PAGaN II: The evolution of AGN jets on sub-parsec scales Junghwan Oh Seoul National University East-Asia AGN Workshop 2016

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PAGaN II: The evolution of AGN jets on sub-parsec scales Junghwan Oh Seoul National University East-Asia AGN Workshop 2016 S. Trippe, S. Kang, D. Kim, M. Kino, SS. Lee, T. Lee, J. Park, B. Sohn

AGN at Radio frequencies strong jet out flows Copyright MPIfR, Krichbaum et al. 1998 Up to ~Megaparsec Synchrotron continuum emission Highly collimated Superluminal motions of jet components

Plasma-physical conditions of AGN jets Spatial structure and kinematics Characteristic variations of optical depth Strength and orientation of magnetic fields Tracking bright knots by deep high resolution imaging Spectral index map by 2 (or more) frequencies simultaneous observation Polarimetric observations

Plasma-physics of Active Galactic Nuclei Spatial structure and kinematics Characteristic variations of optical Depth Strength and orientation of magnetic fields Tracking bright knots by deep high resolution Imaging Spectral index map by 2 (or more) frequencies simultaneous observation Polarimetric observations PAGaN II (KVN+VERA) Oh et al. 2015 PAGaN I (KVN only) Kim et al. 2015

KaVA : KVN and VERA Array KVN 21m 7 stations 21 baselines Baseline length: 305 ~ 2300 km 22 & 43 GHz single polarization VERA 20m Angular resolution : ~1.2 mas (22 GHz) ~0.6 mas (43 GHz) Image taken from http://radio.kasi.re.kr/kava/about_kava.php

Sources & Observations Name Redshift z Angular resolution (pc/mas) Type 3C111 0.0491 0.95 Radio galaxy 3C345 0.593 6.63 Quasar 2200+420 0.0686 1.29 BL Lac object Date Obs. Time (hrs / source) Frequency Sources 2014 Mar. 15 6 43 3C111 2014 Apr. 17 6 43 2200+420 2014 Oct. 22 7 ~ 8 22 3C111, 2200+420 2015 Mar. 31 7.5 ~ 8 22 & 43 All 2016 Mar. 9 5.5 ~ 6 22 & 43 All 2016 Jun. 3 5.5 ~ 6 22 & 43 All

3C111 22 GHz 43 GHz

3C111 1 mas = 0.95 pc 10 mas 9.5 pc 14 mas 13.3 pc 22 GHz 43 GHz

3C111 2014 Oct 23 2.29 Jy/beam 1.05 mjy/beam 1.28 x 1.14 (mas) 2015 Apr 1 1.45 Jy/beam 2.18 mjy/beam 1.23 x 1.08 (mas) 2016 Mar 10 1.35 Jy/beam 0.57 mjy/beam 1.42 x 1.19 (mas) 2016 Jun 3 1.27 Jy/beam 1.32 mjy/beam 22 GHz 1.13 x 1.08 (mas)

3C111 2014 Mar 15 1.57 Jy/beam 1.01 mjy/beam 0.666 x 0.597 (mas) 2015 Apr 2 1.25 Jy/beam 2.66 mjy/beam 0.624 x 0.528 (mas) 2016 Mar 11 0.986 Jy/beam 0.74 mjy/beam 0.737 x 0.69 (mas) 2016 Jun 4 1.03 Jy/beam 0.97 mjy/beam 43 GHz 0.63 x 0.595 (mas)

3C111 161 days 384 days Apparent speed: 1.07 ~ 6.5 c (22) 0.98 ~ 6.4 c (43) 345 days 345 days 86 days 86 days 22 GHz 43 GHz

3C111 161 days 384 days Apparent speed : 1.07 ~ 6.5 c (22) 0.98 ~ 6.4 c (43) 345 days 345 days 86 days 86 days 22 GHz 43 GHz

