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The CDS-CMIP6 subset consists of the following CMIP6 experiments:

Experiment name

Extended Description

historical

The historical experiment is a simulation of the recent past from 1850 to 2014, it is performed with a coupled atmosphere-ocean general circulation model (AOGCM). In the historical simulations the model is forced with changing conditions (consistent with observations) which include atmospheric composition, land use and solar forcing. The initial conditions for the historical simulation are taken from the pre-industrial control simulation (piControl) at a point where the remaining length of the piControl is sufficient to extend beyond the period of the historical simulation to the end of any future "scenario" simulations run by the same model. The historical simulation is used to evaluate model performance against present climate and observed climate change.

ssp585

ssp585 is a scenario experiment extending into the near future from 2015 to 2100, it is performed with a coupled atmosphere-ocean general circulation model (AOGCM). The forcing for the CMIP6 SSP experiments is derived from shared socioeconomic pathways (SSPs), a set of emission scenarios driven by different socioeconomic assumptions, paired with representative concentration pathways (RCPs), global forcing pathways which lead to specific end of century radiative forcing targets. ssp585 is based on SSP5 in which climate change mitigation challenges dominate and RCP8.5, a future pathway with a radiative forcing of 8.5 W/m2 in the year 2100. The ssp585 scenario represents the high end of plausible future forcing pathways.  ssp585 is comparable to the CMIP5 experiment RCP8.5.

ssp370

ssp370 is a scenario experiment extending into the near future from 2015 to 2100, it is performed with a coupled atmosphere-ocean general circulation model (AOGCM). The forcing for the CMIP6 SSP experiments is derived from shared socioeconomic pathways (SSPs), a set of emission scenarios driven by different socioeconomic assumptions, paired with representative concentration pathways (RCPs), global forcing pathways which lead to specific end of century radiative forcing targets. ssp370 is based on SSP3 in which climate change mitigation and adaptation challenges are high and RCP7.0, a future pathway with a radiative forcing of 7.0 W/m2 in the year 2100. The ssp370 scenario represents the medium to high end of plausible future forcing pathways. ssp370 fills a gap in the CMIP5 forcing pathways that is particularly important because it represents a forcing level common to several (unmitigated) SSP baseline pathways.

ssp245

ssp245 is a scenario experiment extending into the near future from 2015 to 2100, it is performed with a coupled atmosphere-ocean general circulation model (AOGCM). The forcing for the CMIP6 SSP experiments is derived from shared socioeconomic pathways (SSPs), a set of emission scenarios driven by different socioeconomic assumptions, paired with representative concentration pathways (RCPs), global forcing pathways which lead to specific end of century radiative forcing targets. ssp245 is based on SSP2 with intermediate climate change mitigation and adaptation challenges and RCP4.5, a future pathway with a radiative forcing of 4.5 W/m2 in the year 2100. The ssp245 scenario represents the medium part of plausible future forcing pathways. ssp245 is comparable to the CMIP5 experiment RCP4.5.

ssp126

ssp126 is a scenario experiment extending into the near future from 2015 to 2100, it is performed with a coupled atmosphere-ocean general circulation model (AOGCM). The forcing for the CMIP6 SSP experiments is derived from shared socioeconomic pathways (SSPs), a set of emission scenarios driven by different socioeconomic assumptions, paired with representative concentration pathways (RCPs), global forcing pathways which lead to specific end of century radiative forcing targets. ssp126 is based on SSP1 with low climate change mitigation and adaptation challenges and RCP2.6, a future pathway with a radiative forcing of 2.6 W/m2 in the year 2100. The ssp126 scenario represents the low end of plausible future forcing pathways. ssp126 depicts a "best case" future from a sustainability perspective.

