Proper Motions of Jets on the Kiloparsec Scale: New Results with HST

TL;DR

This study uses 20-year HST observations to measure the proper motions of kiloparsec-scale optical jets, revealing velocity profiles and deceleration patterns from near the black hole outward.

Contribution

First to measure proper motions of kiloparsec-scale optical jets with high precision, linking parsec and kiloparsec scale velocities for a comprehensive jet profile.

Findings

Jets in FR I galaxies accelerate up to 100 pc from the core.

Proper motions indicate jet deceleration beyond 100 pc.

Velocity profiles connect near the black hole to large-scale jet behavior.

Abstract

The Hubble Space Telescope recently celebrated 25 years of operation. Some of the first images of extragalactic optical jets were taken by HST in the mid-1990s; with time baselines on the order of 20 years and state-of-the-art astrometry techniques, we are now able to reach accuracies in proper-motion measurements on the order of a tenth of a milliarcsecond per year. We present the results of a recent HST program to measure the kiloparsec-scale proper motions of eleven nearby optical jets with Hubble, the first sample of its kind. When paired with VLBI proper-motion measurements on the parsec scale, we are now able to map the full velocity profile of these jets from near the black hole to the final deceleration as they extend out into and beyond the host galaxy. We see convincing evidence that weak-flavor jets (i.e., FR Is) have a slowly increasing jet speed up to 100 pc from the core, where superluminal components are first seen.

Figures

Full text

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8 \doinum10.3390/galaxies5010008 \pubvolume5

\externaleditorAcademic Editors: Jose L. Gómez, Alan P. Marscher and Svetlana G. Jorstad \historyReceived: 13 September 2016; Accepted: 16 January 2017; Published: date \TitleProper Motions of Jets on the Kiloparsec Scale: New Results with HST \AuthorEileen T. Meyer *1,**, William B. Sparks 2, Markos Georganopoulos 1, Roeland van der Marel 2, Jay Anderson 2, Sangmo T. Sohn 2, John Biretta 2, Colin Norman 2, Marco Chiaberge 2 and Eric Perlman 3 \AuthorNamesEileen Meyer, William Sparks, Markos Georganopoulos, Roeland van der Marle, Jay Anderson, Sangmo Sohn, John Biretta, Colin Norman, Marco Chiaberge, Eric Perlman

\corresCorrespondence: meyer@umbc.edu

1 Introduction

Many aspects of the physics of relativistic jets from super-massive black holes are not well understood, including the particle makeup of the jet, their lifetimes, and the speed profile of the plasma as it extends out of the host galaxy and into the intergalactic medium. Proper-motion studies allow us to directly observe the apparent speeds of these jets, resulting in constraints on their Lorentz factors ($\Gamma$). Hundreds of observations of jets with very long baseline interferometry (VLBI) in the radio have detected proper motions of jets on parsec and sub-parsec scales, relatively near to the black hole engine (e.g., giovannini2001 ; piner2004 ; kellermann2004 ; jorstad2005 ; lister2009 ). Because these jets are highly relativistic, apparent superluminal motions can result from velocities near the speed of light coupled with relatively small viewing angles. We start with some definitions: the dimensionless observed apparent velocity $\beta_{\mathrm{app}}$ is related to the real velocity $\beta=v/c$ (where $c$ is the speed of light) and viewing angle $\theta$ through the well-known Doppler formula $\beta_{\mathrm{app}}=\beta\sin\theta/(1-\beta\cos\theta)$. A measurement of $\beta_{\mathrm{app}}$ implies both a lower limit on the Lorentz factor ($\Gamma_{\mathrm{min}}\approx\beta_{\mathrm{app}}$) and an upper limit on the viewing angle. These constraints are difficult to derive using other means such as spectral fitting, due to the inherent degeneracy between intrinsic power, angle, and speed introduced by Doppler boosting of the observed flux.

