values and ranks of raw, interpolated and bias-corrected GCMs for daily minimum temperature

Model nameRaw
Interpolated
Bias-corrected
SPAEFKSSPAEFKSSPAEFKS
BCC-CSM2-MR 0.97(10) 0.003(1) −0.702(17) −2.425(11) 0.106(18) −0.467(18) 
FGOALS-g3 0.98(3) −0.016(14) −0.827(18) −2.209(10) 0.57(10) −0.292(10) 
CanESM5 0.974(7) −0.01(8) −0.298(12) −4.864(20) 0.777(4) 0.256(8) 
CNRM-CM6-1 0.967(11) −0.012(10) −0.304(13) −4.862(19) 0.5(12) −0.329(13) 
CNRM-ESM2-1 0.985(1) −0.01(6) −0.465(14) −3.417(17) 0.548(11) −0.305(11) 
IPSL-CM6A-LR 0.983(2) −0.005(4) −0.264(11) −5.85(21) 0.794(3) −0.157(3) 
ACCESS-ESM1-5 0.972(8) −0.024(16) 0.12(10) 3.041(15) 0.676(6) −0.231(5) 
ACCESS-CM2 0.962(15) 0.033(20) 0.43(2) 0.542(1) 0.662(7) −0.242(6) 
EC-Earth3 0.961(16) −0.011(9) −0.526(15) −2.914(14) 0.89(1) −0.073(1) 
EC-Earth3-Veg 0.964(13) −0.031(19) −0.685(16) −2.472(12) 0.5(13) −0.324(12) 
INM-CM4-8 0.974(6) 0.003(2) 0.289(4) 1.448(5) −0.001(20) −0.498(20) 
INM-CM5-0 0.963(14) −0.012(11) 0.422(3) 0.697(2) −0.181(21) −0.538(21) 
MIROC6 0.95(18) 0.008(5) 0.178(8) 3.401(16) 0.259(15) −0.417(15) 
MIROC-ES2L 0.764(21) 0.005(3) 0.138(9) 3.497(18) 0.191(17) −0.442(17) 
MRI-ESM2-0 0.966(12) 0.02(15) 0.463(1) 0.881(4) 0.453(14) −0.35(14) 
HadGEM3-GC31-LL 0.828(19) −0.146(21) −4.146(21) −0.848(3) 0.659(8) −0.244(7) 
UKESM1-0-LL 0.952(17) −0.027(18) −1.455(20) −1.649(6) 0.689(5) −0.226(4) 
MPI-ESM1-2-HR 0.976(5) 0.012(12) 0.276(5) 1.984(9) 0.226(16) −0.431(16) 
MPI-ESM1-2-LR 0.787(20) 0.014(13) 0.232(6) 1.899(7) 0.628(9) –0.265(9) 
NorESM2-MM 0.979(4) 0.01(7) 0.202(7) 2.63(13) 0.838(2) −0.124(2) 
GFDL-ESM4 0.972(9) −0.024(17) −0.955(19) −1.973(8) 0.057(19) −0.479(19) 
Model nameRaw
Interpolated
Bias-corrected
SPAEFKSSPAEFKSSPAEFKS
BCC-CSM2-MR 0.97(10) 0.003(1) −0.702(17) −2.425(11) 0.106(18) −0.467(18) 
FGOALS-g3 0.98(3) −0.016(14) −0.827(18) −2.209(10) 0.57(10) −0.292(10) 
CanESM5 0.974(7) −0.01(8) −0.298(12) −4.864(20) 0.777(4) 0.256(8) 
CNRM-CM6-1 0.967(11) −0.012(10) −0.304(13) −4.862(19) 0.5(12) −0.329(13) 
CNRM-ESM2-1 0.985(1) −0.01(6) −0.465(14) −3.417(17) 0.548(11) −0.305(11) 
IPSL-CM6A-LR 0.983(2) −0.005(4) −0.264(11) −5.85(21) 0.794(3) −0.157(3) 
ACCESS-ESM1-5 0.972(8) −0.024(16) 0.12(10) 3.041(15) 0.676(6) −0.231(5) 
ACCESS-CM2 0.962(15) 0.033(20) 0.43(2) 0.542(1) 0.662(7) −0.242(6) 
EC-Earth3 0.961(16) −0.011(9) −0.526(15) −2.914(14) 0.89(1) −0.073(1) 
EC-Earth3-Veg 0.964(13) −0.031(19) −0.685(16) −2.472(12) 0.5(13) −0.324(12) 
INM-CM4-8 0.974(6) 0.003(2) 0.289(4) 1.448(5) −0.001(20) −0.498(20) 
INM-CM5-0 0.963(14) −0.012(11) 0.422(3) 0.697(2) −0.181(21) −0.538(21) 
MIROC6 0.95(18) 0.008(5) 0.178(8) 3.401(16) 0.259(15) −0.417(15) 
MIROC-ES2L 0.764(21) 0.005(3) 0.138(9) 3.497(18) 0.191(17) −0.442(17) 
MRI-ESM2-0 0.966(12) 0.02(15) 0.463(1) 0.881(4) 0.453(14) −0.35(14) 
HadGEM3-GC31-LL 0.828(19) −0.146(21) −4.146(21) −0.848(3) 0.659(8) −0.244(7) 
UKESM1-0-LL 0.952(17) −0.027(18) −1.455(20) −1.649(6) 0.689(5) −0.226(4) 
MPI-ESM1-2-HR 0.976(5) 0.012(12) 0.276(5) 1.984(9) 0.226(16) −0.431(16) 
MPI-ESM1-2-LR 0.787(20) 0.014(13) 0.232(6) 1.899(7) 0.628(9) –0.265(9) 
NorESM2-MM 0.979(4) 0.01(7) 0.202(7) 2.63(13) 0.838(2) −0.124(2) 
GFDL-ESM4 0.972(9) −0.024(17) −0.955(19) −1.973(8) 0.057(19) −0.479(19) 