ssp460

ssp460 is a scenario experiment extending into the near future from 2015 to 2100, it is performed with a coupled atmosphere-ocean general circulation model (AOGCM). The forcing for the CMIP6 SSP experiments is derived from shared socioeconomic pathways (SSPs), a set of emission scenarios driven by different socioeconomic assumptions, paired with representative concentration pathways (RCPs), global forcing pathways which lead to specific end of century radiative forcing targets. ssp460 is based on SSP4 in which climate change adaptation challenges dominate and RCP6.0, a future pathway with a radiative forcing of 6.0 W/m2 in the year 2100. The ssp460 scenario fills in the range of medium plausible future forcing pathways. ssp370 defines the low end of the forcing range for unmitigated SSP baseline scenarios.

ssp434

ssp434 is a scenario experiment extending into the near future from 2015 to 2100, it is performed with a coupled atmosphere-ocean general circulation model (AOGCM). The forcing for the CMIP6 SSP experiments is derived from shared socioeconomic pathways (SSPs), a set of emission scenarios driven by different socioeconomic assumptions, paired with representative concentration pathways (RCPs), global forcing pathways which lead to specific end of century radiative forcing targets. ssp434 is based on SSP4 in which climate change adaptation challenges dominate and RCP3.4, a future pathway with a radiative forcing of 3.4 W/m2 in the year 2100. The ssp434 scenario fills a gap at the low end of the range of plausible future forcing pathways. ssp370 is of interest to mitigation policy since mitigation costs differ substantially between forcing levels of 4.5 W/m2 and 2.6 W/m2.

ssp534-over

ssp534-over is a scenario experiment with simulations beginning in the mid-21st century running from 2040 to 2100, it is performed with a coupled atmosphere-ocean general circulation model (AOGCM). The forcing for the CMIP6 SSP experiments is derived from shared socioeconomic pathways (SSPs), a set of emission scenarios driven by different socioeconomic assumptions, paired with representative concentration pathways (RCPs), global forcing pathways which lead to specific end of century radiative forcing targets. ssp534-over is based on SSP5 in which climate change mitigation challenges dominate and RCP3.4-over, a future pathway with a peak and decline in forcing towards an eventual radiative forcing of 3.4 W/m2 in the year 2100. The ssp534-over scenario branches from ssp585 in the year 2040 whereupon it applies substantially negative net emissions. ssp534-over explores the climate science and policy implications of a peak and decline in forcing during the 21st century. ssp534 fills a gap in existing climate simulations by investigating the implications of a substantial overshoot in radiative forcing relative to a longer-term target.

ssp119

ssp119 is a scenario experiment extending into the near future from 2015 to 2100, it is performed with a coupled atmosphere-ocean general circulation model (AOGCM). The forcing for the CMIP6 SSP experiments is derived from shared socioeconomic pathways (SSPs), a set of emission scenarios driven by different socioeconomic assumptions, paired with representative concentration pathways (RCPs), global forcing pathways which lead to specific end of century radiative forcing targets. ssp119 is based on SSP1 with low climate change mitigation and adaptation challenges and RCP1.9, a future pathway with a radiative forcing of 1.9 W/m2 in the year 2100. The ssp119 scenario fills a gap at the very low end of the range of plausible future forcing pathways. ssp119 forcing will be substantially below ssp126 in 2100. There is policy interest in low-forcing scenarios that would inform a possible goal of limiting global mean warming to 1.5°C above pre-industrial levels based on the Paris COP21 agreement[1].

[1] The Paris Agreement https://unfccc.int/process-and-meetings/the-paris-agreement/the-paris-agreement

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The models included in the CDS-CMIP5 CMIP6 subset are detailed in the table below , these include most of the models from the main CMIP5 archive. However a small number of models were not included as the data from the models have a research-only restriction on their use, all data in the CDS are released without restriction, therefore, the MIROC and MRI models from Japan are not included. The following table contains a list of the global climate models in use in the CDS and a including a brief description of the model where this information is readily available, further details can be found on the Earth System Documentation site.

