(sub-)parsec scale jet of 3C273 at mm-wavelengths

Multi-frequency polarization
structure of the (sub-)pc scale jet
in 3C273 at mm-wavelengths
Tuomas Savolainen
Aalto University Metsähovi Radio Observatory, Finland
Max-Planck-Institut für Radioastronomie, Germany
VLBI-scale Faraday rotation in the jet
of 3C273 at cm-wavelengths
McKinney & Blandford 2009
Zavala & Taylor (2005)
Hovatta et al. (2012)
100 π‘Ÿπ‘†
Asada et al. (2002)
2
43-86 GHz EVPA difference
(Attridge et al. 2005)
McKinney & Blandford 2009
β€’ No absolute EVPA calibration at
86 GHz, but 67° change in
Ξ”πœ’43βˆ’86 across the jet at
0.8mas from the core
β€’ βˆ†RM > 3.2 × 104 rad mβˆ’2
β€’ Depolarized core. If external,
πœŽπ‘…π‘€ > 5 × 104 rad/m2
100 π‘Ÿπ‘†
3
43-86 GHz EVPA difference
(Hada et al. 2016)
McKinney & Blandford 2009
100 π‘Ÿπ‘†
No absolute EVPA calibration at 86 GHz.
Ξ”πœ’ = 50° indicates βˆ†RM > 2.4 × 104 rad mβˆ’2
4
15-86 GHz VLBA polarimetry
of 3C273 in Oct 2010
McKinney & Blandford 2009
15 GHz
24 GHz
100 π‘Ÿπ‘†
πΌπ‘π‘’π‘Žπ‘˜ πΌπ‘π‘Žπ‘ π‘’ = 2500
πΌπ‘π‘’π‘Žπ‘˜ πΌπ‘π‘Žπ‘ π‘’ = 1300
5
15-86 GHz VLBA polarimetry
of 3C273 in Oct 2010
McKinney & Blandford 2009
43 GHz
86 GHz
100 π‘Ÿπ‘†
86 GHz EVPA calibration using
IRAM 30-m (Agudo et al. 2014)
πΌπ‘π‘’π‘Žπ‘˜ πΌπ‘π‘Žπ‘ π‘’ = 600
πΌπ‘π‘’π‘Žπ‘˜ πΌπ‘π‘Žπ‘ π‘’ = 260
6
Differences in EVPA
between 86 and 43 GHz
McKinney & Blandford 2009
100 π‘Ÿπ‘†
7
Differences in EVPA
between 86 and 43 GHz
βˆ†π‘πŒ ≳ 𝟐 × πŸπŸŽπŸ’ 𝐫𝐚𝐝 π¦βˆ’πŸ
McKinney & Blandford 2009
βˆ†πŒ = +πŸ“°
βˆ†πŒ = βˆ’πŸπŸŽ°
𝑹𝑴 ~ 𝟏 × πŸπŸŽπŸ’ 𝐫𝐚𝐝 π¦βˆ’πŸ
100 π‘Ÿπ‘†
βˆ†πŒ = βˆ’πŸ’πŸ“°
8
Polarization degree and depolarization
McKinney & Blandford 2009
m = πŸ’ ± 𝟏%
m β‰ˆ 𝟎. πŸ“%
m = 𝟏𝟎 ± 𝟐%
m = πŸ• ± 𝟏%
100 π‘Ÿπ‘†
m β‰ˆ 𝟐𝟎%
86 GHz
43 GHz
Depolarization close to the core. If due to external
Faraday dispersion , πœŽπ‘…π‘€ ≳ 2 × 104 rad/m2
9
Need for higher N-S resolution
Super-resolved
0.15 mas circ. beam
β€’ Transverse polarization structure
within first milliarcsec (2.4 pc /
4000 π‘ŸπΊ )
β€’ β€œThread” of polarized emission
with EVPA following the bend
inside the jet?
β€’ Need for more N-S resolution
and more sensitivity at 86GHz:
GMVA+ALMA observations last
April (Akiyama et al.)
10
Summary
β€’ Obtained high-quality 15-86 GHz polarimetric
VLBA images of 3C273 – including EVPA
calibration also at 86 GHz
β€’ Confirms the earlier results of RM ≳ 2 ×
104 rad mβˆ’2 inside the first milliarcsecond
β€’ Depolarized core at 43 GHz indicating πœŽπ‘…π‘€ ≳
2 × 104 rad/m2
β€’ Calibrated 86 GHz EVPAs seem to align with a
bend inside the first milliarcsecond
11
BACKUP SLIDES
12
RM β€œmapping” at 86-24 GHz
McKinney & Blandford 2009
100 π‘Ÿπ‘†
Problems: (very) poor πœ†2 -coverage, not
enough resolution at 24 GHz, possible
non- πœ†2 behaviour …
13
Multifrequency VLBA
polarimetry at 15-86 GHz
β€’ Observations on 27 Oct 2010 (part of a longer monitoring
program)
β€’ Obs. freqs. 15, 24, 43 and 86 GHz
β€’ Targets: 3C273, 3C279
β€’ Additional calibrators: 0923+392, 1308+326
β€’ D-term rms: 0.024 (86GHz), 0.010 (43GHz), 0.006
(24GHz), 0.004 (15GHz)
β€’ Absolute EVPA calibration by UMRAO (15GHz, M.Aller),
VLA (24, 43 GHz), IRAM-30 (86 GHz; Agudo et al. 2014)
β€’ 𝜎(EVPA): 5° (15GHz), 5° (24GHz), 5° (43GHz), 7° (86GHz)
14
43-86 GHz spectral index image
McKinney & Blandford 2009
100 π‘Ÿπ‘†
15
Differences in EVPA
between 86 and 43 GHz
βˆ†π‘πŒ ≳ 𝟐 × πŸπŸŽπŸ’ 𝐫𝐚𝐝 π¦βˆ’πŸ
McKinney & Blandford 2009
βˆ†πŒ = +πŸ“°
βˆ†πŒ = βˆ’πŸπŸŽ°
𝑹𝑴 ~ 𝟏 × πŸπŸŽπŸ’ 𝐫𝐚𝐝 π¦βˆ’πŸ
100 π‘Ÿπ‘†
βˆ†πŒ = βˆ’πŸ’πŸ“°
16
Polarization degree along the jet
McKinney & Blandford 2009
43 GHz
86 GHz
100 π‘Ÿπ‘†
17
Blank slide
McKinney & Blandford 2009
100 π‘Ÿπ‘†
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