Figure 6 illustrates the ranks of daily minimum temperature at coarse and finer resolutions and those after bias correction based on KS. The daily minimum temperature at coarse and finer resolutions and those after bias correction shows similar to that of daily maximum temperature. Also, the boxplots also show that the mean of daily minimum temperature from bias-corrected GCMs shows the best performance than that from raw and interpolated GCMs.
Figure 6

The ECDFs and boxplots of daily minimum temperature from cma and the GCM simulations.

Figure 6

The ECDFs and boxplots of daily minimum temperature from cma and the GCM simulations.

Close modal
The spatial patterns of the mean daily minimum temperature simulated by the GCMs ranked 1 and 21 were compared with the spatial pattern of cma precipitation at coarse and finer resolutions and those after bias correction and are presented in Figure 7. Figure 7 clearly shows that GCMs after bias correction at finer resolution have higher similarity to the cma daily minimum temperature like precipitation and maximum temperature in Figures 3 and 5. Spatial patterns of the mean daily minimum temperature of bias-corrected GCMs are most similar to those of the observations, no matter the GCM ranked 1 or 21, like that for daily precipitation and daily maximum temperature.
Figure 7

Spatial patterns of mean daily minimum temperature from 1961 to 2014 of the GCM ranked 1, ranked 21 and cma.

Figure 7

Spatial patterns of mean daily minimum temperature from 1961 to 2014 of the GCM ranked 1, ranked 21 and cma.

Close modal

This study not only studied the spatio-temporal performance of climatic variables after interpolation and bias correction but also compared the performance of climate variables of raw GCM, so as to illustrate the impact of reprocessing. It assessed the temporal and spatial accuracy of 21 CMIP6 GCMs in simulating daily precipitation, minimum and maximum temperature at coarse and finer resolutions and those after bias correction over China for the period 1961–2014. The GOF of KS is calculated for the temporal assessment metric, and SPAEF is used for the metric assessment metric. Ahmed et al. (2019) and Abbasian et al. (2019) have evaluated the precipitation and temperature from annual and seasonal scales after interpolation, but researchers seldom studied the performance in daily scale and compared the performance before and after interpolation. This work is important for hydro-climate research for their input is daily scale. The following conclusions were drawn from this study:

  • The GOF of SPAEF in raw resolution shows the greatest at coarser resolution, which mean that daily precipitation, minimum and maximum temperature in raw GCMs have the highest similarity to those in re-gridded observational cma, especially in the spatial pattern. The inverse distance weighted interpolation may decrease the accuracy spatial aspects for all the three variables and temporal in precipitation but not for daily maximum and minimum temperatures.

  • Almost all the GCMs overestimate the daily precipitation at both coarse and finer resolutions, but closer at finer resolution after bias correction. The performance of GCMs in daily minimum and maximum temperatures shows better than that in daily precipitation, where GCMs show a difference in temporal and spatial assessment metrics. It is of great importance to select the GCM before application with different situations.

  • The GCMs after bias correction at finer resolution have the best similarity to the observation in spatial patterns but the poorest similarity in the trend of ECDFs in daily minimum and maximum temperatures. EC-Earth3-Veg (UKESM1-0-LL), EC-Earth3 (EC-Earth3) and MPI-ESM1-2-LR (CNRM-ESM2-1) is the best GCM in SPAEF (KS) at finer resolution after bias correction.

