Issue |
A&A
Volume 517, July 2010
|
|
---|---|---|
Article Number | A63 | |
Number of page(s) | 4 | |
Section | Extragalactic astronomy | |
DOI | https://doi.org/10.1051/0004-6361/200913497 | |
Published online | 06 August 2010 |
Colour behaviour of the blazar PKS 0735+178 in 1994-2004
(Research Note)
L. O. Takalo1 - V. A. Hagen-Thorn2,3 - E. I. Hagen-Thorn2,3,4 - S. Ciprini5 - A. Sillanpää1
1 - Tuorla Observatory, Dept. of Physics and Astronomy, University of Turku, Väisäläntie 20, 21500 Piikkiö, Finland
2 -
Astronomical Institute, St.-Petersburg State University, Universitetsky pr. 28, Petrodvoretz, St.-Petersburg 198504, Russia
3 -
Isaac Newton Institute of Chile, St.-Petersburg Branch, Russia
4 -
Main (Pulkovo) Astronomical Observatory of RAS, St.-Petersburg, Russia
5 -
Osservatorio Astronomico, Universita di Perugia, via B. Bonfigli, 06126 Perugia, Italy
Received 19 October 2009 / Accepted 21 April 2010
Abstract
Context. The properties of variable sources responsible for
blazar activity are still under discussion. Some conclusions can be
drawn from analyzing monitoring observations.
Aims. The results of multicolour monitoring observations of the
blazar PKS 0735+178 are used to study the colour behaviour of the
variable source responsible for the blazar activity in 1994-2004.
Methods. The method of ``flux-flux'' diagrams is used to find the SED of the variable source.
Results. The SED of the variable source was unchanged on
timescales of years and is represented well by a power-law. High
observed polarization and power-law spectrum point to the synchrotron
nature of the variable source. The achromatic variability can then be
explained by variations in the Doppler boosting due to
-variations in the angle between the line of sight and the velocity direction of the radiating source.
Conclusions. There is no doubt about the synchrotron nature of
the variable source. The most probable reason for this variability is
the change in the Doppler boosting.
Key words: BL Lacertae objects: general - BL Lacertae objects: individual: PKS 0735+178 - techniques: photometric
1 Introduction
This article is devoted to studying the colour behaviour of the blazar
PKS 0735+178 in optical wavelengths. The source was optically
identified from the PKS radio catalogue by Blake (1970) and classified as a BL Lac object by Carswell et al. (1974).
The absence of emission lines in its spectrum does not allow any determination of its redshift z, but an absorption feature identified with Mg II line gives an estimation of
.
This object has been studied in all spectral regions from radio to
.
A good review of papers devoted to it is given by Ciprini et al. (2007,
Paper I) and will not be repeated here. Let us only point out that
the object is photometrically active, and its optical variability
amplitude is as high as
(Fan et al. 1997).
For clarifying the nature of the active sources responsible for blazar variability, we need to find the spectral energy distribution (SED) of these sources. But the separation of source radiation from the total observed flux, which includes the radiation of the host galaxy, accretion disk, etc., is not a simple task because the contributions of these components can only be found indirectly (if at all). In some cases, however, the relative SED of the variable source can be found from multicolour photometric monitoring data without any preliminary separation of the contribution of the components (Hagen-Thorn & Marchenko 1999). Results of such a monitoring of PKS 0735+178 are given in Paper I, and are used in this investigation.
2 Observational data and results of their analysis
The light curves of PKS 0735+178 in B,V,R,I
bands given in Paper I cover the 11-year time interval 1994-2004.
They are constructed using CCD-data obtained at 5 observatories with
relatively small telescopes; therefore, on average, the errors of
individual brightness estimations are as high as
for B,
for V,
for R, and
for I.
With such high errors in magnitudes the individual estimations of
colour-indexes are very unreliable. Moreover, because of relatively
small flux variability on short timescales, these errors prevent colour
variability investigations on less than
year timescales. Only long-term (years) colour behaviour of the source can be studied.
