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J/ApJS/194/42 SDSS-DR3 MgII-based black hole masses (Rafiee+, 2011)
Supermassive black hole mass estimates using Sloan Digital Sky Survey quasar spectra at 0.7 < z < 2. Rafiee A., Hall P.B. <Astrophys. J. Suppl. Ser., 194, 42 (2011)> =2011ApJS..194...42R
ADC_Keywords: QSOs ; Stars, masses ; Surveys Keywords: catalogs - methods: data analysis - quasars: emission lines - quasars: general Abstract: We present MgII-based black hole (BH) mass estimates for 27602 quasars with rest-frame UV spectra available in the Sloan Digital Sky Survey Data Release Three (Cat. II/259; superseded by II/294). This estimation is possible due to the existence of an empirical correlation between the radius of the broad-line region (BLR) and the continuum luminosity at 3000Å. We regenerate this correlation by applying our measurement method to UV spectra of low-redshift quasars in the Hubble Space Telescope/International Ultraviolet Explorer databases which have corresponding reverberation mapping estimates of the Hβ BLR's radius. Our mass estimation method uses the line dispersion rather than the full width at half-maximum of the low-ionization MgII emission line. File Summary:
FileName Lrecl Records Explanations
ReadMe 80 . This file table3.dat 280 27602 Catalog of virial mass measurements
See also: II/294 : The SDSS Photometric Catalog, Release 7 (Adelman-McCarthy+, 2009) VII/260 : The SDSS-DR7 quasar catalog (Schneider+, 2010) J/ApJ/699/800 : Mass functions of active black holes (Vestergaard+, 2009) J/ApJ/680/169 : SDSS DR5 virial black hole masses (Shen+, 2008) J/ApJ/669/791 : Quasar black hole masses (Wilhite+, 2007) J/ApJ/614/91 : Black hole mass and accretion rate of AGNs (Wu+, 2004) J/ApJ/596/437 : Stellar-mass black holes in the SDSS (Chisholm+, 2003) http://www.sdss.org/ : SDSS Home Page Byte-by-byte Description of file: table3.dat
Bytes Format Units Label Explanations
1- 18 A18 --- SDSS SDSS designation (HHMMSS.ss+DDMMSS.s; J2000) 20- 29 F10.6 deg RAdeg Right Ascension in decimal degrees (J2000) 31- 40 F10.6 deg DEdeg Declination in decimal degrees (J2000) 42- 47 F6.4 --- z Redshift (spectroscopic) 49- 54 F6.3 mag imag PSF i-band apparent magnitude 56- 62 F7.3 mag iMAG PSF i-band absolute magnitude; K-corrected to z=2 64- 68 I5 d MJD Modified Julian Date of spectroscopy 70- 73 I4 --- Plate Plate number 75- 77 I3 --- Fiber Fiber identification number 79- 84 F6.4 0.1nm sigma Instrumental σ; in Angstroms 86- 93 F8.4 0.1nm sim(b) ?=0 σ(MgII) estimates from the second moments (1) 95-102 F8.4 0.1nm st(b) ?=0 Intrinsic σ(MgII) (1) 104-111 E8.2 cW/m2/nm F3(b) ?=0 F_λ_ at 3000Å; in erg/s/cm2/Å (1) 113-120 E8.2 10+37W LL(b) ?=0 Monochromatic 3000Å luminosity; in 1044erg/s units (2) 122-130 F9.4 173AU R(ld-b) ?=0 Radius of the BLR (broad-line region) in light-days units (3) 132-137 F6.3 --- SN(G-b) Median S/N in G band (1) 139-144 F6.3 --- SN(R-b) Median S/N in R band (1) 146-151 F6.3 --- SN(I-b) Median S/N in I band (1) 153-160 E8.3 Msun MBH(bb) ?=0 BH mass, before PCA and RPC (1) 162-169 E8.3 Msun e_MBH(bb) ?=0 Error in MBH(bb) (1) 171-177 F7.4 0.1nm sim(a) ?=0 σ(MgII) estimates from the second moments (4) 179-185 F7.4 0.1nm st(a) ?=0 Intrinsic σ(MgII); in Angstrom (4) 187-194 E8.3 cW/m2/nm F3(a) ?=0 F_λ_ at 3000Å; in erg/s/cm2/Å (4) 196-203 E8.3 10-7W LL(a) ?=0 Monochromatic 3000Å luminosity; in 1044erg/s units (5) 205-213 F9.4 173AU R(ld-a) ?=0 Radius of the BLR (broad-line region) in light-days units (6) 215-220 F6.3 --- SN(G-a) Median S/N in G band (4) 222-227 F6.3 --- SN(R-a) Median S/N in R band (4) 229-234 F6.3 --- SN(I-a) Median S/N in I band (4) 236-243 E8.3 Msun MBH(ab) ?=0 BH mass, after PCA and before RPC (4) 245-252 E8.3 Msun e_MBH(ab) ?=0 Error in MBH(ab) (4) 254-261 E8.3 Msun MBH(aa) ?=0 BH mass, after PCA and RPC (7) 263-270 E8.3 Msun e_MBH(aa) ?=0 Error in MBH(aa) (7) 272-278 F7.5 --- z(RH) ?=0 Redshift re-estimated by this study (7) 280 I1 --- DR3c [0/1] In DR3 complete subsample? 0=no, 1=yes
Note (1): Before applying Principal Component Analysis and Radiation Pressure Correction. Note (2): Before applying Principal Component Analysis and Radiation Pressure Correction. Bolometric Luminosity can be estimated using BC(3000Å)=5.15 and the monochromatic luminosity at 3000Å (Shen et al. 2008, Cat. J/ApJ/680/169). Note (3): Before applying Principal Component Analysis and Radiation Pressure Correction. Note (4): After applying Principal Component Analysis but before Radiation Pressure Correction. These are the recommended results. Note (5): After applying Principal Component Analysis but before Radiation Pressure Correction. These are the recommended results. Bolometric Luminosity can be estimated using BC(3000Å)=5.15 and the monochromatic luminosity at 3000Å (Shen et al. 2008, Cat. J/ApJ/680/169). Note (6): After applying Principal Component Analysis but before Radiation Pressure Correction. These are the recommended results. Note (7): After applying Principal Component Analysis and Radiation Pressure Correction.
History: From electronic version of the journal
(End) Greg Schwarz [AAS], Emmanuelle Perret [CDS] 01-Aug-2011
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