Model Name

Modelling Centre


ACCESS-CM2

CSIRO-ARCCSS (Commonwealth Scientific and Industrial Research Organisation, Aspendale, Victoria 3195, Australia, Australian Research Council Centre of Excellence for Climate System Science)

Australian Community Climate and Earth System Simulator Climate Model Version 2





ACCESS1-0
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titleClick here to expand...Global climate models included in the CDS


Model

name

Name

Modelling

centre

Centre


ACCESS-CM2

Model details

CSIRO-ARCCSS (Commonwealth Scientific and Industrial Research Organisation, Aspendale, Victoria 3195, Australia

), and BOM (Bureau of Meteorology, Australia)

ACCESS1-0 2011. Atmosphere: AGCM v1.0 (N96 grid-point, 1.875 degrees EW x approx 1.25 degree NS, 38 levels); ocean: NOAA/GFDL MOM4p1 (nominal 1.0 degree EW x 1.0 degrees NS, tripolar north of 65N, equatorial refinement to 1/3 degree from 10S to 10 N, cosine dependent NS south of 25S, 50 levels); sea ice: CICE4.1 (nominal 1.0 degree EW x 1.0 degrees NS, tripolar north of 65N, equatorial refinement to 1/3 degree from 10S to 10 N, cosine dependent NS south of 25S); land: MOSES2 (1.875 degree EW x 1.25 degree NS, 4 levels;

ACCESS1.3

CSIRO (Commonwealth Scientific and Industrial Research Organisation, Australia), and BOM (Bureau of Meteorology, Australia)

ACCESS1-3 2011. Atmosphere: AGCM v1.0 (N96 grid-point, 1.875 degrees EW x approx 1.25 degree NS, 38 levels); ocean: NOAA/GFDL MOM4p1 (nominal 1.0 degree EW x 1.0 degrees NS, tripolar north of 65N, equatorial refinement to 1/3 degree from 10S to 10 N, cosine dependent NS south of 25S, 50 levels); sea ice: CICE4.1 (nominal 1.0 degree EW x 1.0 degrees NS, tripolar north of 65N, equatorial refinement to 1/3 degree from 10S to 10 N, cosine dependent NS south of 25S); land: CABLE1.0 (1.875 degree EW x 1.25 degree NS, 6 levels;

bcc-csm1-1

Beijing Climate Center(BCC),China Meteorological Administration,China

bcc-csm1-1:atmosphere: BCC_AGCM2.1 (T42L26); land: BCC_AVIM1.0;ocean: MOM4_L40 (tripolar, 1 lon x (1-1/3) lat, L40);sea ice: SIS (tripolar,1 lon x (1-1/3) lat);

bcc-csm1-1-m

Beijing Climate Center(BCC),China Meteorological Administration,China

bcc-csm1-1-m:atmosphere: BCC_AGCM2.2 (T106L26); land: BCC_AVIM1.1;ocean: MOM4_L40v2 (tripolar, 1 lon x (1-1/3) lat, L40);sea ice: SIS (tripolar,1 lon x (1-1/3) lat);

BNU-ESM

GCESS,BNU,Beijing,China

BNU-ESM;

CanAM4

CCCma (Canadian Centre for Climate Modelling and Analysis, Victoria, BC, Canada)

CanAM4 2010 atmosphere: CanAM4 (AGCM15i, T63L35) land: CLASS2.7 (Note: Adjusted Land Cover and soil albedo relative to that used in CanESM2 and CanCM4);

CanCM4

CCCma (Canadian Centre for Climate Modelling and Analysis, Victoria, BC, Canada)

CanCM4 2010 atmosphere: CanAM4 (AGCM15i, T63L35) ocean: CanOM4 (OGCM4.0, 256x192L40) sea ice: CanSIM1 (Cavitating Fluid, T63 Gaussian Grid) land: CLASS2.7;

CanESM2

CCCma (Canadian Centre for Climate Modelling and Analysis, Victoria, BC, Canada)

CanESM2 2010 atmosphere: CanAM4 (AGCM15i, T63L35) ocean: CanOM4 (OGCM4.0, 256x192L40) and CMOC1.2 sea ice: CanSIM1 (Cavitating Fluid, T63 Gaussian Grid) land: CLASS2.7 and CTEM1;

CCSM4

NCAR (National Center for Atmospheric Research) Boulder, CO, USA

CCSM4 (repository tag: ccsm4_0_beta49 compset: BRCP26CN);

