2018
DOI: 10.3390/galaxies6010015
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The Global Jet Structure of the Archetypical Quasar 3C 273

Abstract: Abstract:A key question in the formation of the relativistic jets in active galactic nuclei (AGNs) is the collimation process of their energetic plasma flow launched from the central supermassive black hole (SMBH). Recent observations of nearby low-luminosity radio galaxies exhibit a clear picture of parabolic collimation inside the Bondi accretion radius. On the other hand, little is known of the observational properties of jet collimation in more luminous quasars, where the accretion flow may be significantl… Show more

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Cited by 29 publications
(24 citation statements)
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“…Therefore the collimation of AGN jets from M BH = 10 8−9 M ⊙ might commonly break at distances around r SGI ∼ 3 × 10 5 R s . Note that the jet profile of 1H 0323+342 shown by red color in Figure 8 is also sufficiently overlapped with those of NGC 6251 (Tseng et al 2016;Nakamura et al 2018) and 3C 273 (Akiyama et al 2018).…”
Section: Jet Collimation Confinement Medium and Black Hole Massmentioning
confidence: 73%
See 1 more Smart Citation
“…Therefore the collimation of AGN jets from M BH = 10 8−9 M ⊙ might commonly break at distances around r SGI ∼ 3 × 10 5 R s . Note that the jet profile of 1H 0323+342 shown by red color in Figure 8 is also sufficiently overlapped with those of NGC 6251 (Tseng et al 2016;Nakamura et al 2018) and 3C 273 (Akiyama et al 2018).…”
Section: Jet Collimation Confinement Medium and Black Hole Massmentioning
confidence: 73%
“…Regarding the extended jet, there is a possible trend that the spectra on and right down the quasi-stationary feature S are slightly flatter than those in the upstream side of S. Although the uncertainties are still large, this might indicate reenergization of nonthermal electrons via shock in the feature S. Structural transition of jet profile has recently been discovered in some nearby radio galaxies (M87; Asada & Nakamura (2012), NGC 6251; Tseng et al (2016), 3C 273; Akiyama et al (2018), NGC 4261; Nakahara et al (2018)). This has triggered active discussion about the mechanisms of jet formation and collimation.…”
Section: Spectramentioning
confidence: 98%
“…Several observational studies have been performed with the aim of determining the extension of the acceleration and collimation region, thus providing constraints for theoretical models. Such studies were mostly focused on the analysis of low-luminosity radio galaxies, such as NGC 6251 (Tseng et al 2016), 3C 84 (Giovannini et al 2018), 3C 270 (Nakahara et al 2018), 3C 264 (Boccardi et al 2019), NGC 1052 (Nakahara et al 2020) and M 87 (Asada & Nakamura 2012;Mertens et al 2016;Hada et al 2016;Kim et al 2018;Nokhrina et al 2019), but some constraints for high-luminosity radio galaxies, like Cygnus A (Boccardi et al 2016a,b;Nakahara et al 2019), and blazars (Giroletti et al 2008;Akiyama et al 2018;Hada et al 2018;Algaba et al 2019;Traianou et al 2020) were also provided. Moreover, part of the MOJAVE sample was investigated by Pushkarev et al (2017), Kovalev et al (2020).…”
Section: Introductionmentioning
confidence: 99%
“…In particular, mm-VLBI studies (see Boccardi et al (2017) for a review) provide high resolution images of regions deep in the jet that are otherwise optically thick at longer centimeter wavelengths. Millimeter (mm)-wave VLBI images, therefore, give us a direct probe of the inner geometry and velocity structure of jets in different AGN classes: radio galaxies (Cygnus A - Boccardi et al (2016a,b); M 87 - Hada et al (2013), Kim et al (2018); NGC 4261 - Nakahara et al (2018); NGC 1052 - Baczko et al (2016Baczko et al ( , 2019; Nakahara et al (2020)), a narrowline Seyfert 1 (NLS1) galaxy, 1H 0323+342, Hada et al (2018), and few blazars (Mrk 501 - Giroletti et al (2004); 3C 273 Akiyama et al (2018); TXS 2013+370 -Traianou et al (2020). The picture is further complicated by synchrotron opacity effects (Blandford & Königl 1979) which can obscure the inner jet and shift the apparent location of the VLBI radio core at large distances from the black hole, ∼ 10 (4−6) Schwarzshild radii (R s ) (e.g.…”
Section: Introductionmentioning
confidence: 99%