While there are large samples of proper-motion measurements for jets on parsec scales, direct observations of jet motions on much larger scales (kpc–Mpc) with high-resolution telescopes such as the Very Large Array (VLA) or Hubble Space Telescope (HST) are rare. However, the much lower-than-VLBI resolution necessarily also limits potential observations of apparent motions to sources in the very local Universe, and often require years or even decades of repeated observations. For many years, there were only two measured proper motions of jets on kpc scales, both taken with the VLA. These were the famous result of $\beta_{\mathrm{app}}$ up to $6c$ measured by biretta1995 for the jet in M87 (z = 0.004, d = 22 Mpc), and a speed of $\approx$4$c$ for a knot in the jet in 3C 120 (z = 0.033, d = 130 Mpc) by walker1988 , though this was later contradicted by additional VLA and Merlin observations (muxlow1991, ; walker1997, ). In 1999, the first measurement of proper motions in the optical was accomplished by biretta1999 , using four years of HST Faint Object Camera (FOC) imaging to confirm the fast superluminal speeds in the inner jet of M87. In this paper, we present some recent proper-motions results for three nearby optical jets obtained from archival and new HST data, enabled in major part by the long operating lifetime of HST and the resulting 20-year baselines from the original snapshot images of optical jets first taken in the 1990s.

2 Methods

All three optical jets were observed with several of the Hubble Space Telescope imaging instruments over a span of 10–20 years. The analysis of the new and archival data was similar for all three jets. We will present first the methods for the jet in M87, and then briefly remark on the data used for 3C 264 and 3C 273, which was treated very similarly. The data used for all jets and further details can be found in mey13_m87 ; mey15_nature ; mey16_3c273 .

2.1 M87

2.1.1 Astrometry

For M87, the reference frame is based on hundreds of bright globular clusters associated with the host galaxy which are effectively stationary to proper motions over the time of this study. The reference frame was built using the Advanced Camera for Surveys Wide Field Camera (ACS/WFC) exposures in the F606W filter, by first detecting the positions of the globular clusters in each flat-fielded, CTE-corrected ACS/WFC image using a PSF-peak-fitting routine, then applying the standard (filter-specific) geometric correction to those positions, and then finding the best linear transformation for each image which matches the positions in the individual (geometrically-corrected) frames to a master reference frame. This last step is done by a routine similar to MultiDrizzle, but better optimized for astrometry (see and10 ; sohn12 ). The process of finding transformations for all frames is iterated so that the master reference frame (super-sampled to a pixel scale of 0.025*′′*/pixel) effectively gives the average position of each reference source in a geometrically-corrected frame.

The final reference system consists of positions and magnitudes for over 1300 globular clusters within $\sim$100*′′* of the M87 core position. Among all clusters, the median one-dimensional RMS residual relative to the mean position was 0.05 (reference-frame) pixels (1.25 mas), corresponding to a systematic astrometric accuracy ($\times$ 1/$\sqrt{5}6$) of 0.17 mas; over the 13.25 year baseline this is equivalent to 0.003$c$. Astrometric solutions were then found for all the ACS High Resolution Camera (ACS/HRC), ACS/WFC, and Wide Field Planetary Camera 2 (WFPC2) images in the F814W filter. Typical numbers of globular clusters used to match the frames were $\sim$200–500 for ACS/WFC, $\sim$15–30 for WFPC2 images, and $\sim$15–25 for ACS/HRC; corresponding systematic errors were $\sim$0.006, $\sim$0.03, and $\sim$0.05 pixels, or 0.003$c$, 0.015$c$, 0.025$c$ over 13.25 years, respectively.

2.1.2 Measuring the Knot Positions

Within the M87 jet, we first identified the significant features (peaks) of interest using stacked images. The image stacks include the 2006 ACS/WFC stack, four WFPC2 stacks (epochs 1995–1996, 1998–1999, 2001, and 2007–2008), and three stacks of ACS/HRC exposures (November 2002–December 2003, July 2004–September 2005, November 2005–November 2006). The host galaxy was modeled using the ACS/WFC stacked image with the IRAF/STSDAS tasks ellipse and bmodel and then subtracted. A two-dimensional continuous functional representation of the image cutouts was then created using the Cosine Transform function (FourierDCT) in Mathematica, which allowed us to find prominent peaks, as well as contours of constant flux level around those peaks. In general, the number of interesting peaks was chosen by hand, and the contour line levels were at 50% of the flux of the peak, after a “background” level was subtracted. The positions defining the contour were reverse-transformed from master frame coordinates into each distorted, galaxy-subtracted image so that an intensity-weighted centroid position from the pixels within the contour could be calculated. These final positions were then transformed back into the common reference frame, so that each peak of interest was measured in every exposure, resulting in over 400 position measurements spread over the 13 year baseline.

