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Introduction
Active Galactic Nuclei are objects in the universe that
have been observed to emit enormous amounts of energy. One of these objects
can emit 10 million times the energy of a passive galaxy such as the Milky
Way. Active Galactic Nuclei form around supermassive black holes, which
have extremely powerful gravitational fields that draw matter into an
accretion disk surrounding the black holes. The two types of active galaxies
included in this study are BL Lacs and quasars. BL Lacs are observed at
a low beaming angle, typically less than 10 degrees, Quasars are galaxies
that are observed at the same beaming angle as BL Lacs but which are much
more energetic. This paper will discuss three BL Lac objects and one quasar.
Active
Galactic Nuclei are active in the radio wave portion of the electromagnetic
spectrum. They are observed on a milliarcsecond resolution. In order to
achieve a resolution this high, radio astronomers use the Very Long Baseline
Array (VLBA). The VLBA is an interferometer that correlates data received
from telescopes stationed across North America to create radio images
on a milliarcsecond scale. These images are turned into contour maps showing
areas of brightest intensity.
Images
of Active Galactic Nuclei often reveal jets composed of hot plasma radiating
outward from their core. Many of these jets demonstrate a Kelvin-Helmholtz
instability. This is an effect occurring when two fluids with different
velocities move against each other, causing the fluids to deviate from
a linear path. As a result of the Kelvin-Helmholtz instability, the jets
emanating from Active Galactic Nuclei are often observed to take a helical
structure, where the jets fit a continually expanding sinusoidal pattern.
Radio astronomers still know relatively little about the kinematics of
these helical jets and are endeavoring to find a model that fits the observed
astronomical data. One such model has already been proposed (Hardee, 78).
Observations over time have revealed shocks moving along the jets of certain
Active Galactic Nuclei. It is the movement of these shocks that has been
the focus of this summer research project.
Observations
We have generated contour maps of the Active Galactic Nuclei
of interest using data received from the VLBA. The maps we were able to
generate are as follows (Table 1):
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Source
1749 + 096 |
| Epoch |
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| August 2001 |
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22.4 |
| January 2002 |
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22.4 |
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Source
1823 + 568 |
| Epoch |
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| January 2002 |
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15.4,22.4,43 |
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Source
BL Lac |
| Epoch |
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| August 2001 |
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15.4,22.4 |
| January 2002 |
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15.4,22.4,43 |
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Source
2134 + 004 |
| Epoch |
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| January 2002 |
|
15.4,22.4,43 |
Table
1: Observations Data
The contour maps produced from the VLBA data appear as follows
(Figures 1-13):
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Figure
1: 1749 +096, August 2001, 22.4 MHz
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Figure
2: 1749 +096, January 2002, 22.4 MHz
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Figure
3: 1823 +568, January 2002, 15.4 MHz
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Figure
4: 1823 +568, January 2002, 22.4 MHz
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Figure
5: 1823 +568, January 2002, 43 MHz
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Figure 6: BL Lac, August 2001, 15.4 MHz
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Figure
7: BL Lac, August 2001, 22.4 MHz
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Figure
8: BL Lac, January 2002, 15.4 MHz
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Figure 9: BL Lac, January 2002, 22.4 MHz
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Figure
10: BL Lac, January 2002, 43 MHz
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Figure 11: 2134 +004, January 2002, 15.4 MHz
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Figure 12: 2134 +004, January 2002, 22.4 MHz
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Figure 13:
2134 +004, January 2002, 43 MHz
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Analysis
The goal of
this research was to create a helical model for the motion of shocks along
the jets of the four Active Galactic Nuclei 1749 +096, 1823 +568, BL Lac,
and 2134 +004. A helix is characterized by a set of helical parameters.
We varied six of these parameters in an attempt to find the best possible
match. The parameters are as follows: ro represents the opening radius
of the helix, lo represents the initial wavelength of the helix, y represents
the opening angle of the helix, x represents the angle that the helix
forms with the sky coordinate North, f represents the starting point of
the helix, and q represents the angle between the axis of the helix and
the line of sight. Each parameter was tested within a specific range;
we tested ro from .05 to .20, lo from 0.1 to 10.0, y from 1.0 to 4.0,
x from 175.0 to 183.0 for the object BL Lac and from 265.0 to 273.0 for
source 2134 +004, f from 0.0 to 360.0, and q from 4.0 to 10.0. We performed
a reduced chi-squared test on each combination of parameters to determine
the fitness of the overall helix. Our desired value for reduced chi-squared
was one.
The
contour maps revealed the BL Lac object 1749 +096 to be a point source
(Figures 1 - 2). No jets appeared emanating from the core of this active
galaxy, and thus there were no data to model. We did no further analysis
on this object.
The BL Lac object 1823 +568 also had insufficient data to analyze (Figures
3-5). The contour map of this object produced in January 2002 at 15.4
MHz (Figure 3) suggests the beginning of a jet. However, this jet does
not appear in the other maps of 1823 +568 (Figures 4-5). More data needs
to be collected on this object before it is apparent whether or not a
jet exists. We performed no further analysis on this object.
The BL Lac
object BL Lac (Figures 6-10) shows evidence of a helical jet emanating
from the core. As we have observed this object over time, we have seen
a series of shocks move along this jet. These shocks appear on the contour
maps as areas of brighter intensity. The shock that appears in the BL
Lac contour maps from August 2001 and January 2002 is called S11. We have
combined the data from these two maps with previously generated data to
fit a helical model to shock S11 on the object BL Lac. When only considering
the data available through August 2001, we were able to find a suitable
helical model (Figure 14).
Figure
14: A proposed helical model for shock S11 using data through August 2001.
This
helix has the following helical parameters: ro =.05, lo =1.9, y =3.2,
x =183.0,
f =240.0, and q = 9.0. The reduced chi-squared value for this helix is
.05. This is less than the value of 1 that we set as our limit for reduced
chi-squared, which indicates this helix is a good model of the data. However,
when we added in data from January 2002, it became apparent that this
helix did not sufficiently describe the observed data. We attempted to
find a helical model that would account for the observations taken in
January 2002 (Figure 15).

