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Quasars: The Observational Perspectives

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Fifty Years of Quasars

Abstract

The empirical basis of quasar astronomy can be overawing especially in the twenty-first century. A first source of intricacy involves the nomenclature that has evolved to label the multifold phenomenological manifestations now united under the umbrella of active galactic nuclei (AGNs). A further complication involves observations of the many subclasses with the observations now spanning the electromagnetic spectrum.

Contributions by Mauro D’Onofrio, Paola Marziani, Jack W. Sulentic, Greg Shields, Martin Gaskell, Todd Boroson, Ari Laor, Michael Hawkins, Vladimir Pronik, Sergey Sergeev, Deborah Dultzin, Dirk Grupe, Gordon Richards, Raffaella Morganti, Aleksander Volvach, Sebastian Zamfir, Heino Falcke, Elmar Köording, Martin Elvis, Tracey Jane Turner, Ajit Kembhavi, Luigi Foschini, Yuri Neshpor, and Alberto Franceschini

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Notes

  1. 1.

    http://www.cv.nrao.edu/nvss/, see also [106].

  2. 2.

    http://sundog.gtsci.edu/, see also [47].

  3. 3.

    Zamfir et al. [577] define a population of RI quasars with \(\log [L(1.4\mathrm{GHz})]\,=\,31.0 - 31.6\) (erg s − 1 Hz − 1) in order to test whether they show a restricted domain occupation in the optical plane FWHM(Hβ) vs. R FeII of the 4DE1 space. Their conclusion is that RI and RQ sources are statistically indistinguishable.

  4. 4.

    Note, that given the original meaning of the term “quasar”, the term “radio-loud quasar” is actually a tautology, but we will use it nonetheless given its widespread use.

  5. 5.

    Irritatingly, he did this during that brief time he was sharing an office with me, he even told me what he was doing, and I just did not understand it. Rats. It could have been the Soltan–Elvis argument. I guess it pays to be smart.

  6. 6.

    Not radially, like the ion tail of a solar system comet, otherwise we would not see an asymmetrical dip.

  7. 7.

    The ionization parameter introduced here (and defined by (3.1) on page 143) differs from the ionization parameter U that has been defined previously. ξ is customarily defined as proportional to the energy flux divided by the gas density.

  8. 8.

    Before CGRO, only one quasar, namely, 3C 273 (z = 0. 158), was detected at high-energy γ rays (50–500 MeV) by COS-B [501].

  9. 9.

    Another radio galaxy—NGC 6251 (z = 0. 025)—was later indicated as counterpart of the γ-ray source 3EG J1621 + 8203 [168, 359, 366].

  10. 10.

    Indeed, an old classification name for certain quasar was optically violently variable (OVV).

  11. 11.

    The process with the greater cross section is the photon–photon interaction (γγ).

  12. 12.

    \(\delta = {[\Gamma (1 - \beta \cos \theta )]}^{-1}\), where Γ is the bulk Lorentz factor, β is the speed in units of c, and θ is the viewing angle.

  13. 13.

    At the moment of writing these notes, the second catalogue covering 2 years of operations has not yet been published, but it is forthcoming.

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D’Onofrio, M. et al. (2012). Quasars: The Observational Perspectives. In: D'Onofrio, M., Marziani, P., Sulentic, J. (eds) Fifty Years of Quasars. Astrophysics and Space Science Library, vol 386. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-27564-7_3

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