NGC 3516: The Long‐Term Variability of the Active Galactic Nucleus Emission‐Line and Absorption‐Line Regions

1999 ◽  
Vol 524 (2) ◽  
pp. 707-731 ◽  
Author(s):  
M. R. Goad ◽  
A. P. Koratkar ◽  
J. Kim‐Quijano ◽  
K. T. Korista ◽  
P. T. O'Brien ◽  
...  
2020 ◽  
Vol 634 ◽  
pp. A111 ◽  
Author(s):  
J. P. U. Fynbo ◽  
P. Møller ◽  
K. E. Heintz ◽  
J. N. Burchett ◽  
L. Christensen ◽  
...  

We report on the discovery of a peculiar broad absorption line (BAL) quasar identified in our Gaia-assisted survey of red quasars. The systemic redshift of this quasar was difficult to establish because of the absence of conspicuous emission lines. Based on deep and broad BAL troughs of at least Si IV, C IV, and Al III, a redshift of z = 2.41 was established under the assumption that the systemic redshift can be inferred from the red edge of the BAL troughs. However, we observe a weak and spatially extended emission line at 4450 Å that is most likely due to Lyman-α emission, which implies a systemic redshift of z = 2.66 if correctly identified. There is also evidence for the onset of Lyman-α forest absorption bluewards of 4450 Å and evidence for Hα emission in the K band consistent with a systemic redshift of z = 2.66. If this redshift is correct, the quasar is an extreme example of a detached low-ionisation BAL quasar. The BALs must originate from material moving with very large velocities ranging from 22 000 km s−1 to 40 000 km s−1. To our knowledge, this is the first case of a systemic-redshift measurement based on extended Lyman-α emission for a BAL quasar. This method could also be useful in cases of sufficiently distant BL Lac quasars without systemic-redshift information.


2019 ◽  
Vol 870 (2) ◽  
pp. L25 ◽  
Author(s):  
W. Yi ◽  
M. Vivek ◽  
W. N. Brandt ◽  
T. Wang ◽  
J. Timlin ◽  
...  

1979 ◽  
Vol 53 ◽  
pp. 324-328
Author(s):  
Paula Szkody

The 4 known AM Her stars or polars (AM Her, ANUMa, W Pup, and 2A0311-227) are characterized by large circular polarizations of 10-35%, (Tapia 1977a, b, Krzeminski and Serkowski 1977), an emission line spectrum with strong H and He lines (Crampton and Cowley 1977, Greenstein et al. 1977), complex photometric variations (Szkody 1978, Priedhorsky and Krzeminski 1978, Warner & Nather 1972), long term high and low states and short orbital periods (80-180 min.). Models of these systems envision a close binary containing a magnetic white dwarf primary (B ~ 108G) and late type main sequence secondary transferring material into an accretion funnel over one or both poles of the white dwarf (Stockman et al. 1977, Lamb & Masters 1979, Liebert et al. 1978).


1965 ◽  
Vol 43 (10) ◽  
pp. 1843-1852 ◽  
Author(s):  
Sushil K. Misra ◽  
J. M. Daniels

A parameter R(v), relevant to velocity-sensitive Mössbauer spectroscopy, has been computed for the case where the orientation of 57Co nuclei is produced dynamically by the Overhauser effect. This particular pumping scheme for producing nuclear orientation brings out two features. (1) It allows the determination of η, the ratio of flip-flop to flip-flip thermal relaxations, by an experimental measurement of R(v), since the theoretical expressions for R(v) are found to be quite sensitive to the value of η. A numerical evaluation for three cases of overlap between absorber and emitter lines indicates wide variation in R(v) for increasing values of η from 10−7 to 107: for case (a), R(v) increases monotonically from 8.5 × 10−7 to 1.07 × 106 when emission line 3/2 → 1/2 overlaps absorption line −1/2 → −3/2; for case (b), R(v) decreases monotonically from 1.34 × 1014 to 8.91 × 10−5 when emission line −1/2 → 1/2 overlaps absorption line −1/2 → 1/2; and for case (c), R(v) decreases monotonically from 1.62 × 102 to 6.14 × 10−3 when source lines −1/2 → −1/2, 1/2 → −1/2, 1/2 → 1/2, and 3/2 → 1/2 overlap absorber lines −1/2 → −3/2, −1/2 → 1/2, 1/2 → −1/2, and 1/2 → 1/2 respectively. (2) Since these R(v)'s are found to be much different from those that would be achieved through a pumping scheme using the Jeffries–Abragam effect, the possibility of using the Mössbauer effect to distinguish between the various ways of producing the nuclear orientation is suggested.