We used the method of colour variability analysis, described in detail in Hagen-Thorn & Marchenko (1999) and repeatedly tested in blazar investigations (for instance, Hagen-Thorn et al. 2008, 2009).
The method is based on comparing quasi-simultaneous estimations of flux
densities (below ``fluxes'') in the used spectral bands. If the
photometric behaviour of the object during a given time interval is
defined by a single variable source with varying flux density but
unchanged SED, then in ``flux-flux'' diagrams (Fi vs. Fj)
the points presenting simultaneous observations must lie on a straight
line. With some caveats, the opposite is also true. If the points on
``flux-flux'' diagrams lie on straight lines, conclusion may be drawn
about the constancy of the SED of the variable source responsible for
the variability in the time interval considered, and the slopes of the
lines are the flux ratios of the variable source in corresponding bands
.
In other words, the relative SED of the variable source has been found
in the spectral range determined by these used bands. We stress that
this SED is found directly from observational data without knowledge of the contribution of the variable component to the total observed radiation.
The magnitudes from Paper I were transformed to fluxes using the absolute calibration by Mead et al. (1990). Then, if there were several observations on some Julian Date, the mean values for fluxes in each band were calculated (thus, we ignore a possible fast variability within the night-IDV). But more often we found only one observation per night.
The obtained light curves are shown in Fig. 1, where the vertical segments give doubled mean errors. There is a trend in the light curves: before JD 2 450 700 the flux decreased on average (event 1), and after this date a flux increase is seen, which might point to the appearance of a new variable source with other colour characteristics (event 2).
![]() |
Figure 1: The light curves after averaging within JD. |
Open with DEXTER |
![]() |
Figure 2:
Flux-flux diagram FB vs. FR. Cross gives the mean error at the 1 |
Open with DEXTER |
The ``flux-flux'' diagrams are shown in Figs. 2-4. The R
band, in which most observations were carried out, was chosen as the
base one. In all figures, the filled circles show the data for the
event 1, the open circles for the event 2. One can see that
the points lie along straight lines and that there are no systematic
differences between the positions of both symbol types. (This is
confirmed by the data of Cols. 5 and 6 of Table 1: there are no differences at 2
level.) Though the data for fading part in event 2 are incomplete,
the behaviour on rising and fading parts of the light curve seems to be
the same. The slopes of dependences FI vs. FR are the same (
and
).
Thus, the colour characteristics of the variable component were
unchanged during all eleven years. The straight lines in Figs. 2-4 (for all the data) were calculated by the orthogonal regression method.
![]() |
Figure 3:
Flux-flux diagram FV vs. FR. Cross gives the mean error at the 1 |
Open with DEXTER |
![]() |
Figure 4:
Flux-flux diagram FI vs. FR. Cross gives the mean error at the 1 |
Open with DEXTER |
Table 1: The results of determination of the relative SED of the variable source.
The slopes of these lines and their errors are given in Table 1 in the fourth column. (In previous columns the spectral band, corresponding logarithm of the frequency, and correlation coefficient between fluxes with its error are given.) The data in the fourth column give the observed relative SED of the variable component responsible for the long-term variability.
This SED must be corrected for reddening due to light absorption in our Galaxy. This may be done by multiplying the data of Col. 4 by the factor CiR = 100.4(Ai - AR) (Ai according to the NED). The seventh column gives the relative SED of the variable source corrected for Galactic absorption. In the eighth column this is shown on a logarithmic scale.
Results of determining the relative SED of the variable source are shown in Fig. 5 (for R band log
). It is seen that the points lie along a straight line quite well, showing a power-law spectrum
.
The straight line is calculated by the least-squares method with the
errors taken into account. The result gives the spectral index
.
