Linear Polarization Properties of Parsec-Scale AGN Jets ^†

Abstract

We used 15 GHz multi-epoch Very Long Baseline Array (VLBA) polarization sensitive observations of 484 sources within a time interval 1996–2016 from the MOJAVE program, and also from the NRAO data archive. We have analyzed the linear polarization characteristics of the compact core features and regions downstream, and their changes along and across the parsec-scale active galactic nuclei (AGN) jets. We detected a significant increase of fractional polarization with distance from the radio core along the jet as well as towards the jet edges. Compared to quasars, BL Lacs have a higher degree of polarization and exhibit more stable electric vector position angles (EVPAs) in their core features and a better alignment of the EVPAs with the local jet direction. The latter is accompanied by a higher degree of linear polarization, suggesting that compact bright jet features might be strong transverse shocks, which enhance magnetic field regularity by compression.

1. Introduction

Despite substantial progress in the understanding of the phenomenon of the jets of active galactic nuclei (AGN) achieved over the last several decades with the method of very long baseline interferometry (which probes jets from sub- to several hundred parsec scales) the question of how jets are launched, confined and collimated remains an active area of research. The dominant acceleration mechanisms, which could be steady or impulsive in nature, are still unknown. All these questions are expected to be tightly connected with the key agent of jet dynamics, the magnetic (B) field. Construction of the Very Long Baseline Array (VLBA) in 1994 has allowed polarimetric observations of large samples of AGN jets on a regular basis facilitating detailed studies of the polarization characteristics of jet synchrotron radio emission.

VLBA polarization maps provide crucial information on the configuration of the magnetic field associated with an outflow, its regularity and orientation with respect to the local jet direction. In this publication, we analyze the polarization properties of a large sample of AGN jets mainly observed within the MOJAVE program [1] with the VLBA at 15 GHz.

2. Observational Data and the Sample

The data consist of 5410 polarization sensitive VLBA observations of 484 AGNs at 338 individual epochs between 1996 January 19 and 2016 December 26. The sources are drawn from a number of samples: the complete flux density-limited MOJAVE 1.5 sample [2], the joint gamma-ray and radio-selected sample 1FM [3], the VLBA 2 cm survey [4], the MOJAVE low-luminosity sample [5], the 3-rd EGRET gamma-ray catalog [6], and the 3FGL Fermi LAT gamma-ray catalog [7]. Most of the sources (80%) have been detected at high energies by the Fermi LAT instrument [7]. All targets were bright enough ($\underset{\sim }{>}$ 50 mJy) at 15 GHz for direct fringe detection on short integration times. We reduced the data in AIPS software package using standard techniques and performed imaging in Difmap [8].

The overwhelming majority (88%) of the VLBA observations were done within the MOJAVE program [1], while the rest were obtained from the NRAO archive to increase the number of epochs for certain sources. The source cadence in the MOJAVE program is individually determined by the proper motion of jet knots and varies from about a month to two years. The median number of VLBA observation epochs per source is seven, although 54 sources have more than 20 epochs, with a maximum of 133 epochs for BL Lac. Since the beginning of the MOJAVE program in 2002, the noise level of the Stokes Q and U maps improved by a factor of ∼3 and currently reaches a typical value of ∼0.1 mJy beam${}^{-1}$, with a bit rate of 2 Gbps and 2-bit sampling. The corresponding linear polarization and total intensity maps with a more detailed description of image characteristics are available in [9].

The sample is strongly dominated by flat-spectrum radio quasars (71%), with a significant fraction of BL Lacertae objects (20%), and a small fraction of radio galaxies (7%). The rest of the sample (2%) is comprised of optically unidentified sources. The redshifts are currently known for 443 objects (91%), ranging from 0.00436 for the galaxy M87 to 3.636 for the BL Lac object 1549+089 and corresponding to scale factors ranging from 0.01 to 7.35 pc mas${}^{-1}$, respectively. Taking into account that a typical angular resolution of the VLBA observations at 15 GHz is of the order of 1 mas, path lengths along the constructed ridgelines range from 1 to 57 mas and viewing angles are of the order of few degrees for blazars and may reach up to few tens of degrees for radio galaxies [10]. This implies that we probe absolute linear scales from sub- to hectoparsecs of the collimated AGN outflows.

3. Results

For the purposes of our analysis we produced maps of polarized intensity $P={(Q^2+U^2)}^{1/2}$, electric vector position angle $\chi =0.5\mathrm{atan}(U/Q)$, and fractional polarization $m=P/I$, where I is the total intensity. Since the noise in a P image is non-uniform and follows a Ricean distribution, we adopted a conservative approach of estimating the detection limit based on a level at which spurious P signals appear in blank sky region of each map. Typically, this corresponds roughly to a $3\sigma$ level, but in about 16% of the observations it exceeds 5 times $\sigma$ due to a high peak in a total intensity map or high instrumental polarization.

