J/MNRAS/427/1666    Massive galaxies in CANDELS-UDS field    (Bruce+, 2012)

The morphologies of massive galaxies at 1 < z < 3 in the CANDELS-UDS field: compact bulges, and the rise and fall of massive discs. Bruce V.A., Dunlop J.S., Cirasuolo M., McLure R.J., Targett T.A., Bell E.F., Croton D.J., Dekel A., Faber S.M., Ferguson H.C., Grogin N.A., Kocevski D.D., Koekemoer A.M., Koo D.C., Lai K., Lotz J.M., McGrath E.J., Newman J.A., van der Wel A. <Mon. Not. R. Astron. Soc., 427, 1666-1701 (2012)> =2012MNRAS.427.1666B 2012MNRAS.427.1666B
ADC_Keywords: Galaxy catalogs ; Morphology Keywords: galaxies: elliptical and lenticular, cD - galaxies: evolution - galaxies: high-redshift - galaxies: spiral - galaxies: structure Abstract: We have used high-resolution, Hubble Space Telescope, near-infrared imaging to conduct a detailed analysis of the morphological properties of the most massive galaxies at high redshift, modelling the WFC3/IR H160-band images of the ≃200 galaxies in the CANDELS-UDS field with photometric redshifts 1<z<3, and stellar masses M*>1011M. We have explored the results of fitting single-Sersic and bulge+disc models, and have investigated the additional errors and potential biases introduced by uncertainties in the background and the on-image point spread function. Description: The main aim of this paper is to present a comprehensive and robust analysis of the morphological properties of a significant sample of the most massive galaxies in the redshift range 1<z<3. In order to achieve this we have focused our study on the UKIDSS Ultra Deep Survey (UDS; Lawrence et al. 2007, Cat. II/314), the central region of which has been imaged with HST WFC3/IR as part of the CANDELS multicycle treasury programme (Grogin et al. 2011ApJS..197...35G 2011ApJS..197...35G; Koekemoer et al. 2011ApJS..197...36K 2011ApJS..197...36K). In addition to the near-infrared imaging provided by HST, the data sets we make use of for sample selection (i.e. photometric redshifts, stellar mass determination, SFRs and star formation histories) include: deep optical imaging in the B-, V-, R-, i'- and z'-band filters from the Subaru XMM-Newton Deep Survey (SXDS; Sekiguchi et al. 2005, in Renzini A., Bender R., eds, Multiwavelength Mapping of Galaxy Formation and Evolution. Springer, Berlin, p. 82; Furusawa et al. 2008, Cat. J/ApJS/176/301); U-band imaging obtained with MegaCam on Canada-France-Hawaii Telescope; J-, H- and K-band United Kingdom Infrared Telescope (UKIRT) WFCAM imaging from Data Release 8 (DR8) of the UKIDSS UDS; and Spitzer 3.6-, 4.5-, 5.8- and 8.0-um IRAC and 24-um MIPS imaging from the SpUDS legacy programme (PI Dunlop). File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file tables1.dat 113 215 Physical properties and best-fitting parameters -------------------------------------------------------------------------------- See also: II/314 : UKIDSS-DR8 LAS, GCS and DXS Surveys (Lawrence+ 2012) J/ApJS/176/301 : Subaru/XMM-Newton deep survey IV. (SXDS) (Ouchi+, 2008) Byte-by-byte Description of file: tables1.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 6 I6 --- ID [100222/123457] Galaxy identification number 8- 9 I2 h RAh Right ascension (J2000) 11- 12 I2 min RAm Right ascension (J2000) 14- 18 F5.2 s RAs Right ascension (J2000) 20 A1 --- DE- Declination sign (J2000) 21- 22 I2 deg DEd Declination (J2000) 24- 25 I2 arcmin DEm Declination (J2000) 27- 30 F4.1 arcsec DEs Declination (J2000) 32- 35 F4.2 10+11Msun M* Stellar mass (1) 37- 40 F4.2 --- zph [1/3] Photometric redshift (2) 42- 46 F5.2 mag Hmag HST/WFC3 IR H160 total magnitude (3) 48- 51 F4.1 --- n [0/20] Single Sersic index (4) 53- 56 F4.1 kpc re Single Sersic effective radius (4) 58- 61 F4.2 --- b/a [0/1] Single Sersic axial ratio (4) 63- 66 F4.2 --- PSFn [0/1] Single Sersic PSF fraction (4) 68 I1 --- F [0/1] unacceptable single component model (4) 70- 72 F3.1 --- Mod [0/4] Model type (0.0, 1.0 or 4.0; not explained in the paper) 74- 77 F4.1 kpc reB ?=- Bulge effective radius 79- 82 F4.2 --- b/aB ?=- Bulge axial ratio 84- 87 F4.1 kpc reD ?=- Disc effective radius 89- 92 F4.2 --- b/aD [0/1]? Disc axial ratio 94- 97 F4.2 --- Bulge [0/1] Bulge fraction 99-102 F4.2 --- Disc [0/1] Disc fraction 104-107 F4.2 --- PSF [0/1] PSF fraction 109 I1 --- F0 [0/1] Flag original 111 I1 --- F1 [0/1] Flag first refinement 113 I1 --- F2 [0/1] Flag final refinement -------------------------------------------------------------------------------- Note (1): Errors on photometric redshifts are of the order of δz/(1+zsp)=0.05, from Cirasuolo et al. (in preparation). Note (2): We quote errors on our stellar mass estimates of a factor of 2 (Michalowski et al., 2012A&A...541A..85M 2012A&A...541A..85M), where these are driven by uncertainties in the photometry from the IRAC bands and from photometric redshifts. Note (3): We estimate errors on our total magnitudes of order ±0.05mag, as our sample of galaxies are at the extreme bright end (>10σ) so their errors are limited to uncertainties in photometric zero-points. Note (4): Obtaining individual uncertainties for all the parameters of multiple-component fits listed here is impractical as the degree of systematic and correlated errors varies on an object-by-object basis. However, from the detailed parameter space search conducted for our single-Sersic models, we determined errors of the order of 10% for effective radii and 5% for Sersic indices, with errors being somewhat smaller for better constrained parameters such as axial ratios. Therefore, we estimate that the multiple-component errors will be a factor of sqrt(2) larger, giving errors on fitted parameters up to 15%. However, we note that in the case of weak secondary components the errors can potentially be much larger, but as our science plots use only parameters from significant components the errors should be similar to those of the single component models. -------------------------------------------------------------------------------- History: From electronic version of the journal
(End) Patricia Vannier [CDS] 09-Aug-2013
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