Subscribe to the gold package and get unlimited access to Shamra Academy
Register a new userThe shape of the blue/UV continuum of B3-VLA radio quasars: Dependence on redshift, blue/UV luminosity and radio power
58
0
0.0
(
0
)
Authors
R. Carballo
Ask ChatGPT about the research
No Arabic abstract
UBVR photometry of a sample of B3-VLA radio quasars, about 80 per cent complete, is used to analyse their spectral energy distribution (SED). The SEDs are generally well fitted with power-laws, with an average slope alpha=-0.39 (S_nu propto nu^alpha). Two quasars appear clearly differenciated, exhibiting redder colours that the rest, and they have redshifts z=0.50 and 1.12. Broad-band composite SEDs in the range 1300-4500 AA were obtained from the remaining quasars and they show the CIV1549 line and a break at around 3000 A, where the SED changes from alpha_blue=0.11+-0.16 at lambda>3000 A to alpha_UV=-0.66+-0.15 at lambda<3000 A. The continuum shape depends on redshift. For the quasars with z<1.2 we find alpha_blue=0.21+-0.16 and alpha_UV=-0.87+-0.20, and for z>1.2 alpha_UV is more flat, -0.48+-0.12. A similar trend is found between alpha_UV and luminosity at 2400 A, L_2400, with luminous quasars exhibiting a bluer spectrum. In addition, an intrinsic correlation is found between L_2400 and radio power at 408 MHz. The correlations alpha_UV-z, alpha_UV-L_2400 and L_2400-z are consistent with accretion disc models with approximately constant black hole mass and accretion rates increasing with redshift. If the trends L_2400-z and P_408-z are predominantly related to the radio-flux limits of the sample, only one of the correlations alpha_UV-L_2400 or alpha_UV-z needs to be intrinsic.
rate research
Read More
We analyzed a large sample of radio-loud and radio-quiet quasar spectra at redshift 1.0 < z < 1.2 to compare the inferred underlying quasar continuum slopes (after removal of the host galaxy contribution) with accretion disk models. The latter predict redder (decreasing) alpha_3000 continuum slopes (L_ u~ u^alpha at 3000Ang) with increasing black hole mass, bluer alpha_3000 with increasing luminosity at 3000Ang, and bluer alpha_3000 with increasing spin of the black hole, when all other parameters are held fixed. We find no clear evidence for any of these predictions in the data. In particular we find that: (i) alpha_3000 shows no significant dependence on black hole mass or luminosity. Dedicated Monte Carlo tests suggest that the substantial observational uncertainties in the black hole virial masses can effectively erase any intrinsic dependence of alpha_3000 on black hole mass, in line with some previous studies. (ii) The mean slope alpha_3000 of radio-loud sources, thought to be produced by rapidly spinning black holes, is comparable to, or even redder than, that of radio-quiet quasars. Indeed, although quasars appear to become more radio loud with decreasing luminosity, we still do not detect any significant dependence of alpha_3000 on radio loudness. The predicted mean alpha_3000 slopes tend to be bluer than in the data. Disk models with high inclinations and dust extinction tend to produce redder slopes closer to empirical estimates. Our mean alpha_3000 values are close to the ones independently inferred at z<0.5 suggesting weak evolution with redshift, at least for moderately luminous quasars.
We investigate the UV continuum slope $alpha$ of a large quasar sample from SDSS DR7. By using specific continuum windows, we build two samples at lower ($0.71<z<1.19$) and higher ($1.90<z<3.15$) redshifts, which correspond to the continuum slopes at longer (NUV) and shorter (FUV) rest wavelength ranges respectively. Overall, the average continuum slopes are $-0.36$ and $-0.51$ for $alpha_{rm NUV}$ and $alpha_{rm FUV}$ with similar dispersions $sigma_{alpha} sim 0.5$. For both samples, we confirm the luminosity dependence of the continuum slope, i.e., fainter quasars have redder spectra. We further find that both $alpha_{rm NUV}$ and $alpha_{rm FUV}$ have a common upper limit ($sim 1/3$) which is almost independent of the quasar luminosity $L_{rm bol}$. This finding implies that the intrinsic quasar continuum (or the bluest quasar), at any luminosity, obey the standard thin disk model. We propose that the other quasars with redder $alpha$ are caused by the reddening from the dust {it locally}. With this assumption, we employ the dust extinction scenario to model the observed $L_{rm bol}-alpha$ relation. We find that, a typical value of $E(B-V)sim0.1$ to $0.3$ mag (depending on the types of extinction curve) of the quasar {it local} dust is enough to explain the discrepancy of $alpha$ between the observation ($sim-0.5$) and the standard accretion disk model prediction ($sim 1/3$).
