J/MNRAS/456/1195    KMOS AGN Survey at High redshift (KASHz) (Harrison+, 2016)

The KMOS AGN Survey at High redshift (KASHz): the prevalence and drivers of ionized outflows in the host galaxies of X-ray AGN. Harrison C.M., Alexander D.M., Mullaney J.R., Stott J.P., Swinbank A.M., Arumugam V., Bauer F.E., Bower R.G., Bunker A.J., Sharples R.M. <Mon. Not. R. Astron. Soc., 456, 1195-1220 (2016)> =2016MNRAS.456.1195H 2016MNRAS.456.1195H (SIMBAD/NED BibCode)
ADC_Keywords: Active gal. nuclei ; Redshifts Keywords: galaxies: active - galaxies: evolution - galaxies: kinematics and dynamics - quasars: emission lines Abstract: We present the first results from the KMOS (K-band Multi-Object Spectrograph) AGN (active galactic nuclei) Survey at High redshift (KASHz), a VLT/KMOS integral-field spectroscopic (IFS) survey of z≳0.6 AGN. We present galaxy-integrated spectra of 89 X-ray AGN (L2-10keV= 1042-1045erg/s), for which we observed [OIII] (z∼1.1-1.7) or Hα emission (z∼0.6-1.1). The targets have X-ray luminosities representative of the parent AGN population and we explore the emission-line luminosities as a function of X-ray luminosity. For the [OIII] targets, ∼50 per cent have ionized gas velocities indicative of gas that is dominated by outflows and/or highly turbulent material (i.e. overall line widths ≳600km/s). The most luminous half (i.e. LX>6x1043erg/s) have a≳2 times higher incidence of such velocities. On the basis of our results, we find no evidence that X-ray obscured AGN are more likely to host extreme kinematics than unobscured AGN. Our KASHzsample has a distribution of gas velocities that is consistent with a luminosity-matched sample of z<0.4 AGN. This implies little evolution in the prevalence of ionized outflows, for a fixed AGN luminosity, despite an order-of-magnitude decrease in average star formation rates over this redshift range. Furthermore, we compare our Hα targets to a redshift-matched sample of star-forming galaxies and despite a similar distribution of Hα luminosities and likely star formation rates, we find extreme ionized gas velocities are up to ∼10 times more prevalent in the AGN-host galaxies. Our results reveal a high prevalence of extreme ionized gas velocities in high-luminosity X-ray AGN and imply that the most powerful ionized outflows in high-redshift galaxies are driven by AGN activity. Description: KASHz is designed to ultimately obtain spatially resolved emission-line kinematics of ~(100-200) high-redshift (z∼0.6-3.6) AGN. For our target selection we make use of deep X-ray surveys performed in extragalactic fields (COSMOS, see Scoville et al., 2007, Cat. J/ApJS/171/1; CDF-S, see Giacconi et al. 2001ApJ...551..624G 2001ApJ...551..624G and Xue et al., 2011, Cat. J/ApJS/195/10 (CDFS); UDS, SXDS: see Furusawa et al. 2008, Cat. J/ApJS/176/1 (UDS) and SSA22, see Steidel et al. 1998ApJ...492..428S 1998ApJ...492..428S). File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file tablea1.dat 120 89 Properties for the KASHz targets observed so far -------------------------------------------------------------------------------- See also: J/ApJS/176/1 : Subaru/XMM-Newton deep survey (SXDS). II. (Furusawa+, 2008) J/ApJS/195/10 : The CDF-S survey: 4Ms source catalogs (Xue+, 2011) J/ApJS/171/1 : Census of QSOs Narrow Absorption Lines (Misawa+, 2007) J/ApJS/184/158 : Chandra COSMOS survey I. (Elvis+, 2009) J/ApJS/201/30 : Chandra COSMOS survey. III. (Civano+, 2012) J/A+A/497/635 : XMM-Newton wide-field survey in COSMOS field (Cappelluti+ 2009) J/ApJ/716/348 : XMM-Newton survey of the COSMOS field (Brusa+, 2010) Byte-by-byte Description of file: tablea1.