Furthermore, the process of inverse distance weighted interpolation will bring more uncertainty to variables from GCMs, especially in spatial aspects. Also, the TSQM method performs well in representing spatio-temporal precipitation and spatial temperature, but poorly in temporal temperature.

This work was partially supported by the National Natural Science Foundation of China (Grant No. 52109007), the Natural Science Foundation of Chongqing, China (Grant No. cstc2021jcyj-msxm2426) and the Scientific and Technological Research Program of Chongqing Municipal Education Commission (Grant No. KJQN2021007).

Y.L. conceived the original idea, designed the methodology, collected the data, performed the simulations, contributed to the interpretation of the results, and wrote and revised the paper. P.P. reviewed and edited the paper. W.J. reviewed and edited the paper.

All relevant data are included in the paper or its Supplementary Information.

The authors declare that there is no conflict.

Abbasian
M.
,
Moghim
S.
&
Abrishamchi
A.
2019
Performance of the general circulation models in simulating temperature and precipitation over Iran
.
Theoretical and Applied Climatology
135
(
3–4
),
1465
1483
.
https://doi.org/10.1007/s00704-018-2456-y
.
Adib
M. N. M.
&
Harun
S.
2022
Metalearning approach coupled with CMIP6 Multi-GCM for future monthly streamflow forecasting
.
Journal of Hydrologic Engineering
27
(
6
),
1
16
.
https://doi.org/10.1061/(asce)he.1943-5584.0002176
.
Ahmed
K.
,
Sachindra
D. A.
,
Shahid
S.
,
Demirel
M. C.
&
Chung
E. S.
2019
Selection of multi-model ensemble of general circulation models for the simulation of precipitation and maximum and minimum temperature based on spatial assessment metrics
.
Hydrology and Earth System Sciences
23
(
11
),
4803
4824
.
https://doi.org/10.5194/hess-23-4803-2019
.
Chen
J.
,
Brissette
F. P.
,
Chaumont
D.
&
Braun
M.
2013
Performance and uncertainty evaluation of empirical downscaling methods in quantifying the climate change impacts on hydrology over two North American river basins
.
Journal of Hydrology
479
,
200
214
.
https://doi.org/10.1016/j.jhydrol.2012.11.062
.
Cook
B. I.
,
Mankin
J. S.
,
Marvel
K.
,
Williams
A. P.
,
Smerdon
J. E.
&
Anchukaitis
K. J.
2020
Twenty-first century drought projections in the CMIP6 forcing scenarios
.
Earth's Future
8
(
6
),
1
20
.
https://doi.org/10.1029/2019EF001461
.
Cui
T.
,
Li
C.
&
Tian
F.
2021
Evaluation of temperature and precipitation simulations in CMIP6 models over the Tibetan plateau
.
Earth and Space Science
8
(
7
),
1
20
.
https://doi.org/10.1029/2020EA001620
.
Demirel
M. C.
,
Mai
J.
,
Mendiguren
G.
,
Koch
J.
,
Samaniego
L.
&
Stisen
S.
2018
Combining satellite data and appropriate objective functions for improved spatial pattern performance of a distributed hydrologic model
.
Hydrology and Earth System Sciences
22
(
2
),
1299
1315
.
https://doi.org/10.5194/hess-22-1299-2018
.
Eyring
V.
,
Bony
S.
,
Meehl
G. A.
,
Senior
C. A.
,
Stevens
B.
,
Stouffer
R. J.
&
Taylor
K. E.
2016
Overview of the Coupled Model Intercomparison Project Phase 6 (CMIP6) experimental design and organization
.
Geoscientific Model Development
9
(
5
),
1937
1958
.
https://doi.org/10.5194/gmd-9-1937-2016
.
Fischer
E. M.
,
Sedláček
J.
,
Hawkins
E.
&
Knutti
R.
2014
Models agree on forced response pattern of precipitation and temperature extremes
.
Geophysical Research Letters
41
(
23
).
https://doi.org/10.1002/2014GL062018.
Giorgi
F.
&
Mearns
L. O.
2003
