Blobs in AGN Jets

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IISER Pune

Blobs in AGN Jets

Mayur Shende

IISER Pune

January 20, 2016

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 1 / 10

IISER Pune

Introduction

Focus - relativistic jet initiation in blazars

Specifically, episodic jets (as opposed to winds)

To begin with- study data from episodic blobs in the radio galaxy 3C120

Interesting points about 3C 120:

Episodes of radio blob ejection correspond to dips in X-ray luminosity(e.g., Marscher et al 2002, Chatterjee et al 2009)Episodes of radio blob ejection correspond to enhancement in (Fermi)gamma rays (Casadio et al 2015)

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 2 / 10

IISER Pune

Introduction

Focus - relativistic jet initiation in blazars

Specifically, episodic jets (as opposed to winds)

To begin with- study data from episodic blobs in the radio galaxy 3C120

Interesting points about 3C 120:

Episodes of radio blob ejection correspond to dips in X-ray luminosity(e.g., Marscher et al 2002, Chatterjee et al 2009)Episodes of radio blob ejection correspond to enhancement in (Fermi)gamma rays (Casadio et al 2015)

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 2 / 10

IISER Pune

Introduction

Focus - relativistic jet initiation in blazars

Specifically, episodic jets (as opposed to winds)

To begin with- study data from episodic blobs in the radio galaxy 3C120

Interesting points about 3C 120:

Episodes of radio blob ejection correspond to dips in X-ray luminosity(e.g., Marscher et al 2002, Chatterjee et al 2009)Episodes of radio blob ejection correspond to enhancement in (Fermi)gamma rays (Casadio et al 2015)

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 2 / 10

IISER Pune

Introduction

Focus - relativistic jet initiation in blazars

Specifically, episodic jets (as opposed to winds)

To begin with- study data from episodic blobs in the radio galaxy 3C120

Interesting points about 3C 120:

Episodes of radio blob ejection correspond to dips in X-ray luminosity(e.g., Marscher et al 2002, Chatterjee et al 2009)Episodes of radio blob ejection correspond to enhancement in (Fermi)gamma rays (Casadio et al 2015)

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 2 / 10

IISER Pune

Introduction

Focus - relativistic jet initiation in blazars

Specifically, episodic jets (as opposed to winds)

To begin with- study data from episodic blobs in the radio galaxy 3C120

Interesting points about 3C 120:

Episodes of radio blob ejection correspond to dips in X-ray luminosity(e.g., Marscher et al 2002, Chatterjee et al 2009)

Episodes of radio blob ejection correspond to enhancement in (Fermi)gamma rays (Casadio et al 2015)

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 2 / 10

IISER Pune

Introduction

Focus - relativistic jet initiation in blazars

Specifically, episodic jets (as opposed to winds)

To begin with- study data from episodic blobs in the radio galaxy 3C120

Interesting points about 3C 120:

Episodes of radio blob ejection correspond to dips in X-ray luminosity(e.g., Marscher et al 2002, Chatterjee et al 2009)Episodes of radio blob ejection correspond to enhancement in (Fermi)gamma rays (Casadio et al 2015)

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 2 / 10

IISER Pune

Introduction

Questions:

What are these blobs?

These blobs contain energetic electrons (γ = 105 − 106) confinedwithin a small region

How large are they?

Typical sizes 0.2 − 1.6pc

What are the magnetic fields associated with them (using observationsof synchrotron radiation)?Can these fields confine them (if they are tangled)?

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 3 / 10

IISER Pune

Introduction

Questions:What are these blobs?

These blobs contain energetic electrons (γ = 105 − 106) confinedwithin a small region

How large are they?

Typical sizes 0.2 − 1.6pc

What are the magnetic fields associated with them (using observationsof synchrotron radiation)?Can these fields confine them (if they are tangled)?

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 3 / 10

IISER Pune

Introduction

Questions:What are these blobs?

These blobs contain energetic electrons (γ = 105 − 106) confinedwithin a small region

How large are they?

Typical sizes 0.2 − 1.6pc

What are the magnetic fields associated with them (using observationsof synchrotron radiation)?Can these fields confine them (if they are tangled)?

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 3 / 10

IISER Pune

Introduction

Questions:What are these blobs?