To measure the apparent motion of the jet components over time, we define the x-direction as the line from the core through the center of knot I (PA of 290∘), with y-direction perpendicular. Data were binned into 26 time bins (shown on the right in Figure 2), and a linear model was fit using standard weighted least squares. The weights were taken to be the inverse of the variance for each time bin, as measured from 10 nearby globular cluster reference sources.

2.2 3C 264

We obtained deep V-band imaging of 3C 264 with the ACS in May of 2014 in order to compare nearly 20 years of images taken by HST for evidence of proper motions of these knots. In a very similar approach as with M87, we localized over 100 globular clusters in the host galaxy as a reference system on which to register previous images taken with WFPC2 in 1994, 1996, and 2002. The systematic error in the registration of the WFPC2 images is generally on the order of 5 milliarcseconds (mas) or less.

To measure their apparent speeds, the position of each knot was measured with a centroiding technique. In the case of knots B and C, we also modelled the jet as a constant-density conical jet with superimposed resolved knots, in order to better measure their fluxes and positions, particularly in the final epoch when they appear to overlap. We plotted the position of each knot along the direction of the jet axis versus time, and fitted the data with a least-squares linear model. A slope significantly larger than zero indicates significant proper motions, and we used the conversion factor 1.442$c$ year/mas to convert angular speeds ($\mu_{app}$) to units of $c$.

2.3 3C 273

We obtained four orbits of ACS/WFC imaging in F606W in May of 2014. These were stacked into a mean reference image (with cosmic-ray rejection) on a super-sampled scale with 0.025*′′* pixels. The registration of the eight individual exposures utilized a full 6-parameter linear transformation based on the distortion-corrected positions of 15–20 point-like sources. The median one-dimensional rms residual relative to the mean position was 0.07 reference-frame pixels, or 1.75 mas, corresponding to a systematic error on the registration ($\times 1/\sqrt{1}6$) of 0.44 mas, or about two hundredths of a pixel.

2.3.1 Background Source Registration

Unlike with M87 and 3C 264, the globular clusters of 3C273 are not detectable in the older WFPC2 imaging and thus cannot be used as a reference frame. Instead, we identified 15 background galaxies based on the criteria that they can be seen by eye above the noise in the individual WFPC2 exposures. These reference galaxies are highlighted in Figure 1. Note that galaxies 4, 5, and 6 have been previously identified as unrelated to the jet by their lack of radio emission, and the bright point source near the jet is actually a foreground star (and thus unsuitable for registering images due to likely proper motions).

To match the archival images to a common reference frame, our general strategy was to use the shape and light distribution of the galaxy to assist in matching their locations in each image. Instead of identifying a single location associated with each galaxy in the deep reference image, we instead sample the galaxy in a grid pattern, resulting in a list of positions along with the flux at each point, sampling across each galaxy. An initial astrometric transformation solution was found by supplying $\approx$10 pairs of matched locations found by hand between the geometrically-corrected raw image and the ACS reference image and calculating the six transformation parameters (without match evaluation/rejection). The initial transformation solution described above is used as a starting point to transform the x,y locations for each galaxy grid in the reference frame into $x_{gc},y_{gc}$ location in the geometrically corrected image. The intensity can then be sampled at each location in the raw image, to be compared directly to the scaled counts value predicted by the scaled reference pixel value. This information is used to calculate the optimal position shift which is used to update the location of the galaxy in the reference frame.

For each individual exposure, we then compile an updated list of position matches between the reference frame and the GC image from the mean x,y value of the galaxy sampling grid in each. In general, we used a subset of the background galaxies which were identifiable by eye and not overly affected by cosmic ray hits. The process of finding the initial $x_{gc},y_{gc}$ values, followed by finding the optimal $\delta$x,$\delta$y improvement on the mean position, was iterated until the positions of the galaxies stopped improving.