Probability of regional climate change based on the Reliability Ensemble Averaging (REA) method
.
Geophysical Research Letters
30
(
12
).
https://doi.org/10.1029/2003GL017130.
Gu
L.
,
Chen
J.
,
Yin
J.
,
Sullivan
S. C.
,
Wang
H. M.
,
Guo
S.
,
Zhang
L.
&
Kim
J. S.
2020
Projected increases in magnitude and socioeconomic exposure of global droughts in 1.5 and 2°C warmer climates
.
Hydrology and Earth System Sciences
24
(
1
),
451
472
.
https://doi.org/10.5194/hess-24-451-2020
.
Guo
Q.
,
Chen
J.
,
Zhang
X.
,
Shen
M.
,
Chen
H.
&
Guo
S.
2019
A new two-stage multivariate quantile mapping method for bias correcting climate model outputs
.
Climate Dynamics
53
(
5–6
),
3603
3623
.
https://doi.org/10.1007/s00382-019-04729-w
.
Hirabayashi
Y.
,
Tanoue
M.
,
Sasaki
O.
,
Zhou
X.
&
Yamazaki
D.
2021
Global exposure to flooding from the new CMIP6 climate model projections
.
Scientific Reports
11
(
1
),
1
8
.
https://doi.org/10.1038/s41598-021-83279-w
.
Ji
Z.
&
Kang
S.
2015
Evaluation of extreme climate events using a regional climate model for China
.
International Journal of Climatology
35
(
6
).
https://doi.org/10.1002/joc.4024.
Jiang
Z.
,
Li
W.
,
Xu
J.
&
Li
L.
2015
Extreme precipitation indices over China in CMIP5 models. Part I: Model evaluation
.
Journal of Climate
28
(
21
),
8603
8619
.
https://doi.org/10.1175/JCLI-D-15-0099.1
.
Kharin
V. V.
,
Flato
G. M.
,
Zhang
X.
,
Gillett
N. P.
,
Zwiers
F.
&
Anderson
K. J.
2018
Risks from climate extremes change differently from 1.5°C to 2.0°C depending on rarity
.
Earth's Future
6
(
5
).
https://doi.org/10.1002/2018EF000813.
Knutti
R.
,
Masson
D.
&
Gettelman
A.
2013
Climate model genealogy: Generation CMIP5 and how we got there
.
Geophysical Research Letters
40
(
6
),
1194
1199
.
https://doi.org/10.1002/grl.50256
.
Koch
J.
,
Demirel
M. C.
&
Stisen
S.
2018
The SPAtial EFficiency metric (SPAEF): Multiple-component evaluation of spatial patterns for optimization of hydrological models
.
Geoscientific Model Development
11
(
5
),
1873
1886
.
https://doi.org/10.5194/gmd-11-1873-2018
.
Lorenz
R.
,
Stalhandske
Z.
&
Fischer
E. M.
2019
Detection of a climate change signal in extreme heat, heat stress, and cold in Europe from observations
.
Geophysical Research Letters
46
(
14
).
https://doi.org/10.1029/2019GL082062.
Massey
F. J.
1951
The Kolmogorov-Smirnov test for goodness of fit
.
Journal of the American Statistical Association
46
(
253
).
https://doi.org/10.1080/01621459.1951.10500769.
Masson-Delmotte
V.
,
Zhai
P.
,
Pörtner
H.-O.
,
Roberts
D.
,
Skea
J.
,
Shukla
P. R.
,
Pirani
A.
,
Moufouma-Okia
W.
,
Péan
C.
,
Pidcock
R.
,
Connors
S.
,
Matthews
J. B. R.
,
Chen
Y.
,
Zhou
X.
,
Gomis
M. I.
,
Lonnoy
E.
,
Maycock
T.
,
Tignor
M.
&
Waterfield
T.
(eds.)
2018
Special report 1.5 – Summary for policymakers. In: An IPCC Special Report on the impacts of global warming of 1.5 oC above pre-industrial levels
.
Murphy
J. M.
,
Sexton
D. M. H.
,
Barnett
D. N.
,
Jones
G. S.
,
Webb
M. J.
,
Collins
M.
&
Stainforth
D. A.
2004
Quantification of modelling uncertainties in a large ensemble of climate change simulations
.
Nature
430
(
August 2004
),
768
772
.
https://doi.org/10.1038/nature02770.1
.
Ngoma
H.
,
Wen
W.
,
Ayugi
B.
,
Babaousmail
H.
&
Karim
R.
2020
Evaluation of the global climate models in CMIP6 over Uganda Hamida
.
https://doi.org/10.20944/preprints202012.0782.v1.
Ojha
R.
,
Kumar
D. N.
,
Sharma
A.
&
Mehrotra
R.
2014
Assessing GCM convergence for India using the variable convergence score
.
Journal of Hydrologic Engineering
19
(
6
),
1237
1246
.
