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Article

Direct Imaging of a Toroidal Magnetic Field in the Inner Jet of NRAO 150

by
Sol N. Molina
1,*,
Iván Agudo
1,
José L. Gómez
1,
Thomas P. Krichbaum
2,
Iván Martí-Vidal
3 and
Alan L. Roy
2
1
Instituto de Astrofísica de Andalucía, CSIC, Apartado 3004, 18080 Granada, Spain
2
Max-Planck-Institut für Radioastronomie, auf dem Hugel, 69, 53121 Bonn, Germany
3
Department of Earth and Space Sciences, Chalmers University of Technology, Onsala Space Observatory, 43992 Onsala, Sweden
*
Author to whom correspondence should be addressed.
Galaxies 2016, 4(4), 70; https://doi.org/10.3390/galaxies4040070
Submission received: 15 July 2016 / Revised: 15 November 2016 / Accepted: 16 November 2016 / Published: 24 November 2016
(This article belongs to the Special Issue Blazars through Sharp Multi-wavelength Eyes)
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Abstract

:
Most formation models and numerical simulations cause a helical magnetic field to form, accelerate and collimate jets in active galactic nuclei (AGN). For this reason, observational direct evidence for the existence of these helical magnetic fields is of special relevance. In this work, we present ultra- high-resolution observations of the innermost regions of the jet in the quasar NRAO150. We study the polarization structure and report evidence of a helical magnetic field.

1. Introduction

Most formation models and numerical simulations propose a helical magnetic field to form, accelerate and collimate jets in active galactic nuclei (AGN) [1,2,3]. In fact, current models invoke rotation of the accretion disk or black hole ergosphere to create a helical magnetic field [4,5,6].
Despite a variety of observations that provide evidence of helical jet magnetic fields, there has been no previous report of imaging of a polarization structure that appears to directly correspond to the sky projection of a helical magnetic field in the innermost (parsec scale) jet.
Several sources have shown transverse gradients in the observed rotation measure (RM) which suggests that the media that produces the RM gradient has a helical magnetic field structure [7,8,9,10,11,12]. However, these kind of observations have uncertainties related to the difficulty in discriminating whether the Faraday rotating media is internal to the jet emitting region (in which case the helical magnetic field detected is directly related with the magnetic field of the jet) or external.
Moreover, in 3C 454.3 an arc-like feature has been observed with a polarization structure that shows evidence that is compatible with the idea of a helical magnetic field, although for spatial scales of the order of tens of parsecs [13].
Studying the polarization structure with millimeter VLBI can reveal the magnetic configuration in the innermost jet regions. Furthermore, extending polarimetric studies to higher frequencies (above 43 GHz) is important to understand the jet physics near the central black hole in AGN.
The quasar NRAO 150 is a very good candidate to study the structure of the magnetic field. It is a powerful quasar at z = 1.52 [14] and the innermost regions of the jet are oriented within a very small angle to the line of sight [15]. Agudo et al., (2007) [15] measured extremely fast swings of the inner jet structure in the counterclockwise direction at an angular rate of up to ≈ 11 ∘ /year. This angular speed was estimated by assuming that the brightest jet feature in most 43 GHz VLBI images was the core of the jet (called Q0 in this work), therefore assumed to be stationary, and the position of the remaining components were measured with respect to Q0.
Very Long Baseline Interferometry (VLBI) has provided the ultra- high-resolution that is necessary to study the innermost part of the jets. In this work, we have used the Very Long Baseline Array (VLBA) and Global Millimeter VLBI Array (GMVA) images of the total and linearly polarized intensity distributions of NRAO 150 at 22, 43 and 86 GHz.

2. Observations and Data Reduction

We present VLBA observations of the jet in the quasar NRAO 150 at 22 and 43 GHz, between 2008 and 2009. We also show two images taken with the GMVA at 86 GHz between 2009 and 2010. The GMVA is the instrument that provides the best angular resolution from ground telescopes. The initial phase and amplitude calibration of the total flux and polarimetric data was performed with the AIPS software in the usual manner [16].
Analysis of the instrumental polarization at 86 GHz shows that they remain reasonably stable across our observing epochs. Calibration of the electric vector position angle (EVPA) at 22, 43 and 86 GHz was obtained by comparison of the integrated polarization measured from VLBA images for NRAO 150 and three calibrators (BL Lac, DA 193, OJ 287) with VLA observations at contemporaneous epochs at 22 and 43 GHz; and with single-dish polarimetric observations of NRAO 150 obtained by the IRAM 30 m telescope at 86 GHz. Estimated errors of this EVPA calibration lie in the range between 5 ∘ and 10 ∘ .