These blobs contain energetic electrons (γ = 105 − 106) confinedwithin a small region

How large are they?

Typical sizes 0.2 − 1.6pc

What are the magnetic fields associated with them (using observationsof synchrotron radiation)?Can these fields confine them (if they are tangled)?

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 3 / 10

IISER Pune

Introduction

Questions:What are these blobs?

These blobs contain energetic electrons (γ = 105 − 106) confinedwithin a small region

How large are they?

Typical sizes 0.2 − 1.6pc

What are the magnetic fields associated with them (using observationsof synchrotron radiation)?Can these fields confine them (if they are tangled)?

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 3 / 10

IISER Pune

Introduction

Questions:What are these blobs?

These blobs contain energetic electrons (γ = 105 − 106) confinedwithin a small region

How large are they?

Typical sizes 0.2 − 1.6pc

What are the magnetic fields associated with them (using observationsof synchrotron radiation)?

Can these fields confine them (if they are tangled)?

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 3 / 10

IISER Pune

Introduction

Questions:What are these blobs?

These blobs contain energetic electrons (γ = 105 − 106) confinedwithin a small region

How large are they?

Typical sizes 0.2 − 1.6pc

What are the magnetic fields associated with them (using observationsof synchrotron radiation)?Can these fields confine them (if they are tangled)?

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 3 / 10

IISER Pune

3C 120: VLBA 15 GHz (Casadio et al 2015)

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 4 / 10

IISER Pune

3C 120: VLBA 43 GHz (Casadio et al 2015)

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 5 / 10

IISER Pune

Blob size

Component Size(pc)

C0 0.24C1 0.35E0 0.99E1 1.7E4 1.1E6 1.23E8 0.72E9 0.72D11 0.25D11a 0.19D12 0.11D12a 0.16

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 6 / 10

IISER Pune

Magnetic Fields and Larmor Radii

Magnetic field (calculated assuming observed (GHz) radiation is atsynchrotron critical frequency)

B =2mcωc

3γ2e

Larmor radius corresponding to this magnetic field

rL =γmc2

eB, = (3/2)

γ3c

ωc

How does this Larmor radius compare with blob size?

i.e., can the magnetic field “confine” the synchrotron emittingelectrons?

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 7 / 10

IISER Pune

Magnetic Fields and Larmor Radii

Magnetic field (calculated assuming observed (GHz) radiation is atsynchrotron critical frequency)

B =2mcωc

3γ2e

Larmor radius corresponding to this magnetic field

rL =γmc2

eB,

= (3/2)γ3c

ωc

How does this Larmor radius compare with blob size?

i.e., can the magnetic field “confine” the synchrotron emittingelectrons?

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 7 / 10

IISER Pune

Magnetic Fields and Larmor Radii

Magnetic field (calculated assuming observed (GHz) radiation is atsynchrotron critical frequency)

B =2mcωc

3γ2e

Larmor radius corresponding to this magnetic field

rL =γmc2

eB, = (3/2)

γ3c

ωc

How does this Larmor radius compare with blob size?

i.e., can the magnetic field “confine” the synchrotron emittingelectrons?

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 7 / 10

IISER Pune

Magnetic Fields and Larmor Radii

Magnetic field (calculated assuming observed (GHz) radiation is atsynchrotron critical frequency)

B =2mcωc

3γ2e

Larmor radius corresponding to this magnetic field

rL =γmc2

eB, = (3/2)

γ3c

ωc

How does this Larmor radius compare with blob size?

i.e., can the magnetic field “confine” the synchrotron emittingelectrons?

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 7 / 10

IISER Pune

Magnetic Fields and Larmor Radii

Magnetic field (calculated assuming observed (GHz) radiation is atsynchrotron critical frequency)

B =2mcωc

3γ2e

Larmor radius corresponding to this magnetic field

rL =γmc2

eB, = (3/2)

γ3c

ωc

How does this Larmor radius compare with blob size?

i.e., can the magnetic field “confine” the synchrotron emittingelectrons?