CESM1-BGC

NSF/DOE NCAR (National Center for Atmospheric Research) Boulder, CO, USA

CESM1-BGC;

CESM1-CAM5

NSF/DOE NCAR (National Center for Atmospheric Research) Boulder, CO, USA

CESM1-CAM5;

CESM1-FASTCHEM

NSF/DOE NCAR (National Center for Atmospheric Research) Boulder, CO, USA

CESM1-FASTCHEM;

CESM1-WACCM

NSF/DOE NCAR (National Center for Atmospheric Research) Boulder, CO, USA

CESM1-WACCM;

CMCC-CESM

CMCC - Centro Euro-Mediterraneo per i Cambiamenti Climatici, Bologna, Italy

CMCC-CESM;

CMCC-CM

CMCC - Centro Euro-Mediterraneo per i Cambiamenti

CMCC-CM;

CMCC-CMS

CMCC - Centro Euro-Mediterraneo per i Cambiamenti Climatici, Bologna, Italy

CMCC-CMS;

CNRM-CM5

CNRM (Centre National de Recherches Meteorologiques, Meteo-France, Toulouse,France) and CERFACS (Centre Europeen de Recherches et de Formation Avancee en Calcul Scientifique, Toulouse, France)

CNRM-CM5 2010 Atmosphere: ARPEGE-Climat (V5.2.1, TL127L31); Ocean: NEMO (nemo3.3.v10.6.6P, ORCA1degL42); Sea Ice: GELATO (V5.30); River Routing: TRIP (v1); Land: SURFEX (v5.1.c); Coupler : OASIS 3;

CNRM-CM5-2

CNRM (Centre National de Recherches Meteorologiques, Meteo-France, Toulouse, France) and CERFACS (Centre Europeen de Recherches et de Formation Avancee en Calcul Scientifique, Toulouse, France)

CNRM-CM5-2 2010 Atmosphere: ARPEGE-Climat (V5.2.3i, TL127L31); Ocean: NEMO (nemo3.2.v11.3, ORCA1degL42); Sea Ice: GELATO (V5.47f); River Routing: TRIP (v1); Land: SURFEX (v5.1.c); Coupler : OASIS 3;

CSIRO-Mk3-6-0

Australian Commonwealth Scientific and Industrial Research Organization (CSIRO) Marine and Atmospheric Research (Melbourne, Australia) in collaboration with the Queensland Climate Change Centre of Excellence (QCCCE) (Brisbane, Australia)

CSIRO-Mk3-6-0 2010 atmosphere: AGCM v7.3.8 (T63 spectral, 1.875 degrees EW x approx. 1.875 degrees NS, 18 levels); ocean: GFDL MOM2.2 (1.875 degrees EW x approx. 0.9375 degrees NS, 31 levels);

EC-EARTH

EC-EARTH (European Earth System Model)

EC-EARTH 2.3 (2011); atmosphere: IFS (cy31R1+modifications, T159L62); ocean: NEMO (version2+modifications, ORCA1-42lev); sea ice: LIM2; land: HTessel;

FGOALS_g2

IAP (Institute of Atmospheric Physics, Chinese Academy of Sciences, Beijing, China) and THU (Tsinghua University)

FGOALS_g2 2011 atmosphere: GAMIL (gamil2, 128x60L26); ocean: LICOM (licom2, 360x196L30); ice: CICE (cice4_lasg, 360x196L4); land: CLM (clm3, 128x60);

FGOALS-s2; IAP(Institute of Atmospheric Physics),CAS(Chinese Academy of Sciences),Beijing,China

FGOALS-s2 SAMIL 2-4-7

FIO-ESM

FIO(The First Institution of Oceanography,SOA,Qingdao,China)

FIO-ESM

GFDL-CM2p1

NOAA GFDL(201 Forrestal Rd, Princeton, NJ, 08540)

GFDL-CM2p1 2010 ocean: MOM4 (MOM4p1_x1_Z50_cCM2M,Tripolar360x200L50); atmosphere: AM2 (AM2p14,M45L24); sea ice: SIS (SISp2,Tripolar360x200L50); land: LM2 (LM2,M45);