3. Direct Evidence of a Helical Magnetic Field

Figure 1 and Figure 2 show a sequence of VLBA images at three epochs between 2008 and 2009 of the polarized intensity and EVPA at 22.2 and 43.2 GHz. Figure 3 shows the images at two epochs obtained with the GMVA at 86 GHz. At these high frequencies, the jet is mainly extending in the north–south direction.
At 86 GHz, it is possible to observe the innermost structure of the jet in NRAO 150. The total intensity and polarization structure is fully consistent with the structure observed at lower frequencies, hence confirming the good capabilities of the GMVA to obtain ultra-high-resolution polarization imaging [17].
In jets, the total emission at radio frequencies is produced by synchrotron radiation. Because of that, the degree of linear polarization provides relevant information about the level of order of magnetic fields along the line of sight. In NRAO 150, the degree of linear polarization distribution is variable in time, showing a peak in the northern region (≃14%) during 2009 (Figure 4 and Figure 5). This implies that during this epoch the northern region is dominated by a better ordered field.
Figure 4 and Figure 5 show the magnetic vector position angle (considered perpendicular to the electric vector position angle) distribution during 2009 at 22, 43 and 86 GHz. The assumption that a good representation of the magnetic field may be obtained by the rotation of the EVPA by 90 degrees is supported by the spectral index distribution showed in Figure 6, which shows that the emission is mainly optically thin. In order to obtain the spectral index distribution, we have used two methods to align the images at different frequencies. We have used the cross identification of a particular optically thin emission feature, and the two-dimensional (2D) cross-correlation of the optically thin emission distribution of the source [18,19]. In all cases, we used the restoring beam size of the lower frequency image for every pair of images to be compared. We have found that the two-dimensional (2D) cross-correlation gives us more consistent results than the other method. This is expected, considering that the (2D) cross-correlation takes into account all optically thin emission regions on the entire source, not just a particular feature. The detailed method used for making our spectral index maps was published in [20].
At all frequencies, we observe a magnetic vector position angle configuration that shows a circular geometry. This circular polarization structure has not been observed previously in any other source.
Previous studies of this source found a first approximation of the jet viewing angle ≈8 ∘ , remarking that the extreme jet misalignment between the orientation of the sub-mas scale jet, with respect to the larger scales, implies a very small viewing angle (probably smaller than 8 ∘ ) [15]. Spectral index maps show that there is not a preferential optically thick region that could be assumed as the millimeter core of the jet. Considering this, the circular polarization structure can be interpreted as evidence of the toroidal component of the magnetic field onto the plane of the sky.

Acknowledgments

The research at the IAA-CSIC is supported by the Spanish Ministry of Economy and Competitiveness (MINECO) grant AYA2013-40825-P. I.A. acknowledges support by a Ramón y Cajal grant of MINECO. The VLBA is an instrument of the National Radio Astronomy Observatory, a facility of the National Science Foundation operated under cooperative agreement by Associated Universities, Inc. The GMVA is operated by the MPIfR, IRAM, NRAO, OSO, and MRO.

Author Contributions

The order in the authors list represents the contribution to this work.

Conflicts of Interest

The authors declare no conflict of interest.

