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@comment{{Command line: /usr/bin/bib2bib --quiet -c 'not journal:"Discussions"' -c 'not journal:"Polymer Science"' -c '  author:"Codron"  ' -c year=2013 -c $type="ARTICLE" -oc lmd_Codron2013.txt -ob lmd_Codron2013.bib /home/WWW/LMD/public/Publis_LMDEMC3.link.bib}}  @article{2013ClDy...40.2123D, author = {{Dufresne}, J.-L. and {Foujols}, M.-A. and {Denvil}, S. and {Caubel}, A. and {Marti}, O. and {Aumont}, O. and {Balkanski}, Y. and {Bekki}, S. and {Bellenger}, H. and {Benshila}, R. and {Bony}, S. and {Bopp}, L. and {Braconnot}, P. and {Brockmann}, P. and {Cadule}, P. and {Cheruy}, F. and {Codron}, F. and {Cozic}, A. and {Cugnet}, D. and {de Noblet}, N. and {Duvel}, J.-P. and {Ethé}, C. and {Fairhead}, L. and {Fichefet}, T. and {Flavoni}, S. and {Friedlingstein}, P. and {Grandpeix}, J.-Y. and {Guez}, L. and {Guilyardi}, E. and {Hauglustaine}, D. and {Hourdin}, F. and {Idelkadi}, A. and {Ghattas}, J. and {Joussaume}, S. and {Kageyama}, M. and {Krinner}, G. and {Labetoulle}, S. and {Lahellec}, A. and {Lefebvre}, M.-P. and {Lefevre}, F. and {Levy}, C. and {Li}, Z.~X. and {Lloyd}, J. and {Lott}, F. and {Madec}, G. and {Mancip}, M. and {Marchand}, M. and {Masson}, S. and {Meurdesoif}, Y. and {Mignot}, J. and {Musat}, I. and {Parouty}, S. and {Polcher}, J. and {Rio}, C. and {Schulz}, M. and {Swingedouw}, D. and {Szopa}, S. and {Talandier}, C. and {Terray}, P. and {Viovy}, N. and {Vuichard}, N.}, title = {{Climate change projections using the IPSL-CM5 Earth System Model: from CMIP3 to CMIP5}}, journal = {Climate Dynamics}, keywords = {Climate, Climate change, Climate projections, Earth System Model, CMIP5, CMIP3, Greenhouse gases, Aerosols, Carbon cycle, Allowable emissions, RCP scenarios, Land use changes}, year = 2013, month = may, volume = 40, pages = {2123-2165}, abstract = {{We present the global general circulation model IPSL-CM5 developed to study the long-term response of the climate system to natural and anthropogenic forcings as part of the 5th Phase of the Coupled Model Intercomparison Project (CMIP5). This model includes an interactive carbon cycle, a representation of tropospheric and stratospheric chemistry, and a comprehensive representation of aerosols. As it represents the principal dynamical, physical, and bio-geochemical processes relevant to the climate system, it may be referred to as an Earth System Model. However, the IPSL-CM5 model may be used in a multitude of configurations associated with different boundary conditions and with a range of complexities in terms of processes and interactions. This paper presents an overview of the different model components and explains how they were coupled and used to simulate historical climate changes over the past 150 years and different scenarios of future climate change. A single version of the IPSL-CM5 model (IPSL-CM5A-LR) was used to provide climate projections associated with different socio-economic scenarios, including the different Representative Concentration Pathways considered by CMIP5 and several scenarios from the Special Report on Emission Scenarios considered by CMIP3. Results suggest that the magnitude of global warming projections primarily depends on the socio-economic scenario considered, that there is potential for an aggressive mitigation policy to limit global warming to about two degrees, and that the behavior of some components of the climate system such as the Arctic sea ice and the Atlantic Meridional Overturning Circulation may change drastically by the end of the twenty-first century in the case of a no climate policy scenario. Although the magnitude of regional temperature and precipitation changes depends fairly linearly on the magnitude of the projected global warming (and thus on the scenario considered), the geographical pattern of these changes is strikingly similar for the different scenarios. The representation of atmospheric physical processes in the model is shown to strongly influence the simulated climate variability and both the magnitude and pattern of the projected climate changes. }}, doi = {10.1007/s00382-012-1636-1}, adsurl = {http://adsabs.harvard.edu/abs/2013ClDy...40.2123D}, adsnote = {Provided by the SAO/NASA Astrophysics Data System} }  @article{2013ClDy...40.2167H, author = {{Hourdin}, F. and {Foujols}, M.-A. and {Codron}, F. and {Guemas}, V. and {Dufresne}, J.