J/ApJ/685/773       X-ray-UV relations in SDSS DR5 QSOs      (Gibson+, 2008)
Are optically selected quasars universally X-ray luminous?
X-ray-UV relations in Sloan Digital Sky Survey quasars.
    Gibson R.R., Brandt W.N., Schneider D.P.
   <Astrophys. J., 685, 773-786 (2008)>
   =2008ApJ...685..773G 2008ApJ...685..773G
ADC_Keywords: Surveys ; QSOs ; X-ray sources ; Ultraviolet ; Redshifts
Keywords: galaxies: active - galaxies: nuclei - quasars: absorption lines -
          quasars: emission lines - X-rays: general
Abstract:
    We analyze archived Chandra and XMM-Newton X-ray observations of 536
    Sloan Digital Sky Survey (SDSS) Data Release 5 (DR5) quasars (QSOs) at
    1.7≤z≤2.7 in order to characterize the relative UV and X-ray
    spectral properties of QSOs that do not have broad UV absorption lines
    (BALs). We constrain the fraction of X-ray-weak, non-BAL QSOs and find
    that such objects are rare; for example, sources underluminous by a
    factor of 10 comprise ≲2% of optically selected SDSS QSOs. X-ray
    luminosities vary with respect to UV emission by a factor of ≲2 over
    several years for most sources. UV continuum reddening and the
    presence of narrow-line absorbing systems are not strongly associated
    with X-ray weakness in our sample. X-ray brightness is significantly
    correlated with UV emission-line properties, so that relatively
    X-ray-weak, non-BAL QSOs generally have weaker, blueshifted CIV
    λ1549 emission and broader CIII] λ1909 lines. The CIV
    emission-line strength depends on both UV and X-ray luminosity,
    suggesting that the physical mechanism driving the global Baldwin
    effect is also associated with X-ray emission.
Description:
    In this study we consider the 536 SDSS QSOs at redshifts 1.7≤z≤2.7
    that have been observed with Chandra or XMM-Newton. The lower limit on
    redshift ensures that the SDSS spectrum reaches to ∼1400Å allowing
    good coverage of any potential high-velocity CIV absorption, up to
    ~-30000km/s. The upper redshift limit ensures that the 2500Å
    continuum is in view so that we can determine the UV continuum flux
    accurately.
File Summary:
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 FileName   Lrecl  Records   Explanations
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ReadMe         80        .   This file
table1.dat    111      536   Source information
table2.dat     55      536   UV emission line measurements
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See also:
       VII/252 : SDSS-DR5 quasar catalog (Schneider+, 2007)
  J/AJ/133/313 : AGN from RASS and SDSS DR5 (Anderson+, 2007)
   http://www.sdss.org : SDSS Home Page
Byte-by-byte Description of file: table1.dat
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   Bytes Format Units      Label   Explanations
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   1- 19  A19   ---        SDSS    SDSS source name JHHMMSS.ss+DDMMSS.s
  21- 24  F4.2  ---        z       Spectroscopic redshift
  26- 35  I10   ---        ObsId   Chandra or XMM observation identification
                                    number (1)
  37- 41  F5.1  ks         Expo    X-ray exposure time (2)
  43- 46  I4    ct         Scts    Observed-frame soft (0.5-2keV) counts
                                    in source region
  48- 50  I3    ct         Hcts    Observed-frame hard (2-8keV) counts
                                    in source region
      52  I1    ---        X       [0/1] X-ray detected? (1=yes)
      54  I1    ---        B       [0/1] Source in sample B? (1=yes)
      56  A1    ---      l_logR*   Limit flag on logR*
  58- 62  F5.2  [-]        logR*   Radio-loudness parameter (5)
  64- 68  I5    km/s       CIV.0   Rest-frame balnicity index 
                                    for CIV absorption (6)
      70  I1    ---        Mg      Number of narrow Mg II absorption systems (7)
  72- 76  F5.2 [10-7W/Hz]  L1400   Log of monochromatic luminosity at
                                    1400Å (8)
  78- 82  F5.2 [10-7W/Hz]  L2500   Log of monochromatic luminosity at
                                    2500Å (8)
      84  A1    ---      l_L2keV   Limit flag on log2keV
  86- 90  F5.2 [10-7W/Hz]  L2keV   Log of monochromatic luminosity at 2keV (8)
      92  A1    ---      l_a.OX    Limit flag on a.OX
  94- 98  F5.2  ---        a.OX    X-ray/optical spectral index (9)
 100-103  F4.2  ---      e_a.OX    ? Uncertainty in a.OX (10)
     105  A1    ---      l_Da.OX   Limit flag on Da.OX
 107-111  F5.2  ---        Da.OX   Relative X-ray brightness (11)
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Note (1): The Chandra or XMM-Newton observation identification number.
     Ten-digit numbers correspond to XMM-Newton observations, while shorter
     numbers correspond to Chandra observations.
Note (2): Reported by the CIAO or SAS toolchains for the extraction of the
     source region.
Note (5): Where log(R*)=log[Lν(5GHz)/Lν(2500Å)]. We classify
     sources with log(R*)≥1 as "radio-loud" and all other sources as
     "radio-quiet".
Note (6): Similar to the traditional "balnicity index", BI, of Weymann et
     al. (1991ApJ...373...23W 1991ApJ...373...23W), except that it is integrated from velocity
     offsets -25000km/s to 0km/s from the QSO rest frame.
Note (7): Found using the method described in Section 2.2.
Note (8): Where the luminosity is in units of erg/s/Hz.
Note (9): Where a.OX = αOX = 0.3838*log(L(2keV)/L(2500Å)).
Note (10): Errors assumed to be dominated by the error on X-ray luminosity.
Note (11): Relative to "ordinary" QSOs.  Where
     Da.OX = ΔαOX = αOX - 
             (-0.217±0.036)*log(L2500Å)+(5.075±1.118).
      (for instance, a value of -0.5 corresponds to  X-ray weakness 
      by a factor of ∼20 compared to QSOs with the same UV luminosity)
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Byte-by-byte Description of file: table2.dat
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   Bytes Format Units   Label    Explanations
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   1- 19  A19   ---     SDSS     SDSS source identification, JHHMMSS.ss+DDMMSS.s
  21- 25  F5.1  0.1nm   C4EW     Equivalent width of CIV (1549Å)
  27- 32  F6.1  0.1nm   C4Wave   Central wavelength of CIV (1549Å)
  34- 37  F4.1  0.1nm   C4FWHM   Full-Width at Half-Maximum of CIV (1549Å)
  39- 42  F4.1  0.1nm   C3EW     ? Equivalent width of CIII] (1909Å) (1)
  44- 49  F6.1  0.1nm   C3Wave   ? Central wavelength of CIII] (1909Å) (1)
  51- 55  F5.1  0.1nm   C3FWHM   ? Full-Width at Half-Maximum of
                                   CIII] (1909Å) (1)
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Note (1): Blank entries indicate that the C III] emission line could not be
     fit because the spectrum was bad in that region.
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History:
    From electronic version of the journal
(End)                  Greg Schwarz [AAS], Patricia Vannier [CDS]    03-Sep-2009