GFDL-CM3

NOAA GFDL(201 Forrestal Rd, Princeton, NJ, 08540)

GFDL-CM3 2010 atmosphere: AM3 (AM3p9,C48L48); sea ice: SIS (SISp2,Tripolar360x200); land: LM3 (LM3p7_cCM3,C48); ocean: MOM4 (MOM4p1_x1_Z50_cCM3,Tripolar360x200L50);

GFDL-ESM2G

NOAA GFDL(201 Forrestal Rd, Princeton, NJ, 08540)

GFDL-ESM2G 2010 ocean: TOPAZ (TOPAZ1p2,Tripolar360x210L63); atmosphere: AM2 (AM2p14,M45L24); sea ice: SIS (SISp2,Tripolar360x210L63); land: LM3 (LM3p7_cESM,M45);

GFDL-ESM2M

NOAA GFDL(201 Forrestal Rd, Princeton, NJ, 08540)

GFDL-ESM2M 2010 ocean: MOM4 (MOM4p1_x1_Z50_cCM2M,Tripolar360x200L50); atmosphere: AM2 (AM2p14,M45L24); sea ice: SIS (SISp2,Tripolar360x200L50); land: LM3 (LM3p7_cESM,M45) Computing resources were provided by the Climate Simulation Laboratory at the NCAR Computational and Information Systems Laboratory (CISL),\n,;

GFDL-HIRAM-C180

NOAA GFDL(201 Forrestal Rd, Princeton, NJ, 08540)

GFDL-HIRAM-C180 2010 atmosphere: HIRAM (HIRAMp1,C180L32); land: LM3 (LM3p7_cHIRAM,C180);

GFDL-HIRAM-C360

NOAA GFDL(201 Forrestal Rd, Princeton, NJ, 08540)

GFDL-HIRAM-C360 2010 atmosphere: HIRAM (HIRAMp1,C360L32); land: LM3 (LM3p7_cHIRAM,C360);

GISS-E2-H

NASA/GISS (Goddard Institute for Space Studies) New York, NY

GISS-E2-H-Eh135f9b Atmosphere: GISS-E2; Ocean: H;

GISS-E2-H-CC

NASA/GISS (Goddard Institute for Space Studies) New York, NY

GISS-E2-H-CC-E4arobio_h8P Atmosphere: GISS-E2; Ocean: H;

GISS-E2-R

NASA/GISS (Goddard Institute for Space Studies) New York, NY

GISS-E2-R-E135OCNf9aF40 Atmosphere: GISS-E2;

GISS-E2-R-CC

NASA/GISS (Goddard Institute for Space Studies) New York, NY

GISS-E2-R-CC-E4arobio_g8RCP45 Atmosphere: GISS-E2; Ocean: R;

HadCM3

Met Office Hadley Centre, Fitzroy Road, Exeter, Devon, EX1 3PB, UK, (http://www.metoffice.gov.uk)

HadCM3 - Hadley Centre Coupled Model Version 3 (2000) atmosphere: HadAM3 (N48L19); ocean: HadOM (lat: 1.25 lon: 1.25 L20); land-surface/vegetation: MOSES1;;

HadGEM2-A

Met Office Hadley Centre, Fitzroy Road, Exeter, Devon, EX1 3PB, UK, (http://www.metoffice.gov.uk)

HadGEM2-A (2009) atmosphere: HadGAM2 (N96L38); land-surface/vegetation: MOSES2;

HadGEM2-CC

Met Office Hadley Centre, Fitzroy Road, Exeter, Devon, EX1 3PB, UK, (http://www.metoffice.gov.uk)

HadGEM2-CC (2011) atmosphere: HadGAM2(N96L60); ocean: HadGOM2 (lat: 1.0-0.3 lon: 1.0 L40); land-surface/vegetation: MOSES2 and TRIFFID; ocean biogeochemistry: diat-HadOCC;

HadGEM2-ES

Met Office Hadley Centre, Fitzroy Road, Exeter, Devon, EX1 3PB, UK, (http://www.metoffice.gov.uk)