2200+420 (BL LAC) 22 GHz 43 GHz

2200+420 (BL LAC) 1 mas = 1.29 pc 10 mas 22 GHz 14 mas 12.9 pc 43 GHz 18 pc

2200+420 (BL LAC) 22 GHz 2014 Oct 22 2016 Mar 9 3.53 Jy/beam 1.29 Jy/beam 1.0 mjy/beam 0.93 mjy/beam 1.36 x 1.12 (mas) 1.32 x 1.25 (mas) 2015 Mar 31 2016 Jun 3 1.92 Jy/beam 1.08 Jy/beam 3.46 mjy/beam 0.9 mjy/beam 1.12 x 1.04 (mas) 1.28 x 1.11 (mas)

2200+420 (BL LAC) 43 GHz 2014 Apr 17 2016 Mar 10 4.1 Jy/beam 1.02 Jy/beam 2.93 mjy/beam 0.8 mjy/beam 0.647 x 0.53 (mas) 0.764 x 0.663 (mas) 2015 Apr 1 2016 Jun 04 1.76 Jy/beam 0.926 Jy/beam 1.82 mjy/beam 1.03 mjy/beam 0.633 x 0.596 (mas) 0.696 x 0.598 (mas)

2200+420 (BL LAC) 22 GHz 161 days 345 days 85 days Apparent speed : 1 ~ 4 c

2200+420 (BL LAC) 22 GHz 161 days 345 days 85 days Apparent speed : 1 ~ 4 c

2200+420 (BL LAC) 43 GHz 350 days 345 days 85 days Apparent speed : 4.0 ~ 5.9 c

3C345 22 GHz 43 GHz

3C345 1 mas = 6.63 pc 10 mas 66.3 pc 14 mas 92.8 pc 22 GHz 43 GHz

3C345 2015 Mar 31 2.35 Jy/beam 4.57 mjy/beam 1.05 x 1.01 (mas) 2016 Mar 9 3.37 Jy/beam 2.66 mjy/beam 1.43 x 1.24 (mas) 2016 Jun 3 3.06 Jy/beam 3.7 mjy/beam 22 GHz 1.42 x 1.07 (mas)

3C345 2015 Apr 1 2.0 Jy/beam 1.87 mjy/beam 0.654 x 0.607 (mas) 2016 Mar 9 2.0 Jy/beam 3.0 mjy/beam 0.759 x 0.697 (mas) 43 GHz 2016 Jun 3 2.46 Jy/beam 4.47 mjy/beam 0.81 x 0.552 (mas)

3C345 345 days 345 days Apparent speed : 1.97 ~ 10.8 c (43) 85 days 87 days 22 GHz 43 GHz

Viewing angle β = 0.999 c β = 0.998 c β = 0.995 c β = 0.99 c β = 0.98 c β = 0.95 c β = 0.9 c β = 0.5 c

Viewing angle 3C345 β = 0.999 c β = 0.998 c β = 0.995 c β = 0.99 c β = 0.98 c β = 0.95 c β = 0.9 c β = 0.5 c 3C111 2200+420

3C111

3C345

2200+420

BL Lac object (flat) Radio galaxy (moderate steep) Quasar (steep)

Jet expansion (preliminary) Distance (pc) vs Radius (pc) All jet components except core of all sources Linear fit Errors not estimated

Jet expansion (preliminary) Distance (pc) vs Radius (pc) All jet components except core of all sources Linear fit Errors not estimated d = 0.184 r

Summary We obtained interferometric maps sufficient to identify individual source components. We observed significant proper motions of jet components in 3C111, 2200+420 and 3C345. In all sources, we found superluminal apparent jet speeds up to about 10 c. The spectral index maps for 3C 111, 2200+420 and 3C 345 show a tendency for an increasingly fast steepening of the spectral index as function of core distance in the order BL Lac object radio galaxy quasar. This is probably caused by systematic differences in viewing angle. Jet components show systematically larger diameters d at larger core distances r. the components of our targets all follow the same universal relation d 0.184 r.