We present an investigation of the interdependence of the optical-to-X-ray spectral slope ($alpha_{rm ox}$), the HeII equivalent-width (EW), and the monochromatic luminosity at 2500 Angstroms ($L_{2500}$). The values of $alpha_{rm ox}$ and HeII EW are indicators of the strength/shape of the quasar ionizing continuum, from the ultraviolet (UV; 1500--2500 Angstroms), through the extreme ultraviolet (EUV; 300--50 Angstroms), to the X-ray (2 keV) regime. For this investigation, we measure the HeII EW of 206 radio-quiet quasars devoid of broad absorption lines that have high-quality spectral observations of the UV and 2 keV X-rays. The sample spans wide redshift ($approx$ 0.13--3.5) and luminosity (log$(L_{2500}$) $approx$ 29.2--32.5 erg s$^{-1}$ Hz$^{-1}$) ranges. We recover the well-known $alpha_{rm ox}$--$L_{2500}$ and HeII EW--$L_{2500}$ anti-correlations, and we find a similarly strong correlation between $alpha_{rm ox}$ and HeII EW, and thus the overall spectral shape from the UV, through the EUV, to the X-ray regime is largely set by luminosity. A significant $alpha_{rm ox}$--HeII EW correlation remains after removing the contribution of $L_{2500}$ from each quantity, and thus the emission in the EUV and the X-rays are also directly tied. This set of relations is surprising, since the UV, EUV, and X-ray emission are expected to be formed in three physically distinct regions. Our results indicate the presence of a redshift-independent physical mechanism that couples the continuum emission from these three different regions, and thus controls the overall continuum shape from the UV to the X-ray regime.
We study six luminous Lyman-alpha emitters (LAEs) with very blue rest-frame UV continua at $5.7le z le 6.6$. These LAEs have previous HST and Spitzer IRAC observations. Combining our newly acquired HST images, we find that their UV-continuum slopes $beta$ are in a range of $-3.4le beta le -2.6$. Unlike previous, tentative detections of $beta simeq -3$ in photometrically selected, low-luminosity galaxies, our LAEs are spectroscopically confirmed and luminous ($M_{rm UV}<-20$ mag). We model their broadband spectral energy distributions (SEDs), and find that two $betasimeq-2.6pm0.2$ galaxies can be well fitted with young and dust-free stellar populations. However, it becomes increasingly difficult to fit bluer galaxies. We explore further interpretations by including non-zero LyC escape fraction $f_{rm esc}$, very low metallicities, and/or AGN contributions. Assuming $f_{rm esc}simeq0.2$, we achieve the bluest slopes $betasimeq-2.7$ when nebular emission is considered. This can nearly explain the SEDs of two galaxies with $betasimeq-2.8$ and --2.9 ($sigma_{beta}=0.15$). Larger $f_{rm esc}$ values and very low metallicities are not favored by the strong nebular line emission (evidenced by the IRAC flux) or the observed (IRAC 1 - IRAC 2) color. Finally, we find that the $betasimeq-2.9$ galaxy can potentially be well explained by the combination of a very young population with a high $f_{rm esc}$ ($ge0.5$) and an old, dusty population. We are not able to produce two $beta simeq -3.4 pm0.4$ galaxies. Future deep spectroscopic observations are needed to fully understand these galaxies.
We present new deep multi-frequency radio-polarimetric images of a sample of high redshift radio galaxies (HzRGs), having redshift between 1.7 and 4.1. The radio data at 4.7 and 8.2 GHz were taken with the Very Large Array in the A configuration and provide a highest angular resolution of 0.2. Maps of total intensity, radio spectral index, radio polarization and internal magnetic field are presented for each source. The morphology of most objects is that of standard FRII double radio sources, but several contain multiple hot-spots in one or both lobes. Compared to similar samples of HzRGs previously imaged, there is a higher fraction (29%) of compact steep spectrum sources (i.e. sources with a projected linear size less than 20 kpc). Radio cores are identified in about half of the sample and tend to have relatively steep spectra (alpha < -1). Polarization is detected in all but 4 sources, with typical polarization at 8.2 GHz of around 10-20%. The Faraday rotation can be measured in most of the radio galaxies: the observed rotation measure (RM) of 8 radio sources exceeds 100 rad m^{-2} in at least one of the lobes, with large gradients between the two lobes. We find no dependence of Faraday rotation with other properties of the radio sources. If the origin of the Faraday rotation is local to the sources, as we believe, then the intrinsic RM is more than a 1000 rad m^{-2}. Because low redshift radio galaxies residing at the center of clusters usually show extreme RMs, we suggest that the high-z large RM sources also lie in very dense environments. Finally, we find that the fraction of powerful radio galaxies with extreme Faraday rotation increases with redshift, as would be expected if their average environment tends to become denser with decreasing cosmic epoch.
Log in to be able to interact and post comments
comments
Fetching comments
Sign in to be able to follow your search criteria
