{"data":{"id":"10.6084/m9.figshare.3126946.v4","type":"dois","attributes":{"doi":"10.6084/m9.figshare.3126946.v4","prefix":"10.6084","suffix":"m9.figshare.3126946.v4","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Flender, Samuel","nameType":"Personal","givenName":"Samuel","familyName":"Flender","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"Full-sky SZ maps and cluster catalog"}],"publisher":"figshare","container":{},"publicationYear":2016,"subjects":[{"subject":"Cosmology"},{"subject":"Astrophysics"},{"subject":"20103 Cosmology and Extragalactic Astronomy","subjectScheme":"FOR"},{"subject":"FOS: Physical sciences","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"FOS: Physical sciences","subjectScheme":"Fields of Science and Technology (FOS)"}],"contributors":[],"dates":[{"date":"2016-03-31","dateType":"Created"},{"date":"2016-03-31","dateType":"Updated"},{"date":"2016","dateType":"Issued"}],"language":null,"types":{"ris":"DATA","bibtex":"misc","citeproc":"dataset","schemaOrg":"Dataset","resourceType":"Dataset","resourceTypeGeneral":"Dataset"},"relatedIdentifiers":[{"relationType":"IsPreviousVersionOf","relatedIdentifier":"10.6084/m9.figshare.3126946","relatedIdentifierType":"DOI"}],"relatedItems":[],"sizes":["16848443520 Bytes"],"formats":[],"version":null,"rightsList":[{"rights":"Creative Commons Zero v1.0 Universal","rightsUri":"https://creativecommons.org/publicdomain/zero/1.0/legalcode","schemeUri":"https://spdx.org/licenses/","rightsIdentifier":"cc0-1.0","rightsIdentifierScheme":"SPDX"}],"descriptions":[{"description":"This page contains full-sky maps of the kinematic and thermal Sunyaev-Zel'dovich signal. The different models are described in detail in our paper (Flender et al 2015, arXiv:1511.02843). We make the following data products available:\u003cbr\u003eksz_mod1_R13.fits - kSZ map, Model Iksz_mod2_R13.fits - kSZ map, Model IIksz_mod3_R13.fits - kSZ map, Model IIItsz150_R13.fits - tSZ map at 150Ghzcatalog_fullsky_zsm1.fits - full-sky halo catalog\u003cbr\u003eAll maps are provided in the form of full-sky Healpix maps in ring-ordering with nside=8192. The units in all maps are mikro-Kelvin, relative to the average CMB temperature. The halo catalog contains all halos identified with a friends-of-friends halo finder with more than 1000 particles. The catalog is in fits format with the following fits keys (all float, except HALO_ID, which is a long int):\u003cbr\u003eRA - right ascension in degreesDEC - declination in degreesM200RED - M200c (defined with respect to the critical density) in units of Msun/hM200 - M200c in units of MsunM500RED - M500c in units of Msun/h (translated from M200RED, using the cM-relation from Bhattacharya et al. (2013))M500 - M500c in units of MsunREDSHIFT - redshift of the haloHALO_ID - identification number of the haloVLOS - comoving peculiar line-of-sight velocity of the halo, in km/sC200 - concentration assigned to the halo based on M200c, following the cM-relation from Bhattacharya et al. (2013)\u003cbr\u003e---The Simulation---Our maps were generated from a simulation carried out with HACC (Habib et al. 2016). In this simulation, 3200\u003csup\u003e3\u003c/sup\u003e particles were evolved in a (2.1Gpc)\u003csup\u003e3\u003c/sup\u003e volume, leading to a mass resolution of ~10\u003csup\u003e10\u003c/sup\u003eMsun. The cosmology used is close to the best-fit WMAP-7 parameters. The simulation is part of a large suite of simulations, the so-called Titan-Mira Universe suite. More results from this simulation, including power spectra, mass functions, and concentration-mass relation measurements can be found in Heitmann et al. (2015).\u003cbr\u003e---Publications---If you use our maps and catalogs, please cite our paper:Simulations of the Pairwise Kinematic Sunyaev-Zeldovich SignalS. Flender, L. Bleem, H. Finkel, S. Habib, K. Heitmann, G. Holder, arXiv:1511.02843This research used resources of the ALCF, which is supported by DOE/SC under contract DE-AC02-06CH11357 and resources of the National Energy Research Scientific Computing Center, a DOE Office of Science User Facility supported by the Office of Science of the U.S. Department of Energy under Contract No. DE-AC02-05CH11231.\u003cbr\u003e---More Information---For more information, please contact me via email: samuel dot flender at googlemail.com","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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