References

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Galaxies 04 00070 g001 550
Figure 1. Sequence of three VLBA images at 22 GHz from 2008 to 2009. Contours show the 22 GHz total intensity. Grey scale represents the linearly polarized intensity, and the short white sticks indicate the electric vector position angle distribution. A common convolving beam, as shown in the lower-left corner of the plot, was used for all images. Note that the length of the white sticks is homogeneous over the images, i.e., not proportional to the polarization intensity.
Figure 1. Sequence of three VLBA images at 22 GHz from 2008 to 2009. Contours show the 22 GHz total intensity. Grey scale represents the linearly polarized intensity, and the short white sticks indicate the electric vector position angle distribution. A common convolving beam, as shown in the lower-left corner of the plot, was used for all images. Note that the length of the white sticks is homogeneous over the images, i.e., not proportional to the polarization intensity.
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Figure 2. Sequence of three VLBA images at 43 GHz from 2008 to 2009. Contours show the 43 GHz total intensity. Grey scale represents the linearly polarized intensity, and the short white sticks indicate the electric vector position angle distribution. A common convolving beam, as shown in the lower-left corner of the plot, was used for all images.
Figure 2. Sequence of three VLBA images at 43 GHz from 2008 to 2009. Contours show the 43 GHz total intensity. Grey scale represents the linearly polarized intensity, and the short white sticks indicate the electric vector position angle distribution. A common convolving beam, as shown in the lower-left corner of the plot, was used for all images.
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Figure 3. Sequence of two GMVA images at 86 GHz obtained with GMVA during 2008 and 2009. Contours show total intensity, grey scale represents the linearly polarized intensity, and the short white sticks indicate the electric vector position angle distribution. A common convolving beam, as shown in the lower-left corner of the plot, was used for all images.
Figure 3. Sequence of two GMVA images at 86 GHz obtained with GMVA during 2008 and 2009. Contours show total intensity, grey scale represents the linearly polarized intensity, and the short white sticks indicate the electric vector position angle distribution. A common convolving beam, as shown in the lower-left corner of the plot, was used for all images.
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Figure 4. Linear polarization degree of NRAO 150 as measured with the VLBA at 22 and 43 GHz (left and right, respectively) superposed with the distribution of the magnetic vector position angle during 2009.
Figure 4. Linear polarization degree of NRAO 150 as measured with the VLBA at 22 and 43 GHz (left and right, respectively) superposed with the distribution of the magnetic vector position angle during 2009.
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Figure 5. Linear polarization degree of NRAO 150 as measured at 86 GHz superposed with the distribution of the magnetic vector position angle during 2009.
Figure 5. Linear polarization degree of NRAO 150 as measured at 86 GHz superposed with the distribution of the magnetic vector position angle during 2009.
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Figure 6. Left: The 22 GHz to 43 GHz spectral index distributions overlaid with 22 GHz total intensity contours. Images at the two observing frequencies were convolved with a restoring beam with FWHM 0.33 × 0.25 mas and PA = −6.40 ∘ ; Right: 43 GHz to 86 GHz spectral index distributions overlaid with 43 GHz total intensity contours. Images at the two observing frequencies were convolved with a restoring beam with FWHM 0.17 × 0.123 mas and PA = −14.85 ∘ .
Figure 6. Left: The 22 GHz to 43 GHz spectral index distributions overlaid with 22 GHz total intensity contours. Images at the two observing frequencies were convolved with a restoring beam with FWHM 0.33 × 0.25 mas and PA = −6.40 ∘ ; Right: 43 GHz to 86 GHz spectral index distributions overlaid with 43 GHz total intensity contours. Images at the two observing frequencies were convolved with a restoring beam with FWHM 0.17 × 0.123 mas and PA = −14.85 ∘ .
Galaxies 04 00070 g006

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MDPI and ACS Style

Molina, S.N.; Agudo, I.; Gómez, J.L.; Krichbaum, T.P.; Martí-Vidal, I.; Roy, A.L. Direct Imaging of a Toroidal Magnetic Field in the Inner Jet of NRAO 150. Galaxies 2016, 4, 70. https://doi.org/10.3390/galaxies4040070

AMA Style

Molina SN, Agudo I, Gómez JL, Krichbaum TP, Martí-Vidal I, Roy AL. Direct Imaging of a Toroidal Magnetic Field in the Inner Jet of NRAO 150. Galaxies. 2016; 4(4):70. https://doi.org/10.3390/galaxies4040070

Chicago/Turabian Style

Molina, Sol N., Iván Agudo, José L. Gómez, Thomas P. Krichbaum, Iván Martí-Vidal, and Alan L. Roy. 2016. "Direct Imaging of a Toroidal Magnetic Field in the Inner Jet of NRAO 150" Galaxies 4, no. 4: 70. https://doi.org/10.3390/galaxies4040070

APA Style

Molina, S. N., Agudo, I., Gómez, J. L., Krichbaum, T. P., Martí-Vidal, I., & Roy, A. L. (2016). Direct Imaging of a Toroidal Magnetic Field in the Inner Jet of NRAO 150. Galaxies, 4(4), 70. https://doi.org/10.3390/galaxies4040070

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