2009A&A...495...83M


Query : 2009A&A...495...83M

2009A&A...495...83M - Astronomy and Astrophysics, volume 49583-112 (2009/2-3)

VLT/ISAAC spectra of the Hβ region. in intermediate-redshift quasars. III. Hβ broad-line profile analysis and inferences about BLR structure.

MARZIANI P., SULENTIC J.W., STIRPE G.M., ZAMFIR S. and CALVANI M.

Abstract (from CDS):

We present new VLT ISAAC spectra for 30 quasars, which we combine with previous data to yield a sample of 53 intermediate-redshift (z≃0.9-3.0) sources. The sample is used to explore properties of prominent lines in the hβ spectral region of these very luminous quasars. We compare this data with two large low-redshift (z<0.8) samples in a search for trends over almost 6dex in source luminosity. We find two major trends: (1) a systematic increase in minimum FWHM hβ with luminosity (discussed in a previous paper). This lower FWHM envelope is best fit by assuming that the narrowest sources radiate near the Eddington limit, show line emission from a virialized cloud distribution, and obey a well-defined broad line region size vs. luminosity relation. (2) A systematic decrease in equivalent width of [oIII]λλ4959,5007 (from W≃15 to ∼1Å) with increasing source bolometric luminosity (from logLbol≃43 to logLbol≃49). Other identified trends require differntiating between so-called Population A and Bsources. We generate median composite spectra in six luminosity bins to maximize S/N. Population A sources show reasonably symmetric Lorentzian hβ profiles at all luminosities, while Pop. B sources require two component fits involving an unshifted broad and a redshifted very broad component. Very broad hβ increases in strength with increasing logLbol, while the broad component remains constant, resulting in an apparent ``Baldwin effect'' with equivalent width decreasing from W∼80 to ∼20Å over our sample luminosity range. The roughly constant equivalent width shown by the hβ very broad component implies production in optically-thick, photoionized gas. The onset of the redshifted very broad component appears to be a critical change that occurs near the Pop. A-B boundary at FWHM hβ≃4000km/s, which we relate to a critical Eddington ratio (≃0.2±0.1).

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Journal keyword(s): galaxies: quasars: general - galaxies: quasars: emission lines - black hole physics - line: profiles

Simbad objects: 35

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Number of rows : 35
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 [VV98] J003806.3-283648 QSO 00 38 06.4669749456 -28 36 49.014457020   17.03 17.20     ~ 12 0
2 [VV2000] J004539.5-224356 Bla 00 45 39.5973797976 -22 43 55.340267880   17.06 17.20 16.23   ~ 28 1
3 Mrk 1502 Sy1 00 53 34.9331107632 +12 41 35.929269132   14.41 14.03     ~ 1242 1
4 PHL 7019 QSO 01 00 39.3008393928 -32 14 54.953234196   18.4 17.10     ~ 12 0
5 PHL 3349 QSO 01 08 00.0883413576 -29 50 12.847457184   17.06 16.70     ~ 8 0
6 QSO B0109-353 QSO 01 11 43.6321128912 -35 03 00.587535660   16.6 16.9     ~ 79 0
7 QSO B0119-3325 QSO 01 22 04.3890758112 -33 10 12.286752348   17.17 17.2     ~ 8 0
8 [VV2000] J014455.1-460428 QSO 01 44 55.1055884424 -46 04 26.720064228   16.9       ~ 5 0
9 [VV2000] J020552.4-461330 QSO 02 05 52.4564457120 -46 13 30.295753176     17.34     ~ 10 0
10 QSO B0205-3756 QSO 02 07 27.11 -37 41 55.8   17.17 17.2     ~ 30 0
11 [VV2000] J022628.9-381249 QSO 02 26 28.7908685376 -38 12 48.337846236   16.83 16.10     ~ 5 0
12 [VV2000] J023113.6-555010 QSO 02 31 13.5849820632 -55 50 10.281583572     16.90     ~ 5 0
13 [VV2000] J024047.9-475644 QSO 02 40 48.0080544792 -47 56 43.356193836   17.12 17.60     ~ 7 0
14 [VV2000] J025055.4-361636 QSO 02 50 55.3418030448 -36 16 35.794668072   16.58 16.20 16.3   ~ 31 0
15 [VV96] J025240.1-553832 QSO 02 52 40.1052821064 -55 38 32.029465596   17.4 17.4     ~ 15 0
16 [VV96] J035059.3-524035 QSO 03 50 59.4251742840 -52 40 34.515922152 15.54 16.29 16.11     ~ 12 0
17 [VV2000] J035509.9-391027 QSO 03 55 09.9543157680 -39 10 27.272745696     15.60     ~ 7 0
18 [VV2000] J040114.0-395132 QSO 04 01 14.0652420192 -39 51 32.682179196     17.00     ~ 16 0
19 [VV2000] J043711.8-430603 QSO 04 37 11.7934289544 -43 06 04.281362568     17.20     ~ 14 0
20 [VV96] J043837.3-370342 QSO 04 38 37.3845247512 -37 03 41.858978220   17.0 17.0     ~ 11 0
21 QSO B0512-3329 QSO 05 14 10.91 -33 26 22.4     17.0     ~ 62 0
22 3C 206 Sy1 08 39 50.5829445936 -12 14 34.327188564   15.78 15.76     ~ 254 1
23 QSO B0940-1050 QSO 09 42 53.5078384704 -11 04 25.931336376   16.96 16.6 16.6   ~ 102 0
24 [VV2000] J104219.3-074036 QSO 10 42 19.2758048208 -07 40 36.381885060   17.16 17.40     ~ 11 0
25 QSO B1120+0154 QSO 11 23 20.7258496872 +01 37 47.506567620   16.45 16.12     ~ 135 1
26 LBQS 1348+0118 QSO 13 51 28.3252180560 +01 03 38.563706592   17.49 17.22     ~ 43 0
27 QSO B1349+001 QSO 13 51 50.4774968064 -00 07 38.941651236   17.08 16.86     ~ 50 0
28 [VV2000] J141221.8+004717 QSO 14 12 21.7539348984 +00 47 18.891515184   16.87 16.46     ~ 10 0
29 [OKM2018] SWIFT J1419.0-1323 Sy1 14 19 03.8170514760 -13 10 44.785212600   16.46 16.10 16.50   ~ 245 0
30 LBQS 1430-0041 QSO 14 33 21.4210756680 -00 54 45.736079364   16.71 16.39     ~ 17 0
31 [VV2000] J150759.0+020053 QSO 15 07 59.0606834112 +02 00 53.841474576   17.18 16.77     ~ 32 0
32 Z 252-40 Bla 17 19 14.4925971408 +48 58 49.423205136   15.86 14.81 9.44   ~ 335 1
33 [VV2000] J215052.3-315825 QSO 21 50 52.2977004648 -31 58 25.785792228   16.84 17.10     ~ 14 0
34 [VV2000] J215954.7-400550 QSO 21 59 54.6863451864 -40 05 50.383293108     17.90     ~ 13 0
35 [VV2000] J233742.3-301317 QSO 23 37 42.3557983584 -30 13 18.128981892     16.90     ~ 7 0

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