2014A&A...570A..96S


Query : 2014A&A...570A..96S

2014A&A...570A..96S - Astronomy and Astrophysics, volume 570A96-96 (2014/10-1)

GTC spectra of z ≃ 2.3 quasars: comparison with local luminosity analogs.

SULENTIC J.W., MARZIANI P., DEL OLMO A., DULTZIN D., PEREA J. and NEGRETE C.A.

Abstract (from CDS):

The advent of 8-10m class telescopes for the first time makes it possible to compare in detail quasars with similar luminosity and very different redshifts. We conducted a search for z-dependent gradients in line-emission diagnostics and derived physical properties by comparing, in a narrow bolometric luminosity range (logL ∼46.1±0.4[erg/s]), some of the most luminous local z<0.6 quasars with some of the lowest luminosity sources yet found at redshift z=2.1-2.5. Moderate signal-to-noise ratio spectra for 22 high-redshift sources were obtained with the 10.4m Gran Telescopio Canarias (GTC), for which the HST (largely the Faint Object Spectrograph) archive provides a low-redshift control sample. We compared the spectra in the context of the 4D Eigenvector 1 formalism, meaning that we divided both source samples into highly accreting population A and population B sources accreting at a lower rate. CIVλ1549, the strongest and most reliable diagnostic line, shows very similar properties at both redshifts, which confirms the CIVλ1549 profile differences at high redshift between populations A and B, which are well established in local quasars. The CIVλ1549 blueshift that appears quasi-ubiquitous in higher L sources is found in only half (population A) of the quasars observed in the two samples. A CIVλ1549 evolutionary Baldwin effect is certainly disfavored. We find evidence for lower metallicity in the GTC sample that may point toward a gradient with z. No evidence for a gradient in MBH or L/LEdd is found. Spectroscopic differences established at low z are also present in much higher redshift quasars. Our results on the CIVλ1549 blueshift suggest that it depends both on source luminosity and L/LEdd. Given that our samples involve sources with very similar luminosity, the evidence for a systematic metallicity decrease, if real, points toward an evolutionary effect. Our samples are not large enough to effectively constrain possible changes of MBH or L/LEdd with redshift. The two samples appear representative of a slowly evolving quasar population that is most likely present at all redshifts.

Abstract Copyright: ∼

Journal keyword(s): quasars: emission lines - quasars: supermassive black holes - ISM: abundances - line: profiles - cosmology: observations

VizieR on-line data: <Available at CDS (J/A+A/570/A96): table12.dat sp/*>

Simbad objects: 31

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Number of rows : 31
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 Mrk 1502 Sy1 00 53 34.9331107632 +12 41 35.929269132   14.41 14.03     ~ 1242 1
2 GD 24 WD* 02 13 05.3882485536 +16 43 12.484075620   16.0       DA 15 0
3 Feige 34 HS* 10 39 36.7358839104 +43 06 09.212615280 9.613 10.91 11.14 11.319 11.464 sdOp 731 0
4 GD 140 WD* 11 37 05.1041466528 +29 47 58.288741080 11.47 12.42 12.45 12.73 12.714 DA2.2 257 0
5 QSO B1216-1046 QSO 12 18 48.6969173736 -11 03 32.606123724     21.1     ~ 7 1
6 QSO B1232-1059 QSO 12 34 39.1070566056 -11 16 23.352980664     20.7     ~ 6 0
7 QSO B1232-1113 QSO 12 35 02.4660909264 -11 30 28.628364924     20.9     ~ 7 0
8 [VV2006] J123742.6+621811 QSO 12 37 42.529 +62 18 11.70 22.49 21.6741 22.097 21.8 21.5746 ~ 37 0
9 QSO B1257+357 QSO 12 59 35.3383760424 +35 30 52.189151904   20.89 20.78     ~ 18 0
10 [VV2006] J134206.3-003702 QSO 13 42 06.3480711672 -00 37 01.252136820   20.68 20.34     ~ 15 0
11 QSO B1340+277 QSO 13 42 35.91 +27 29 11.7   21.0 21.4     ~ 6 0
12 [VV96] J134424.0-002846 QSO 13 44 23.958 -00 28 46.53   21.71       ~ 6 0
13 Feige 92 HS? 14 11 31.8784689192 +50 07 04.144734912   11.42 11.50     B9kp 48 0
14 [OKM2018] SWIFT J1419.0-1323 Sy1 14 19 03.8170514760 -13 10 44.785212600   16.46 16.10 16.50   ~ 245 0
15 [VV2006] J143400.1+002648 QSO 14 34 00.0936593640 +00 26 49.098612264     20.83     ~ 15 0
16 2MASS J15315047+2423178 QSO 15 31 50.4620222616 +24 23 17.732350032   20.52   19.17   ~ 15 0
17 [VV2006] J153231.6-231032 QSO 15 32 31.52834798 -23 10 32.4637064     21.4     ~ 16 1
18 [VV2000] J162359.1+554108 QSO 16 23 59.206 +55 41 08.78   21.02 20.79     ~ 11 1
19 [VV2000] J162421.1+554243 QSO 16 24 21.286 +55 42 43.07   21.97 21.87     ~ 10 1
20 Ross 640 WD* 16 28 25.0030896166 +36 46 15.846877416   14.01   13.9   DZ6 220 0
21 QSO B1634+332 QSO 16 36 21.0961314576 +33 09 42.758753904   21.22 21.02     ~ 7 0
22 QSO B1640+4056 QSO 16 42 26.902 +40 50 34.34   20.4 20.4     ~ 9 0
23 SDSS J171941.24+592242.1 QSO 17 19 41.2449942432 +59 22 42.046512852   21.06 20.69     ~ 3 0
24 QSO B1721+3400 QSO 17 23 12.4823503248 +33 57 59.845088592   21.01 20.86     ~ 12 0
25 QSO B1834+509 QSO 18 36 09.2424058944 +51 00 22.231902168   20.2 20.2     ~ 6 0
26 QSO B1835+509 QSO 18 36 14.4395707200 +51 01 44.615921016   20.6 20.6     ~ 7 0
27 LAWD 73 WD* 19 00 10.2533239461 +70 39 51.416733790   13.24   13.5   DAP4.5 264 0
28 [VV2006] J205620.5-043059 QSO 20 56 20.5833745584 -04 31 00.690827988           ~ 6 0
29 SDSS J224314.28+005528.2 QSO 22 43 14.2822844088 +00 55 28.225734096   20.69 20.36     ~ 12 0
30 HD 219175 PM* 23 14 07.4751763094 -08 55 27.579468877   8.12 7.56     F7V 95 0
31 [VV2006] J234752.5+010306 QSO 23 47 52.5603647706 +01 03 05.042258966           ~ 15 0

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