Baldwin effect (astronomy)

The Baldwin effect in astronomy describes a relationship between continuum and emission-line fluxes observed in the electromagnetic spectra of quasars and active galactic nuclei, namely an anticorrelation between the equivalent width, Wλ, of a spectral line and the continuum luminosity, L, in broad UV optical emission lines. This means that the ratio of brightness of the emission line to the brightness of the nearby continuum decreases with increasing luminosity of the continuum.

Discovery and observations

The effect was discovered in observations of high-redshift quasars reported in 1977, and has been commonly named after the discoverer[1] Jack Allen Baldwin, an astronomer at Lick Observatory. It was found that the width of the broad ultraviolet C IV λ 1549 emission line, caused by the presence of thrice ionised carbon C3+, increased with increasing continuum luminosity of the source.[2] For flat-spectrum, radio-loud quasars the relation

Wλ (C IV λ 1549) ~ L-0.6

was found.[3]

The same effect has been observed for other spectral lines such as the Lα hydrogen line and the C III λ 1909 line of twice ionised carbon.[2] It has also been found for spectral lines in the infrared range, e.g. in several Seyfert galaxies.[4]

Explanation

More or less satisfactory explanations of the phenomenon have been attempted using photoionization models, continuum beaming, variability, or continuum shape. An adequate, but not exclusive explanation is offered as a consequence of the presence of massive accretion disks in the centres of active galaxies and quasars.[5] However, a complete explanation is still outstanding.

References

  1. ↑ Pogge, Richard W.; Peterson, Bradley M. (1992). "The intrinsic nature of the Baldwin effect". Astronomical Journal. 103: 1084–1088. Bibcode:1992AJ....103.1084P. doi:10.1086/116127. ISSN 0004-6256.
  2. 1 2 Baldwin, Jack A. (1977). "Luminosity Indicators in the Spectra of Quasi-Stellar Objects". Astrophysical Journal. 214: 679–684. Bibcode:1977ApJ...214..679B. doi:10.1086/155294.
  3. ↑ Baldwin, J. A.; Wampler, E. Joseph; Gaskell, C. Martin (1989). "Emission-line properties of optically and radio-selected complete quasar samples". Astrophysical Journal, Part I. 338: 630–653. Bibcode:1989ApJ...338..630B. doi:10.1086/167224. ISSN 0004-637X.
  4. ↑ Hönig, S. F.; Smette, A.; Beckert, T.; Horst, H.; Duschl, W.; Gandhi, P.; Kishimoto, M.; Weigelt, G. (2008). "Discovery of a strong Baldwin effect in mid-infrared AGN lines". Astronomy and Astrophysics. 485 (2): L21–L24. doi:10.1051/0004-6361:200810123.
  5. ↑ Netzer, H. (1985). "Quasar discs – I. The Baldwin effect". MNRAS. 216 (1): 63–78. Bibcode:1985MNRAS.216...63N. doi:10.1093/mnras/216.1.63.

External links

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