We extracted fractional linear polarization values from the constructed m-maps at the positions of total intensity components that were derived from structure model fitting performed in Difmap. If the polarization intensity of a component was lower than the noise level, we calculated a corresponding upper limit. In Figure 1 we plot the degree of polarization of the jet components of all sources separated by optical classification at all available epochs as a function of distance to the VLBA core. It shows a tendency for fractional polarization to increase with core separation implying that the magnetic field becomes more regular down the jet. Polarization of radio galaxies is weaker, especially for jet components within a few milliarcseconds from the core, with a significantly larger fraction of upper limits (53%) compared to quasars (23%) and BL Lacs (22%).

Figure 1. (a) Fractional polarization at positions of components in total intensity with distance from the 15 GHz core for quasars (black) and BL Lacertae objects (blue). Dots show measurements, while red arrows represent upper limits. (b) Same for radio galaxies.

Core features typically have the highest levels of polarized flux density in the jet but lower fractional linear polarization. The cores, being partially optically thick, have typical degree of polarization on levels of a few per cent in quasars and BL Lacs, while the cores of radio galaxies are weakly polarized, with $m_{\mathrm{core}}<0.5$% (Figure 2). Low- and intermediate SED peak BL Lacs have the most highly polarized cores. In only 30 out of 5410 total epochs $m_{\mathrm{core}}>10$%. Both core and jet components of BL Lacs, on average, are more polarized than those of quasars.

Figure 2. (a) Histograms of fractional polarization of core (filled gray bins) and jet components (empty bins) for quasars, (b) for BL Lacs, (c) for radio galaxies.

We have also found that roughly 40% of the AGN jet cores show a tendency for a preferred EVPA direction over time. BL Lac cores have more stable EVPAs than those of quasars and show a tendency to be aligned with the inner parsec-scale jet. Similar behaviour is detected for the EVPA of jet components of BL Lacertae objects, which tend to be aligned with the local jet direction. In contrast, quasars and radio galaxies do not show such a trend. This confirms the findings of earlier studies, e.g., [11,12]. In many BL Lacs, high degrees of polarization are associated with low deviations of EVPAs from the jet direction (Figure 3).

Figure 3. (a) Negative correlation between degree of polarization of total intensity components and absolute deviation of the electric vector position angles (EVPA) from the local jet direction for BL Lac object 0823+033. (b) Same for BL Lac.

Fractional polarization maps taken within our program, and also in individual source studies, e.g., [13], often manifest clear increase of m-values towards the jet edges. To analyze changes in degree of polarization across the jet, we constructed jet ridgelines in total intensity following the procedure described in [10], and made m-slices transverse to the local jet direction. In Figure 4 we present examples of two sources, the radio galaxy 0430+052 and quasar 1150+812, that reveal rich polarization structure at 15 GHz and have many epochs of observations. The sources show a characteristic V-shaped profile in the m-cuts (where the x-axis is a measure of offset from the ridgeline of the jet in units of restoring beams). Closer to the jet edges, the degree of polarization increases up to a few tens of per cent. Many other sources show similar tendency suggesting that this effect is quite common.

Figure 4. (a) Fractional polarization from slices transverse to the local jet direction as a function of offset from total intensity ridgeline for the radio galaxy 3C 120 (0430+052). Black, cyan and blue dots show measurements at distances $r<1$ mas, $1<r<3$ mas, and $r>3$ mas from the 15 GHz core measured along ridgeline, respectively. (b) Same for the quasar 1151+812.

4. Discussion

Since a jet expands with distance, magnetic field decreases as $B\propto r^{-b}$ ($b=1$ for a pure toroidal field, $b=2$ for a pure axial field) but becomes more regular, as is evident from the observed increase in fractional polarization. One possible explanation of this trend is that magnetohydrodinamic turbulence is expected to decrease with distance from relativistic shocks and also down the jet [14]. The observed increase of the degree of polarization towards the jet edges is likely due to the superposition of synchrotron emission from regions with different magnetic field orientations resulting in depolarization, which is more efficient closer to the jet axis and weaker to the edges, where the emission layer is thinner.

The VLBA core features have a degree of polarization within 10% implying that synchrotron radiation from these regions is optically thick, while it is optically thin in the jet as $m_{\mathrm{jet}}$ often exceeds this limit. In BL Lacs, the observed increase in alignment of EVPA with jet direction (perpendicular B-field) accompanied by a higher fractional polarization suggests that the bright jet components might be shock fronts that enhance magnetic field orderliness by compression. Alternatively, it may be interpreted in terms of a toroidal component of a large-scale helical B-field associated with the jet, though this scenario faces difficulties explaining inverse dependence between $|\mathrm{EVPA}-\mathrm{jet}\mathrm{PA}|$ and m detected in BL Lacs.