-L. and {Bony}, S. and {Denvil}, S. and {Guez}, L. and {Lott}, F. and {Ghattas}, J. and {Braconnot}, P. and {Marti}, O. and {Meurdesoif}, Y. and {Bopp}, L.}, title = {{Impact of the LMDZ atmospheric grid configuration on the climate and sensitivity of the IPSL-CM5A coupled model}}, journal = {Climate Dynamics}, keywords = {Climate modeling, Grid resolution, Climate change projections}, year = 2013, month = may, volume = 40, pages = {2167-2192}, abstract = {{The IPSL-CM5A climate model was used to perform a large number of control, historical and climate change simulations in the frame of CMIP5. The refined horizontal and vertical grid of the atmospheric component, LMDZ, constitutes a major difference compared to the previous IPSL-CM4 version used for CMIP3. From imposed-SST (Sea Surface Temperature) and coupled numerical experiments, we systematically analyze the impact of the horizontal and vertical grid resolution on the simulated climate. The refinement of the horizontal grid results in a systematic reduction of major biases in the mean tropospheric structures and SST. The mid-latitude jets, located too close to the equator with the coarsest grids, move poleward. This robust feature, is accompanied by a drying at mid-latitudes and a reduction of cold biases in mid-latitudes relative to the equator. The model was also extended to the stratosphere by increasing the number of layers on the vertical from 19 to 39 (15 in the stratosphere) and adding relevant parameterizations. The 39-layer version captures the dominant modes of the stratospheric variability and exhibits stratospheric sudden warmings. Changing either the vertical or horizontal resolution modifies the global energy balance in imposed-SST simulations by typically several W/m$^{2}$which translates in the coupled atmosphere-ocean simulations into a different global-mean SST. The sensitivity is of about 1.2 K per 1 W/m$^{2}$when varying the horizontal grid. A re-tuning of model parameters was thus required to restore this energy balance in the imposed-SST simulations and reduce the biases in the simulated mean surface temperature and, to some extent, latitudinal SST variations in the coupled experiments for the modern climate. The tuning hardly compensates, however, for robust biases of the coupled model. Despite the wide range of grid configurations explored and their significant impact on the present-day climate, the climate sensitivity remains essentially unchanged. }}, doi = {10.1007/s00382-012-1411-3}, adsurl = {http://adsabs.harvard.edu/abs/2013ClDy...40.2167H}, adsnote = {Provided by the SAO/NASA Astrophysics Data System} }  @article{2013JGRD..11810414C, author = {{Charnay}, B. and {Forget}, F. and {Wordsworth}, R. and {Leconte}, J. and {Millour}, E. and {Codron}, F. and {Spiga}, A.}, title = {{Exploring the faint young Sun problem and the possible climates of the Archean Earth with a 3-D GCM}}, journal = {Journal of Geophysical Research (Atmospheres)}, archiveprefix = {arXiv}, eprint = {1310.4286}, primaryclass = {astro-ph.EP}, keywords = {early Earth, Archean, paleo-climates}, year = 2013, month = sep, volume = 118, number = d17, pages = {10414}, abstract = {{Different solutions have been proposed to solve the ''faint young Sun problem,'' defined by the fact that the Earth was not fully frozen during the Archean despite the fainter Sun. Most previous studies were performed with simple 1-D radiative convective models and did not account well for the clouds and ice-albedo feedback or the atmospheric and oceanic transport of energy. We apply a global climate model (GCM) to test the different solutions to the faint young Sun problem. We explore the effect of greenhouse gases (CO$_{2}$and CH$_{4}$), atmospheric pressure, cloud droplet size, land distribution, and Earth's rotation rate. We show that neglecting organic haze, 100 mbar of CO$_{2}$with 2 mbar of CH$_{4}$at 3.8 Ga and 10 mbar of CO$_{2}$with 2 mbar of CH$_{4}$at 2.5 Ga allow a temperate climate (mean surface temperature between 10{\deg}C and 20{\deg}C). Such amounts of greenhouse gases remain consistent with the geological data. Removing continents produces a warming lower than +4{\deg}C. The effect of rotation rate is even more limited. Larger droplets (radii of 17 {$\mu$}m versus 12 {$\mu$}m) and a doubling of the atmospheric pressure produce a similar warming of around +7{\deg}C. In our model, ice-free water belts can be maintained up to 25{\deg}N/S with less than 1 mbar of CO$_{2}$and no methane. An interesting cloud feedback appears above cold oceans, stopping the glaciation. Such a resistance against full glaciation tends to strongly mitigate the faint young Sun problem. }}, doi = {10.1002/jgrd.50808}, adsurl = {http://adsabs.harvard.edu/abs/2013JGRD..11810414C}, adsnote = {Provided by the SAO/NASA Astrophysics Data System} }  @article{2013ClDy...40.2293C, author = {{Cattiaux}, J. and {Quesada}, B. and {Arakélian}, A. and {Codron}, F. and {Vautard}, R. and {Yiou}, P.