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 9 A9 --- Name Source name (Field-X-ray ID) (1) 10 A1 --- n_Name [*] Note on Name (2) 12- 16 F5.3 --- zA Archival redshift 18 A1 --- n_zA [spi] Archival redshift type (3) 20 A1 --- l_F0.5-2 Limit flag on F0.5-2 21- 25 F5.2 10-18W/m2 F0.5-2 Soft-band (0.5-2keV) X-ray flux 27- 31 F5.2 10-18W/m2 F2-10 Hard-band (2-10keV) X-ray flux 32 A1 --- n_F2-10 [+] Note on F2-10 (4) 34 A1 --- Obs [UO?] obscured/unobscured candidate flag (5) 36 A1 --- RL [xv?] radio luminous flag (6) 38 A1 --- Inst [KS] Instrument used for the observations (K = KMOS and S = SINFONI) 40 A1 --- Line [OH] Primary targeted emission line (7) 42- 45 F4.1 ks texp On-source exposure time 47 A1 --- Note [CLN] Note on data (8) 49- 53 A5 --- BLR [alpha beta -] Note for the identification of a BLR component (alpha for Hα and beta for Hβ) 55- 59 F5.3 --- zl ?=- Redshift derived from the narrowest Gaussian component of the emission-line profile fit 61 A1 --- l_SA Limit flag on SA 62- 65 F4.1 10-20W/m2 SA ?=- Flux of the narrower Gaussian component 67- 69 F3.1 10-20W/m2 e_SA ? rms uncertainty on SA (10) 71- 73 I3 km/s FWA ?=- FWHM of the narrower Gaussian component 75- 77 I3 km/s e_FWA ? rms uncertainty on FWA (10) 79- 83 F5.1 10-20W/m2 SB ?=- Flux of the broader Gaussian component (9) 85- 87 F3.1 10-20W/m2 e_SB ? rms uncertainty on SB (10) 89- 92 I4 km/s FWB ?=- FWHM of the broader Gaussian component (9) 94- 97 I4 km/s e_FWB ? rms uncertainty on FWB (10) 99-102 I4 km/s DV ?=- Velocity offset between the two Gaussian components 104-106 I3 km/s e_DV ? rms uncertainty on DV (108) 108 A1 --- l_S[NII] Limit flag on S[NII] 109-112 F4.2 10-20W/m2 S[NII] ?=- Flux of [NII] 6583 where applicable 114-116 I3 km/s W80 ? Overall emission-line width 118-120 I3 km/s e_W80 ? rms uncertainty on W80 (10) -------------------------------------------------------------------------------- Note (1): Field are CDFS for Chandra Deep Field South, Xue et al. (2011, Cat. J/ApJS/195/10) UDS for Ultra Deep Survey, Furusawa et al. (2008, Cat. J/ApJS/176/1) COS for C-COSMOS, Civano et al. (2012, Cat. J/ApJS/201/30) XCOS for XMM-COSMOS, Brusa et al. (2010, Cat. J/ApJ/716/348) SSA22 for SSA22 z=3.09 protocluster field (see Steidel et al. 1998ApJ...492..428S 1998ApJ...492..428S) Note (2): * for targets excluded from the analyses presented in this paper (see Section 4.1). Note (3): Archival redshift type as follows: p = photometric s = secure spectroscopic redshift i = insecure spectroscopic redshift Note (4): + for hard-band values estimated from the soft-band fluxes (see Section 2.1). Note (5): Flag as follows: O = X-ray obscured candidates U = unobscured ? = candidates without sufficient constraints Note (6): Flag to indicate the 'radio luminous' targets with L1.4GHz>1024W/Hz (Section 2.5). Note (7): Primary targeted emission line flag as follows: O = [OIII] H = Halpha Note (8): Note on data as follows: L = line detected C = continuum only detected N = no detection Note (9): for sources with 'alpha' in column BLR, this is the BLR component Note (10): All of the quoted uncertainties are the random errors on the fits due to the noise in the spectra; however, we note that throughout this work we add an extra 30 per cent systematic error to the emission-line fluxes to account for the uncertainty in the flux calibration (see Section 3.2). -------------------------------------------------------------------------------- History: From electronic version of the journal
(End) Patricia Vannier [CDS] 03-Aug-2016
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