Figure 15:
A proposed helical model for shock S11 using data through January 2002.
This
model has the following helical parameters: ro =.11, lo =5.3, y =2.3,
x =180.2, f =208.0, and q = 6.6. When we performed the reduced chi-squared
test on this helix, we arrived at a value of 4.304 for reduced chi-squared.
This value did not meet our qualification of being close to one, and thus
we concluded that this helical model did not accurately fit our data.
We have been unable to find a better helical model for shock S11 of the
object BL Lac.
Quasar
2134 +004 did not show evidence of a jet emanating from the core (Figures
11-13). However, we noticed that the contour maps revealed an overall
helical shape to the quasar. We endeavored to model the shape of 2134
+004 (Figure 16).

Figure 16:
A helical model of quasar 2134 +004
This
model has the following helical parameters: ro =.10, lo =3.7, y =3.8,
x =280.0, f =130.0, and q = 8.5. The reduced chi-squared value for this
helix is 1.06, which is significantly close to our desired value of 1.0.
Thus, we concluded that this model fit the data well and accurately describes
the shape of quasar 2134 +004.
Conclusion
Through analyzing
contour maps created using the VLBA, we were able to propose new models
to describe the motion of active galactic nuclei. We were unable to analyze
two sources we observed, 1749 +096 and 1823 +568. We analyzed the source
BL Lac, but were not able to find an accurate model. Our greatest success
was with the source 2134 +004, for which we were able to propose a helical
model that accurately describes the observed data.
For
future research, we hope to find a helical model that more accurately
describes shock S11 for the object BL Lac. We will also continue observing
source 1823 +568 in hopes of finding a jet emanating from its core, at
which time we will attempt to fit a helical model to this jet.
Works Cited
Hardee, P.E.,
(1987), "Spatial Stability of Relativistic Jets - Application to
3C345" Astrophysical Journal, 318, 78.

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This page updated February
27, 2004
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