2.3.2 Measuring Knot Positions in 3C 273

As a consistency check, we also measured the shift of each knot using a second method which we refer to as the “cross-correlation” method. Over a grid with sub-pixel spacing of 0.2 super-sampled pixels (5 mas), we shifted the 1995 and 2003 images of each individual knot relative to the 2014 image (same cutout area) over a 6 $\times$ 6 pixel area, evaluating the sum of the squared differences between interpolated flux over the knot area for each x/y shift combination. The resulting sum-of-squared differences image in all cases clearly shows a smooth “depression” feature which is reasonably well-fit by a two-dimensional Gaussian under the transformation $g=1-f/\mathrm{max}(f)$, where $f$ is the original sum of squared differences. Taking the minimum $f$ location as measured by the peak of the two-dimensional Gaussian fit, we measure the optimal shift for each knot.

To measure the approximate error on the positions measured, we repeated both of the above methods for simulated images of the jet at each epoch. The simulated images were created by taking the deep 2014 ACS image and adding a Gaussian noise component appropriately scaled from the counts in the original WFPC2 exposures. Since the 2014 image itself has some noise, and also a slightly different PSF from the WFPC2 images, this method likely slightly overestimates the errors. We take the error on each knot measurement to be the standard deviation of the measurements in the simulated images (10 in each epoch).

Finally, we plotted the position of each feature relative to the 2014 position, versus time, to look for evidence of proper motions. We have transformed from the coordinate frame of the aligned images (North up) to one based on the jet, where positive $x$ is in the outflow direction along the jet (taken as position angle (PA) 42∘ south of east) and positive $y$ is orthogonal and to the north of the jet. For both methods, the estimated error on the measurement has been convolved with the systematic error of the registration, which is 0.18, 0.22, and 0.02 reference pixels (4.5, 2.8, and 0.5 mas) for the 1995, 2003, and 2014 epochs, respectively.

3 Results and Discussion

3.1 M87

The most notable findings for M87 were the findings of both deceleration and transverse motions for the first time. In Figure 2, we show the knot complex D, which consists of three sub-knots. Knot D is the most consistently bright feature after the knot A/B/C complex, and significant proper motions were measured in previous studies. As suggested by the contours overlaid on Figure 2, D-Middle is one of the fastest components with a speed of 4.27 $\pm$ 0.30$c$ along the jet, while the brighter D-West shows evidence of deceleration radially, slowing to a near stop by the final epoch in 2008, while maintaining one of the largest transverse speeds of $-$0.59 $\pm$ 0.05$c$ (right panel of Figure 2). Previous results on knot D-East have been conflicting: B95 found that it moved inward along the jet at 0.23 $\pm$ 0.12$c$ (possibly consistent with being stationary), while B99 found a large outward apparent velocity of 3.12 $\pm$ 0.29$c$; our result of 0.28 $\pm$ 0.05 is more in line with B95. It is possible that there is a stationary feature at D-East, through which components emerge (analogous to what is seen in HST-1). In that case, the higher-resolution FOC was perhaps tracking an emerging bright component, while over longer periods the global feature at D-East is stationary. In the outer jet (from knot A), we find apparent velocities that are still superluminal and velocity vectors that appear to line up into a helical/side-to-side pattern.

On the left in Figure 3, we show the complete radial and transverse velocity field of M87 as a function of distance along the jet, including previous work covering similar scales and radio interferometry results.

3.2 3C 264

After aligning all images to a common reference frame, the fast proper motion of knot B is clearly visible, as shown in Figure 4. We found that knots A and D have a $\beta_{app}$ consistent with zero, while the inner knots B and C have $\beta_{app}$ = 7.0 $\pm$ 0.8$c$ and 1.8 $\pm$ 0.5$c$, respectively (Figure 2). The value for knot B exceeds the fastest speeds measured in the jet in M87, the only other source for which speeds on kpc scales have been measured (biretta1999, ; mey13_m87, ). The difference in speeds between knots B and C puts them on a collision course, an interaction which has already begun in the final epoch from 2014, where the knots begin to overlap (Figure 2). This appears to be the first direct observation of colliding knots in an extragalactic jet.