![]() |
Figure 5: The spectrum of the variable source. |
Open with DEXTER |
3 Discussion
Power-law spectrum and observed high polarization (20%, e.g. Mead et al. 1990)
point to the synchrotron nature of the variable source. Paper I is
devoted, in principle, to searching for periodic components in the
light curve of PKS 0735+178; however, it contains a part devoted to
analysing of colour variability (see Fig. 5
in Paper I). The authors used another method for the analysis than
here. They suggest that all the observed flux is radiated by the
variable component and find spectral indexes for individual
observations suggesting a power-law spectrum. The mean value of the
spectral index
found by them agree with our value. They affirm that light variability
is achromatic on the time-scales of years (we agree with this), but in
individual events colour variability possibly exist. We stress that our
observational data do not permit us to state anything about colour
variability on the shorter time-scales (days/weeks). This is evident if
we compare the scatter of the points relative to the straight lines in
Figs. 2-4 with the 1
errors shown in the figures by crosses. The whole scatter of the points
relative to the straight lines may be attributed to accidental errors,
and the flux variability can be explained if the variable source does
not change its SED.
The colour characteristics of the variable source may be
different on different time intervals. Thus, from the PKS 0735+178
observations in 1982-84 published by Sitko et al. (1985) and Smith et al. (1987), a variable source with spectral index
was found by Hagen-Thorn et al. (1990) when applying the same method as used here. A variable source with
can be found from the data published by Mead et al. (1990)
for observations carried out in 1988. This means that, at different
time intervals, the energy distribution in the assembly of relativistic
electrons responsible for synchrotron radiation may be different.
The constancy of the spectral shape of the variable component
excludes all variability mechanisms, resulting in a change in SED (for
instance, fading because of synchrotron losses). For synchrotron
sources, achromatic variability is best explained by the change in the
relativistic boosting of the flux due to variation in the
Doppler-factor
,
which is caused by the change in the angle between the line of sight and velocity direction of the moving source
.
The movement of the superluminal component in the radio jet of PKS 0735+178 gives a Lorentz-factor
between 2 and 4 (Agudo et al. 2006). If we accept
,
then we get
for the velocity of the source. The ratio of fluxes in maximum and minimum brightness (see Fig. 1) is
.
For
,
the corresponding ratio of the Doppler-factors will be
.
Keeping in mind that
,
we suggest
and find a lower limit for the angle at minimum
and
.
For a more realistic value
,
it will be
and
.
Evidently, these estimations are valid only for time interval 1994-2004.
4 Conclusions
Thus, the results of the colour behaviour investigation of blazar PKS 0735+178 based on the 11-year (1994-2004) four-colour (B,V,R,I) photometric monitoring can be summarised as follows.
Long-term (years) variability in optical wavelengths is caused by the
flux variations in the source with unchanged relative SED. This SED is
represented well by a power-law spectrum, which is a property of a
homogenous synchrotron source
.
The synchrotron nature of the variable source is confirmed by the high polarization observed in PKS 0735+178.
Most probably, the achromatic variability stems from a change in the
Doppler-factor within limits of 3 to 5, which is caused by about a
change between the line of sight and velocity direction of the moving source.
This work was supported by RFBR grant No. 09-02-00092. V.A. and E.I.H.-Th. thank Tuorla Observatory for hospitality.
References
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All Tables
Table 1: The results of determination of the relative SED of the variable source.
All Figures
![]() |
Figure 1: The light curves after averaging within JD. |
Open with DEXTER | |
In the text |
![]() |
Figure 2:
Flux-flux diagram FB vs. FR. Cross gives the mean error at the 1 |
Open with DEXTER | |
In the text |
![]() |
Figure 3:
Flux-flux diagram FV vs. FR. Cross gives the mean error at the 1 |
Open with DEXTER | |
In the text |
![]() |
Figure 4:
Flux-flux diagram FI vs. FR. Cross gives the mean error at the 1 |
Open with DEXTER | |
In the text |
![]() |
Figure 5: The spectrum of the variable source. |
Open with DEXTER | |
In the text |
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