2020 ◽  
Vol 499 (1) ◽  
pp. 1522-1529
Author(s):  
Timothy R Miller ◽  
Nahum Arav ◽  
Xinfeng Xu ◽  
Gerard A Kriss

ABSTRACT Determining the distance of quasar absorption outflows from the central source (R) and their kinetic luminosity ($\dot{E}_\mathrm{\scriptstyle k}$) is crucial for understanding their contribution to active galactic nucleus (AGN) feedback. Here, we summarize the results for a sample of nine luminous quasars that were observed with the Hubble Space Telescope. We find that the outflows in more than half of the objects are powerful enough to be the main agents for AGN feedback, and that most outflows are found at R > 100 pc. The sample is representative of the quasar absorption outflow population as a whole and is unbiased towards specific ranges of R and $\dot{E}_\mathrm{\scriptstyle k}$. Therefore, the analysis results can be extended to the majority of such objects, including broad absorption line quasars. We find that these results are consistent with those of another sample (seven quasars) that is also unbiased towards specific ranges of R and $\dot{E}_\mathrm{\scriptstyle k}$. Assuming that all quasars have absorption outflows, we conclude that most luminous quasars produce outflows that can contribute significantly to AGN feedback. We also discuss the criterion for whether an outflow is energetic enough to cause AGN feedback effects.


1987 ◽  
Vol 92 ◽  
pp. 84-86
Author(s):  
D. R. Gies ◽  
David McDavid

Evidence is now accumulating that many Be stars display photospheric line profile variations on timescales of days or less that are probably caused by nonradial pulsations (Baade 1984; Penrod 1986). In some circumstances these pulsations can promote mass loss into the circumstellar envelope, and consequently the conditions in the inner part of the envelope may vary on similar timescales. Changes in the envelope could produce variations in the polarization and emission line profiles, and observers have reported rapid variability in both. We describe here an initial attempt to search for simultaneous variations in continuum polarization, Hα emission, and the He I λ6678 photospheric absorption line in order to investigate correlated changes on short timescales.


2019 ◽  
Vol 488 (1) ◽  
pp. 135-152 ◽  
Author(s):  
Maan H Hani ◽  
Sara L Ellison ◽  
Martin Sparre ◽  
Robert J J Grand ◽  
Rüediger Pakmor ◽  
...  

ABSTRACT Galaxies are surrounded by massive gas reservoirs (i.e. the circumgalactic medium; CGM) which play a key role in their evolution. The properties of the CGM, which are dependent on a variety of internal and environmental factors, are often inferred from absorption line surveys which rely on a limited number of single lines-of-sight. In this work we present an analysis of 28 galaxy haloes selected from the Auriga project, a cosmological magneto-hydrodynamical zoom-in simulation suite of isolated Milky Way-mass galaxies, to understand the impact of CGM diversity on observational studies. Although the Auriga haloes are selected to populate a narrow range in halo mass, our work demonstrates that the CGM of L⋆ galaxies is extremely diverse: column densities of commonly observed species span ∼3 − 4 dex and their covering fractions range from ${\sim } 5$ to $90{{\ \rm per\ cent}}$. Despite this diversity, we identify the following correlations: 1) the covering fractions (CF) of hydrogen and metals of the Auriga haloes positively correlate with stellar mass, 2) the CF of H i, C iv, and Si ii anticorrelate with active galactic nucleus luminosity due to ionization effects, and 3) the CF of H i, C iv, and Si ii positively correlate with galaxy disc fraction due to outflows populating the CGM with cool and dense gas. The Auriga sample demonstrates striking diversity within the CGM of L⋆ galaxies, which poses a challenge for observations reconstructing CGM characteristics from limited samples, and also indicates that long-term merger assembly history and recent star formation are not the dominant sculptors of the CGM.


1977 ◽  
Vol 74 ◽  
pp. 193-222 ◽  
Author(s):  
A. Boksenberg

In addition to the characteristic emission lines, absorption lines frequently are seen in the spectra of QSOs, usually those with high redshift (zem ≳ 1.8). About 10 percent of all QSOs listed in the compilation of Burbidge et al. (1976a) are recorded as having at least one ‘identified’ absorption system, meaning that a pattern of several selected observed lines can be matched with the apparent wavelengths of transitions (generally from the ground level) in a physical plausible group of atoms or ions at the same, although arbitrary, redshift (Bahcall 1968, Aaronson et al. 1975). Identified absorption line redshifts range from being comparable with the associated emission line redshifts, to having very much smaller values with relative velocities exceeding 0.5c in the QSO frame. Added to this, there are many QSOs having absorption lines not yet recognised as belonging to identified systems, both those objects already having one or more identifications, and others with none.


2003 ◽  
Vol 126 (6) ◽  
pp. 2594-2607 ◽  
Author(s):  
Timothy A. Reichard ◽  
Gordon T. Richards ◽  
Patrick B. Hall ◽  
Donald P. Schneider ◽  
Daniel E. Vanden Berk ◽  
...  

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