}, title = {{North-Atlantic dynamics and European temperature extremes in the IPSL model: sensitivity to atmospheric resolution}}, journal = {Climate Dynamics}, keywords = {Global climate model, Atmospheric resolution, Mid-latitudes jet stream, Weather regimes, European temperature extremes}, year = 2013, month = may, volume = 40, pages = {2293-2310}, abstract = {{The variability of the European climate is mostly controlled by the unstable nature of the North-Atlantic dynamics, especially in wintertime. The intra-seasonal to inter-annual fluctuations of atmospheric circulations has often been described as the alternation between a limited number of preferential weather regimes. Such discrete description can be justified by the multi-modality of the latitudinal position of the jet stream. In addition, seasonal extremes in European temperatures are generally associated with an exceptional persistence into one weather regime. Here we investigate the skill of the IPSL model to both simulate North-Atlantic weather regimes and European temperature extremes, including summer heat waves and winter cold spells. We use a set of eight IPSL experiments, with six different horizontal resolutions and the two versions used in CMIP3 and CMIP5. We find that despite a substantial deficit in the simulated poleward peak of the jet stream, the IPSL model represents weather regimes fairly well. A significant improvement is found for all horizontal resolutions higher than the one used in CMIP3, while the increase in vertical resolution included in the CMIP5 version tends to improve the wintertime dynamics. In addition to a recurrent cold bias over Europe, the IPSL model generally overestimates (underestimates) the indices of winter cold spells (summer heat waves) such as frequencies or durations. We find that the increase in horizontal resolution almost always improves these statistics, while the influence of vertical resolution is less clear. Overall, the CMIP5 version of the IPSL model appears to carry promising improvements in the simulation of the European climate variability. }}, doi = {10.1007/s00382-012-1529-3}, adsurl = {http://adsabs.harvard.edu/abs/2013ClDy...40.2293C}, adsnote = {Provided by the SAO/NASA Astrophysics Data System} }  @article{2013CliPa...9..517C, author = {{Chavaillaz}, Y. and {Codron}, F. and {Kageyama}, M.}, title = {{Southern westerlies in LGM and future (RCP4.5) climates}}, journal = {Climate of the Past}, year = 2013, month = mar, volume = 9, pages = {517-524}, abstract = {{Mid-latitude westerlies are a major component of the atmospheric circulation and understanding their behaviour under climate change is important for understanding changes in precipitation, storms and atmosphere-ocean momentum, heat and CO$_{2}$exchanges. The Southern Hemisphere westerlies have been particularly studied in terms of the latter aspects, since the Southern Ocean is a key region for the global oceanic circulation as well as for CO$_{2}\$ uptake. In this
study, we analyse, mainly in terms of jet stream position, the behaviour
of the southern westerlies for the Last Glacial Maximum (LGM, 21 000 yr
ago, which is the last past cold extreme) and for a future climate,
obtained after stabilisation of the RCP4.5 scenario. The a priori guess
would be that the behaviour of the westerly jet stream would be similar
when examining its changes from LGM to pre-industrial (PI) conditions
and from PI to RCP4.5, i.e. in both cases a poleward shift in response
to global warming. We show that this is in fact not the case, due to the
impact of altitude changes of the Antarctic ice sheet and/or to sea ice
cover changes.
}},
doi = {10.5194/cp-9-517-2013},
adsnote = {Provided by the SAO/NASA Astrophysics Data System}
}

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