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 7 / 10

IISER Pune

Magnetic Fields and Larmor Radii

γ = 105 and blob size= 0.24pc

Freq(GHz) B(Gauss) rL(pc) Ratio(rL:blob size)

15 3.57 × 10−7 1.55 × 10−4 6.4 × 10−4

37 8.82 × 10−7 6.27 × 10−5 2.6 × 10−4

43 10.25×10−7 5.4 × 10−5 2.25 × 10−4

γ = 106

Freq(GHz) B(Gauss) rL(pc) Ratio(rL:blob size)

15 3.57 × 10−9 0.1550.65

37 8.82 × 10−9 0.0630.26

43 10.25×10−9 0.0540.23

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 8 / 10

IISER Pune

Larmor radius to blob size ratio at 15GHz

γ = 105

Blob size(pc) rL(pc) Ratio

0.24 1.55 × 10−4 6.45 × 10−4

0.72 1.55 × 10−4 2.15 × 10−4

1.698 1.55 × 10−4 9.13 × 10−5

γ = 106

Blob size(pc) rL(pc) ratio

0.24 0.1550.65

0.72 0.1550.22

1.698 0.1550.091

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 9 / 10

IISER Pune

Conclusions

The magnetic fields required to explain the observed GHz emissionrange from 10−7 − 10−9 G assuming γ = 105 − 106

If γ ≈ 105, rL � blob size; i.e., several Larmor radii can fit inside ablob, and the tangled magnetic field can be considered as a goodconfining agent

However, for γ ≈ 106, the Larmor radius is comparable to the blobsize

Hence we need to appeal to additional scattering/confinementmechanisms

Maybe self-generated turbulence?

Thank you for your attention!

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 10 / 10

IISER Pune

Conclusions

The magnetic fields required to explain the observed GHz emissionrange from 10−7 − 10−9 G assuming γ = 105 − 106

If γ ≈ 105, rL � blob size; i.e., several Larmor radii can fit inside ablob, and the tangled magnetic field can be considered as a goodconfining agent

However, for γ ≈ 106, the Larmor radius is comparable to the blobsize

Hence we need to appeal to additional scattering/confinementmechanisms

Maybe self-generated turbulence?

Thank you for your attention!

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 10 / 10

IISER Pune

Conclusions

The magnetic fields required to explain the observed GHz emissionrange from 10−7 − 10−9 G assuming γ = 105 − 106

If γ ≈ 105, rL � blob size; i.e., several Larmor radii can fit inside ablob, and the tangled magnetic field can be considered as a goodconfining agent

However, for γ ≈ 106, the Larmor radius is comparable to the blobsize

Hence we need to appeal to additional scattering/confinementmechanisms

Maybe self-generated turbulence?

Thank you for your attention!

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 10 / 10

IISER Pune

Conclusions

The magnetic fields required to explain the observed GHz emissionrange from 10−7 − 10−9 G assuming γ = 105 − 106

If γ ≈ 105, rL � blob size; i.e., several Larmor radii can fit inside ablob, and the tangled magnetic field can be considered as a goodconfining agent

However, for γ ≈ 106, the Larmor radius is comparable to the blobsize

Hence we need to appeal to additional scattering/confinementmechanisms

Maybe self-generated turbulence?

Thank you for your attention!

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 10 / 10

IISER Pune

Conclusions

The magnetic fields required to explain the observed GHz emissionrange from 10−7 − 10−9 G assuming γ = 105 − 106

If γ ≈ 105, rL � blob size; i.e., several Larmor radii can fit inside ablob, and the tangled magnetic field can be considered as a goodconfining agent

However, for γ ≈ 106, the Larmor radius is comparable to the blobsize

Hence we need to appeal to additional scattering/confinementmechanisms

Maybe self-generated turbulence?

Thank you for your attention!

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 10 / 10

IISER Pune

Conclusions

The magnetic fields required to explain the observed GHz emissionrange from 10−7 − 10−9 G assuming γ = 105 − 106

If γ ≈ 105, rL � blob size; i.e., several Larmor radii can fit inside ablob, and the tangled magnetic field can be considered as a goodconfining agent

However, for γ ≈ 106, the Larmor radius is comparable to the blobsize

Hence we need to appeal to additional scattering/confinementmechanisms

Maybe self-generated turbulence?

Thank you for your attention!

Mayur Shende (IISER Pune) Blobs in AGN Jets January 20, 2016 10 / 10

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