scholarly journals The luminosity function of TeV-emitting BL Lacs: observations of an HBL sample with VERITAS

2021 ◽  
Author(s):  
Manel Errando ◽  
Veritas Collaboration
Keyword(s):  
1986 ◽  
Vol 119 ◽  
pp. 491-492
Author(s):  
A. Cavaliere ◽  
E. Giallongo ◽  
F. Vagnetti

If the BL Lac Objects are active nuclei with a beamed component that is dominant when directed at us, their observed luminosity function must comprise a flat faint branch: N(L)dL ∝ L1+1/pdL with p=4.5 (Urry and Shafer 1984). If this is flatter than the LF NP(L) of the parent objects at equal observed L, then we expect the counts of BL Lacs to flatten out in turn at fluxes quite higher than the counts of the parents, even when both populations evolve strongly and uniformly with comparable timescales (Cavaliere, Giallongo and Vagnetti 1985).


1983 ◽  
Vol 104 ◽  
pp. 347-347
Author(s):  
C. Megan Urry ◽  
Richard F. Mushotzky ◽  
Allyn F. Tennant ◽  
Elihu A. Boldt ◽  
Stephen S. Holt

HEAO 1 A2 and Einstein SSS spectral observations of Seyfert galaxies and BL Lac objects suggest that in both cases, the X-ray emission is due to relativistic particles. The five BL Lac objects have very soft spectra and at higher energies (above 10 keV) may have hard tails. Combining our X-ray data with radio, infrared, optical, and ultraviolet observations, we can fit the BL Lac spectra with the familiar synchrotron self-Compton model if we allow for relativistic beaming (Urry and Mushotzky 1982, Urry et al. 1982). We show that Doppler beaming of an underlying (Seyfert-like) source population flattens the observed luminosity function, and we emphasize that the relative numbers of BL Lacs and quasars in given spectral intervals are strong functions of selection effects, the degree of Doppler beaming, and the form of the intrinsic luminosity function.


2019 ◽  
Vol 490 (1) ◽  
pp. 758-765
Author(s):  
Yankun Qu ◽  
Houdun Zeng ◽  
Dahai Yan

ABSTRACT Using a significantly enlarged Fermi-LAT BL Lac objects (BL Lacs) sample, we construct the gamma-ray luminosity function (GLF) of BL Lacs, by the joint use of the space density distribution and source counts distribution. We use three well-studied forms of the GLF, i.e. the forms of pure density evolution (PDE), pure luminosity evolution (PLE), and luminosity-dependent density evolution (LDDE). The Markov Chain Monte Carlo (MCMC) technique is used to constrain model parameters. Our results suggest that LDDE model can give the best description for the BL Lac GLF. And the model shows that the BL Lacs with a harder GeV spectrum and a less luminosity evolve as strongly as flat spectrum radio quasars, and the evolution decreases as increasing luminosity. We also model the average photon spectra of BL Lacs with a double power-laws model. Using this modelled spectra, BL Lacs contribute $\sim \!20{{\ \rm per\ cent}}$ of the total extragalactic gamma-ray background (EGB) at E > 100 MeV, $\sim \!100{{\ \rm per\ cent}}$ of the EGB at E > 50 GeV, and the unresolved BL Lacs contribute $\sim\! 20 {{\ \rm per\ cent}}$ of the isotropic diffuse gamma-ray background at E > 100 MeV. A prediction of the TeV EGB spectra are given, which may be tested by the future detectors.


2012 ◽  
Vol 2 (7) ◽  
pp. 15-18
Author(s):  
Mariwan A. Rasheed ◽  
◽  
Mohamad A. Brza

1998 ◽  
Vol 116 (3) ◽  
pp. 1118-1124 ◽  
Author(s):  
Roberto De Propris ◽  
Christopher J. Pritchet

2000 ◽  
Vol 119 (6) ◽  
pp. 2540-2555 ◽  
Author(s):  
A. Grazian ◽  
S. Cristiani ◽  
V. D’Odorico ◽  
A. Omizzolo ◽  
A. Pizzella
Keyword(s):  

1997 ◽  
Vol 476 (1) ◽  
pp. 144-165 ◽  
Author(s):  
Christopher F. McKee ◽  
Jonathan P. Williams

1997 ◽  
Vol 180 ◽  
pp. 475-476
Author(s):  
M. G. Richer ◽  
G. Stasińska ◽  
M. L. McCall

We have obtained spectra of 28 planetary nebulae in the bulge of M31 using the MOS spectrograph at the Canada-France-Hawaii Telescope. Typically, we observed the [O II] λ3727 to He I λ5876 wavelength region at a resolution of approximately 1.6 å/pixel. For 19 of the 21 planetary nebulae whose [OIII]λ5007 luminosities are within 1 mag of the peak of the planetary nebula luminosity function, our oxygen abundances are based upon a measured [OIII]λ4363 intensity, so they are based upon a measured electron temperature. The oxygen abundances cover a wide range, 7.85 dex < 12 + log(O/H) < 9.09 dex, but the mean abundance is surprisingly low, 12 + log(O/H)–8.64 ± 0.32 dex, i.e., roughly half the solar value (Anders & Grevesse 1989). The distribution of oxygen abundances is shown in Figure 1, where the ordinate indicates the number of planetary nebulae with abundances within ±0.1 dex of any point on the x-axis. The dashed line indicates the mean abundance, and the dotted lines indicate the ±1 σ points. The shape of this abundance distribution seems to indicate that the bulge of M31 does not contain a large population of bright, oxygen-rich planetary nebulae. This is a surprising result, for various population synthesis studies (e.g., Bica et al. 1990) have found a mean stellar metallicity approximately 0.2 dex above solar. This 0.5 dex discrepancy leads one to question whether the mean stellar metallicity is as high as the population synthesis results indicate or if such metal-rich stars produce bright planetary nebulae at all. This could be a clue concerning the mechanism responsible for the variation in the number of bright planetary nebulae observed per unit luminosity in different galaxies (e.g., Hui et al. 1993).


2018 ◽  
Vol 867 (1) ◽  
pp. 46 ◽  
Author(s):  
Ryohei Itoh ◽  
Masami Ouchi ◽  
Haibin Zhang ◽  
Akio K. Inoue ◽  
Ken Mawatari ◽  
...  

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