BROAD EMISSION LINES Lα, C IV AND Hβ IN NGC 5548

2003 ◽  
Vol 22 (4-5) ◽  
pp. 681-689
Author(s):  
L. S. Nazarova
2004 ◽  
Vol 422 (3) ◽  
pp. 925-940 ◽  
Author(s):  
A. I. Shapovalova ◽  
V. T. Doroshenko ◽  
N. G. Bochkarev ◽  
A. N. Burenkov ◽  
L. Carrasco ◽  
...  

Author(s):  
A.I. SHAPOVALOVA ◽  
V.T. DOROSHENKO ◽  
N.G. BOCHKAREV ◽  
A.N. BURENKOV ◽  
L. CARRASCO ◽  
...  

2018 ◽  
Vol 857 (2) ◽  
pp. 86 ◽  
Author(s):  
Mouyuan Sun ◽  
Yongquan Xue ◽  
Zhenyi Cai ◽  
Hengxiao Guo

2020 ◽  
Vol 898 (2) ◽  
pp. 141 ◽  
Author(s):  
M. Dehghanian ◽  
G. J. Ferland ◽  
G. A. Kriss ◽  
B. M. Peterson ◽  
K. T. Korista ◽  
...  

2021 ◽  
Vol 907 (2) ◽  
pp. 76
Author(s):  
Keith Horne ◽  
G. De Rosa ◽  
B. M. Peterson ◽  
A. J. Barth ◽  
J. Ely ◽  
...  

2006 ◽  
Vol 2 (S238) ◽  
pp. 475-476
Author(s):  
Alexander F. Zakharov

AbstractRecent X-ray observations of microquasars and Seyfert galaxies reveal broad emission lines in their spectra, which can arise in the innermost parts of accretion disks. Recently Müller & Camenzind (2004) classified different types of spectral line shapes and described their origin. Zakharov (2006b) clarified their conclusions about an origin of doubled peaked and double horned line shapes in the framework of a radiating annulus model and discussed s possibility to evaluate black hole parameters analyzing spectral line shapes.


2006 ◽  
pp. 1-11 ◽  
Author(s):  
L.C. Popovic

In this paper a discussion of kinematics and physics of the Broad Line Region (BLR) is given. The possible physical conditions in the BLR and problems in determination of the physical parameters (electron temperature and density) are considered. Moreover, one analyses the geometry of the BLR and the probability that (at least) a fraction of the radiation in the Broad Emission Lines (BELs) originates from a relativistic accretion disk.


2009 ◽  
Vol 5 (S267) ◽  
pp. 398-398
Author(s):  
Patrick B. Hall ◽  
Laura S. Chajet

Murray & Chiang (1997) developed a model wherein broad emission lines come from the optically thick base of a rotating, outwardly accelerating wind at the surface of an accretion disk. Photons preferentially escape radially in such a wind, explaining why broad emission lines are usually single-peaked. Less well understood are the observed shifts of emission-line peaks (from 1000 km s−1 redshifted to 2500 km s−1 blueshifted in C iv, with an average 800 km s−1 blueshift).


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