HadGEM2-ES (2009) atmosphere: HadGAM2 (N96L38); ocean: HadGOM2 (lat: 1.0-0.3 lon: 1.0 L40); land-surface/vegetation: MOSES2 and TRIFFID; tropospheric chemistry: UKCA; ocean biogeochemistry: diat-HadOCC;

inmcm4

INM (Institute for Numerical Mathematics, Moscow, Russia)

inmcm4 (2009);

IPSL-CM5A-LR

IPSL (Institut Pierre Simon Laplace, Paris, France)

IPSL-CM5A-LR (2010) : atmos : LMDZ4 (LMDZ4_v5, 96x95x39); ocean : ORCA2 (NEMOV2_3, 2x2L31); seaIce : LIM2 (NEMOV2_3); ocnBgchem : PISCES (NEMOV2_3); land : ORCHIDEE (orchidee_1_9_4_AR5);

IPSL-CM5A-MR

IPSL (Institut Pierre Simon Laplace, Paris, France)

IPSL-CM5A-MR (2010) : atmos : LMDZ4 (LMDZ4_v5, 144x143x39); ocean : ORCA2 (NEMOV2_3, 2x2L31); seaIce : LIM2 (NEMOV2_3); ocnBgchem : PISCES (NEMOV2_3); land : ORCHIDEE (orchidee_1_9_4_AR5);

IPSL-CM5B-LR

IPSL (Institut Pierre Simon Laplace, Paris, France)

IPSL-CM5B-LR (2011) : atmos : LMDZ5 (LMDZ5_NPv3.1, 96x95x39); ocean : ORCA2 (NEMOV2_3, 2x2L31); seaIce : LIM2 (NEMOV2_3); ocnBgchem : PISCES (NEMOV2_3); land : ORCHIDEE (orchidee_1_9_4_AR5);

MPI-ESM-LR

Max Planck Institute for Meteorology

MPI-ESM-LR 2011; URL: https://www.mpimet.mpg.de/en/science/models/mpi-esm/; atmosphere: ECHAM6 (REV: 4418), T63L47; land: JSBACH (REV: 4418);;

MPI-ESM-MR

Max Planck Institute for Meteorology

MPI-ESM-MR 2011; URL: https://www.mpimet.mpg.de/en/science/models/mpi-esm/; atmosphere: ECHAM6 (REV: 4968), T63L47; land: JSBACH (REV: 4968);;

MPI-ESM-P

Max Planck Institute for Meteorology

MPI-ESM-P 2011; URL: https://www.mpimet.mpg.de/en/science/models/mpi-esm/; atmosphere: ECHAM6 (REV: 5051), T63L47; land: JSBACH (REV: 5051); ocean: MPIOM (REV: 5051), GR15L40; sea ice: 5051; marine bgc: HAMOCC (REV: 5051);;

NorESM1-M

Norwegian Climate Centre

NorESM1-M 2011 atmosphere: CAM-Oslo (CAM4-Oslo-noresm-ver1_cmip5-r112, f19L26); ocean: MICOM (MICOM-noresm-ver1_cmip5-r112, gx1v6L53); sea ice: CICE (CICE4-noresm-ver1_cmip5-r112); land: CLM (CLM4-noresm-ver1_cmip5-r112);

NorESM1-ME

Norwegian Climate Centre

NorESM1-ME 2011 atmosphere: CAM-Oslo (CAM4-Oslo-noresm-ver1_cmip5-r139, f19L26); ocean: MICOM (MICOM-noresm-ver1_cmip5-r139, gx1v6L53); ocean biogeochemistry: HAMOCC (HAMOCC-noresm-ver1_cmip5-r139, gx1v6L53); sea ice: CICE (CICE4-noresm-ver1_cmip5-r139); land: CLM (CLM4-noresm-ver1_cmip5-r139);

, Australian Research Council Centre of Excellence for Climate System Science)

Australian Community Climate and Earth System Simulator Climate Model Version 2


Pressure levels

For pressure level data the model output is available on the pressure levels according to the table below. Note that not all models provide the same pressure levels. 

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