Our data show that in the final 2014 epoch, both knots B and C brighten at the same time by approximately 40% over the mean flux level of the previous three epochs (Figure 4, right). This suggests that fresh particle acceleration has recently taken place, which we attribute to the ongoing collision between these components. Under equipartition, the cooling length for the optical-emitting electrons for knots B and C is longer than the distance they travelled in our observations, consistent with the lack of any decay in flux levels for these knots over the first three epochs. This is not the case for stationary knot A, which can be seen to decay with a timescale of $\sim$70 years. Knot A appears analogous to knot HST-1 in the M87 jet; the latter is thought to be a stationary reconfinement shock where the jet pressure drops below that of the external environment (stawarz06, ). The event that energized knot A may have been the passage of fast-moving knot B circa 1971${}^{+8}_{-17}$, comparable to the knot A decay time.

Radio data taken in October 1983 with the VLA suggest that knots B and C were moving faster in the past and may have decelerated. In the case of knot B, a quadratic fit to the HST + VLA data suggests that in late 1983, the knot had a speed of 10.2$c$, slowing by 0.16$c$/year to reach 5.6$c$ at the beginning of 2014. While a quadratic fit is very poor for the combined data on knot C, a linear fit between the 1983 and 1994 epochs similarly suggests a speed of 9.8$c$. It appears that a much more distinct deceleration “event” occurred for knot C.

In the internal shock model, the efficiency ($\eta$) of the conversion of the liberated kinetic energy ($E_{kin}$) into radiation is generally unknown, with values assumed in the literature in order to match the source luminosity. For the collision in 3C 264, we can estimate the energy available for conversion from our observations to be at least 10*-3*, subject to uncertainties in the total cooling time, and the future evolution of the observed flux.

3.3 3C 273

In the case of 3C 273, all knots have speeds consistent with zero with typical 1$\sigma$ errors on the order of 0.1$-$0.2 mas/year or 1.5$c$, and with 99% upper limit values ranging from $1-5$c. Nearby background galaxies, used as a control check, show that these limits are consistent with stationary objects in the same field (see Figure 3, right).

These results suggest that the knots in the kpc-scale jet, if they are moving packets of plasma, must be relatively slow, in agreement with previous studies based on jet-to-counterjet ratios in radio-loud populations (arshakian2004, ; mullin2009, ). Assuming that the jet either remains at the same speed or decelerates as you move downstream, the $2\sigma$ upper limit speed derived from all knots combined of $1c$ suggests that the entire optical jet is at most mildly relativistic, with a maximum Lorentz factor of $\Gamma<2.9$. However, we cannot rule out the possibility that the knots are standing shock features in the flow, where the bulk plasma moves through the features with a higher $\Gamma$. The best limits on the bulk plasma speed thus remain the limits derived from the non-detection of the IC/CMB component in gamma-rays by mey15_iccmb , where $\delta<7.8$ is implied assuming equipartition magnetic fields.

Finally, we show that the observed upper limits on the proper motion of the knots confirms that the a near-equipartition IC/CMB model for the X-rays of the kpc-scale knots is ruled out. The equipartition IC/CMB model requires that the knots are ballistic packets of moving plasma moving at the bulk speed $\Gamma\approx 15-20$ which would imply proper motions on the order of 10$c$ or 1.12 mas/year which could have been detected in our study; our upper limits easily rule this out at a high level of significance ($>$5$\sigma$). Moving away from equipartition conditions, an IC/CMB model consistent with our observations requires a jet power on the order of five to several hundred times the Eddington limit, and is thus energetically disfavored.

In comparison to other recent HST observations of lower-power optical jets M87 and 3C264, where highly superluminal speeds (6$-$7$c$) have been observed in the optical kpc-scale jet, our first proper-motion study of a powerful quasar jet reveals no significant proper motions. It remains to be seen whether this is because the jet has truly decelerated and is only mildly relativistic, or because the knot features in sources such as M87/3C 264 and 3C 273 represent very different things: moving packets of plasma in the first instance and standing shocks in the second.

Acknowledgements.

Eileen T. Meyer acknowledges HST grants AR-11283, GO-12271, AR-12635, GO-13327 \authorcontributionsEileen T. Meyer reduced the data and wrote the article. Jay Anderson, Tony Sohn, and Roeland van der Marel assisted with the geometric correction and astronomy portion of the analysis. All authors contributed to the interpretation and have read and commented on the manuscript. \conflictofinterestsThe authors declare no conflict of interest.