https://doi.org/10.1061/(asce)he.1943-5584.0000888
.
Perkins
S. E.
,
Pitman
A. J.
,
Holbrook
N. J.
&
McAneney
J.
2007
Evaluation of the AR4 climate models’ simulated daily maximum temperature, minimum temperature, and precipitation over Australia using probability density functions
.
Journal of Climate
20
(
17
),
4356
4376
.
https://doi.org/10.1175/JCLI4253.1
.
Salman
S. A.
,
Shahid
S.
,
Ismail
T.
,
Ahmed
K.
&
Wang
X. J.
2018
Selection of climate models for projection of spatiotemporal changes in temperature of Iraq with uncertainties
.
Atmospheric Research
213
(
July
),
509
522
.
https://doi.org/10.1016/j.atmosres.2018.07.008
.
Sansom
P. G.
,
Stephenson
D. B.
,
Ferro
C. A. T.
,
Zappa
G.
&
Shaffrey
L.
2013
Simple uncertainty frameworks for selecting weighting schemes and interpreting multimodel ensemble climate change experiments
.
Journal of Climate
26
(
12
),
4017
4037
.
https://doi.org/10.1175/JCLI-D-12-00462.1
.
Shepard
D.
1968
A two-dimensional interpolation function for irregularly-spaced data
. In:
Proceedings of the 1968 23rd ACM National Conference, ACM 1968
.
https://doi.org/10.1145/800186.810616.
Shukla
J.
,
DelSole
T.
,
Fennessy
M.
,
Kinter
J.
&
Paolino
D.
2006
Climate model fidelity and projections of climate change
.
Geophysical Research Letters
33
(
7
).
https://doi.org/10.1029/2005GL025579.
Srinivasa Raju
K.
,
Sonali
P.
&
Nagesh Kumar
D.
2017
Ranking of CMIP5-based global climate models for India using compromise programming
.
Theoretical and Applied Climatology
128
(
3–4
),
563
574
.
https://doi.org/10.1007/s00704-015-1721-6
.
Terando
A.
,
Keller
K.
&
Easterling
W. E.
2012
Probabilistic projections of agro-climate indices in North America
.
Journal of Geophysical Research Atmospheres
117
(
8
).
https://doi.org/10.1029/2012JD017436.
Wan
Y.
,
Chen
J.
,
Xu
C. Y.
,
Xie
P.
,
Qi
W.
,
Li
D.
&
Zhang
S.
2021
Performance dependence of multi-model combination methods on hydrological model calibration strategy and ensemble size
.
Journal of Hydrology
603
(
PC
),
127065
.
https://doi.org/10.1016/j.jhydrol.2021.127065
.
Wheeler
T.
&
Von Braun
J.
2013
Climate change impacts on global food security
.
Science
341
(
6145
).
https://doi.org/10.1126/science.1239402.
Xu
Z.
,
Han
Y.
,
Tam
C.-Y.
,
Yang
Z.-L.
&
Fu
C.
2021
Bias-corrected CMIP6 global dataset for dynamical downscaling of the historical and future climate (1979–2100)
.
Scientific Data
8
(
1
),
1
11
.
https://doi.org/10.1038/s41597-021-01079-3
.
Xuan
W.
,
Ma
C.
,
Kang
L.
,
Gu
H.
,
Pan
S.
&
Xu
Y. P.
2017
Evaluating historical simulations of CMIP5 GCMs for key climatic variables in Zhejiang Province, China
.
Theoretical and Applied Climatology
128
(
1–2
),
207
222
.
https://doi.org/10.1007/s00704-015-1704-7
.
Yang
X.
,
Zhou
B.
,
Xu
Y.
&
Han
Z.
2021
CMIP6 evaluation and projection of temperature and precipitation over China
.
Advances in Atmospheric Sciences
38
(
5
),
817
830
.
https://doi.org/10.1007/s00376-021-0351-4
.
Yin
J.
,
Guo
S.
,
Gu
L.
,
Zeng
Z.
,
Liu
D.
,
Chen
J.
,
Shen
Y.
&
Xu
C. Y.
2021
Blending multi-satellite, atmospheric reanalysis and gauge precipitation products to facilitate hydrological modelling
.
Journal of Hydrology
593
(
December 2020
),
125878
.
https://doi.org/10.1016/j.jhydrol.2020.125878
.
Zhang
Q.
,
Xiao
M.
,
Singh
V. P.
,
Liu
L.
&
Xu
C. Y.
2015
Observational evidence of summer precipitation deficit-temperature coupling in China
.
Journal of Geophysical Research
120
(
19
).
https://doi.org/10.1002/2015JD023830.
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