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In-situ acceleration of radio-emitting particles in the lobes of radio galaxies: Evolving observational perspective and recent clues

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Abstract

The issue of radiation mechanisms triggered in 1950–60s the first applications of plasma physics to understand the nature of radio galaxies. This interplay has steadily intensified during the past five decades due to the premise of in-situ acceleration of relativistic electrons occurring in the lobes of radio galaxies. This article briefly traces the chain of these remarkable developments, largely from an observational perspective. We recount several observational and theoretical milestones established along the way and the lessons drawn from them. We also present a new observational clue about in-situ acceleration of the relativistic particles radiating in the lobes of radio galaxies, gleaned by us from the very recently published sensitive radio observations of a tailed radio source in the galaxy cluster Abell 1033.

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  1. Before 1970, the most comprehensive information about structures of radio galaxies came using the Cambridge one-mile telescope (Ryle 1962), which also yielded spectral gradients across some sources (MacDonald et al. 1968). However, the scope of this information was quite limited due to the small frequency range covered (408–1407 MHz) and the large beam size (\({\sim }80\) arcsec).

  2. The lunar occultation technique for determining positions and brightness profiles of celestial radio sources was initially proposed by Getmantsev & Ginzburg (1950). It came into the limelight when its application by Hazard et al. (1963) paved the way for the discovery of the first quasar, 3C 273 (Schmidt 1963). The restoration technique for recovering the strip-brightness distribution from a lunar occultation profile, which required the removal of the effects of Fresnel diffraction at the Moon’s limb, was first developed by Scheuer (1962), von Hoerner (1964) and Cohen (1969). Early applications of this technique to radio galaxies and quasars are summarized in Taylor & de Jong (1968). Except for 3C 273, the occultations were observed using medium-size telescopes (the 140-ft or 85-ft dishes in the USA) and covering a narrow frequency range (200–500 MHz). Due to these constraining factors, these pioneering occultation observations yielded limited information on spectral index gradients across radio galaxies. Likewise, no significant information on spectral index gradients could be adduced from lunar occultation observations of six sources at 81.5 MHz (Collins & Scott 1969). The same holds for the occultation of 3C 212 reported at the very low frequency of 20–25 MHz (Bovkun 1976).

  3. For a more general account of this, sometimes termed ‘youth-redshift degeneracy’, see Blundell & Rawlings (1999).

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Acknowledgements

We thank Henrik Edler for permission to republish Figure 1 and for providing the data used in plotting Figure 2. With the publication of this article, the authors will have co-authored 100 research publications. We take this opportunity to dedicate this article to the memory of Prof. Govind Swarup (1929–2020), who seeded radio astronomy in India and steered its course for the first five decades. GK is thankful to the Indian National Science Academy (INSA) for his current INSA Senior Scientist position.

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Correspondence to Paul J. Wiita.

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Gopal-Krishna, Wiita, P.J. In-situ acceleration of radio-emitting particles in the lobes of radio galaxies: Evolving observational perspective and recent clues. J Astrophys Astron 45, 12 (2024). https://doi.org/10.1007/s12036-024-10000-4

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