A Study of Magnetic Field by Using Core Shift for Radio Galaxy 3C - - PowerPoint PPT Presentation

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Jul 05, 2023 135 likes •412 views

A Study of Magnetic Field by Using Core Shift for Radio Galaxy 3C 111 K.Shiotani , K.Fujisawa, K.Niinuma (Yamaguchi univ.) Introduction AGN Jets SMBH Lobe Relativistic jet (~10) Cygnus A radio image for VLA(Image courtesy of NRAO) A

SLIDE 1

A Study of Magnetic Field by Using Core Shift for Radio Galaxy 3C 111

K.Shiotani , K.Fujisawa, K.Niinuma (Yamaguchi univ.)

SLIDE 2

Introduction

SLIDE 3

AGN Jets

Powerful energy emission ( erg/s) from very compact region
Radio to γ-ray emission ; Synchrotron + Inverse Compton
Collimated plasma flow with relativistic velocity

SMBH Lobe Relativistic jet (Γ~10) Cygnus A radio image for VLA(Image courtesy of NRAO)

A lot of issues has not been clarified

a few kpc ~ Mpc

∼ 1040

How collimate? How accelerate?

SLIDE 4

Magnetically Driven Model

Helical magnetic field・Synchrotron radiation・high speed jet

⇨magnetically driven model is a most likely model

J.McKinney 2006

Important to estimate the magnetic field strength of the jet

f pc or less scale for more realistic simulation

宇宙ジェットの磁気駆動モデルのコンピュータシミュレーション (http://home.hiroshima-u.ac.jp/hasc/news/3c279/index.html , Shibata and Uchida 1986)

SLIDE 5

Motivation

Estimating physical parameters (especially the magnetic field) at the pc scale from the observation, constraining the theoretical model Magnetic field can not be measured directly . . .

“Core shift” gives us indirect measurement of magnetic field

SLIDE 6

Method & Target

SLIDE 7

Core shift phenomenon
Radio core position observed at higher frequency moves more upstream
f the jet (Lovanov 1998)
Z
Z

Core Shift

rcore ∝ ν− 1

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B = B1pcr−m

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N = N1pcr−n

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k = (3 − 2α)m + 2n − 2 5 − 2α

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, Hada+ 2011

SLIDE 8

Estimation of B using core shift

Assuming equipartition in conical jet (Hirotani et al.2005)

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ν1, ν2

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: displacement radio core at difference frequency : frequency : luminosity distance : redshift : doppler factor : jet opening angle : the angle between the jet and the line of sight

∆rcore

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r

1pc

B1pc = 1.45 × 10−8 ✓∆rcoreDLν1ν2 ν2 − ν1 ◆ 3

4 ✓

1 (1 + z)4δ2φ sin2 θ ◆

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Only need to estimate magnetic field at 1pc

Δrcore

Only VLBI observation

SLIDE 9

Estimation of B using core shift

Author

Frequency [GHz]

Source sample Number of observations

Kovalev+08

2.3, 8.6

29 ≦3/a source O’sullivan+09

4.6, 5.1, 7.9, 8.9, 12.9,15.4, 22.2, 43.1

6 1/a source Pushkarev+12 8.1, 8.4, 12.1, 15.4 191 12/a source

・High frequency ・Single source/Monitoring

Previous studies

Our observation

・Large viewing angle ・The distance is close ・Flare phase ・Single source

SLIDE 10

Radio Galaxy 3C 111

Relatively close (distance of 196Mpc;Grandi +12)
Typical FR II radio galaxy , the jet viewing angle θ=18°(Jorstad+05)
Jet activity is powerful and just in the flare phase!!

VLBA 15GHz Radio Image (MOJAVE project) The light curve of map peak at VLBA 15GHz radio images

SLIDE 11

Purpose & Observation

SLIDE 12

The purpose

To measure the core shift and its time variation, by high-frequency, single target and monitoring

Target Array

Large viewing angle Flare phase

3C 111

High frequency High image quality

KaVA

SLIDE 13

Array：KaVA (Code : k18ks01)
Obs. time：8hours /1epoch
Frequency:22/43 GHz
& freq. switching/1hour
Integration time : 4 hours/freq.

Observation

Epoch Date

The light curve (up: 22 GHz, bottom: 43 GHz)
(red: core, blue: K1, green: K2)

Preliminary

SLIDE 20

Measuring core offset from each jet component

Core offset measurement

∆rcore

Pinned Jet 22 GHz Core 43 GHz Core

DOY Jet Component 23 K1

0.112±0.036 0.210±0.090

23 K2

0.026±0.024 0.070±0.068

101 K2

0.111±0.047 0.208±0.110

154 K1

0.246±0.071 0.380±0.149

B1pc

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∆rcore

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B1pc = 1.45 × 10−8 ( ΔrcoreDLν1ν2 ν2 − ν1 )

3 4

Core offset vs Distance from Core
( blue: K1, green: K2)

？

Preliminary

SLIDE 24

Jet variation

22GHz 43GHz

The jet component is optically thin or thick?

Thin Thick

SLIDE 25

Jet variation

22GHz 43GHz

The jet component is optically thin or thick?

Thick

Preliminary

SLIDE 26

Summary & Future

SLIDE 27

Summary & Future

To constrain magnetically model, we estimated the physical

parameter, especially the magnetic field, by using core shift.

We performed monitoring observation for 3C111 with KaVA
and confirmed the variation of the core offset
Estimated the magnetic field at 1pc is
We got a possibility to suggest variations
We will measure the physical parameter variation and

associate with phenomenon

Please continue to observe with KaVA.

B1pc ≈ 0.07 − 0.38[G]

Summary Future