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On the nature of On the nature of High High Frequency Frequency Peaker Peaker radio sources radio sources Monica Orienti Girdwood, 22/05/2007 Monica Orienti – Extragalactic Jets (INAF – IRA, Bologna) Daniele Dallacasa (UniBo, Bologna)
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On the nature of High Frequency Peaker radio sources

Jan 14, 2016

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On the nature of High Frequency Peaker radio sources. Monica Orienti. (INAF – IRA, Bologna). Daniele Dallacasa (UniBo, Bologna). Girdwood, 22/05/2007 Monica Orienti – Extragalactic Jets. The Goals. - PowerPoint PPT Presentation
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Page 1: On the nature of  High  Frequency  Peaker  radio sources

On the nature of On the nature of High High FrequencyFrequency Peaker Peaker

radio sourcesradio sources

Monica Orienti

Girdwood, 22/05/2007 Monica Orienti – Extragalactic Jets

(INAF – IRA, Bologna)

Daniele Dallacasa (UniBo, Bologna)

Page 2: On the nature of  High  Frequency  Peaker  radio sources

The GoalsThe Goals

• Analysis of the variability, morphology and polarization of candidate HFPs;

• Selection of a sample of genuine young HFPs;

• What can we learn from HFPs?

Page 3: On the nature of  High  Frequency  Peaker  radio sources

Peaks > 5 GHz;

t ~ 102 - 103 years

Bright HFP sample consists of

55 objects:

• 10 galaxies;

• 34 quasars;

• 5 BL Lacs;

• 6 Empty Fields

(Dallacasa et al. 2000)

High Frequency PeakersHigh Frequency PeakersA sample of young HFPA sample of young HFP

Page 4: On the nature of  High  Frequency  Peaker  radio sources

Contamination from BL Lac objectsContamination from BL Lac objects

Young radio sources

• No flux-density variability;

• “Double/Triple” structure;

• Unpolarized

Blazars

• Strong flux density variability;

• Core-Jet structure;

• Significantly polarized

Blazars may display the characteristics of young radio sources when their emission is dominated by a flare in the jet-base.

A sample of young HFPA sample of young HFP

Page 5: On the nature of  High  Frequency  Peaker  radio sources

Multi-frequency VLA observationsMulti-frequency VLA observations

• Galaxies V<3;

• 21 sources (18 quasars and 3 BL

Lacs) V >>3;

• 12 quasars no longer show a peaked spectrum;

4 epochs of VLA observations at 9 frequencies ( 1.4 – 43 GHz)

(Si – Si)2

V= 1

mi = 1

m

i

A sample of young HFPA sample of young HFP

Page 6: On the nature of  High  Frequency  Peaker  radio sources

VLBA observationsVLBA observations

Two-frequencies VLBA observations

In the optically-thin part of the spectrum

We find that:

• 27% “Double/Triple” morphology;

• 12% “Core-Jet” morphology;

• 61% Unresolved

Orienti et al. 2006a, A&A, 450, 959

=0.2

A sample of young HFPA sample of young HFP

Page 7: On the nature of  High  Frequency  Peaker  radio sources

Polarization propertiesPolarization properties

From simultaneous VLA observations at

4.5, 8.4, 15 and 22 GHz + information

from the NVSS at 1.4 GHz, we find:

• 57% have fractional polarization >1%;

• 36% are completely unpolarized;

• All the galaxies are unpolarized;

• 70% of quasars are highly-polarized.

A sample of young HFPA sample of young HFP

Page 8: On the nature of  High  Frequency  Peaker  radio sources

ResultsResults

From the flux density variability, morphology and polarization we

find that:

Quasars are:

Variable;

“Core-Jet” morphology;

Polarized emission (>1%).

Galaxies are:

No Variability

“Double-Triple” morphology

Unpolarized or slightly (<1%) polarized

Only 25 from the HFP sample are still young radio source candidates

A sample of young HFPA sample of young HFP

Page 9: On the nature of  High  Frequency  Peaker  radio sources

HFPs and the source growthHFPs and the source growth

Strong flux-density and arm-

length asymmetries in

compact (< 15 kpc) radio

sources

Constraining the radio source evolutionConstraining the radio source evolution

Page 10: On the nature of  High  Frequency  Peaker  radio sources

The evolution modelThe evolution modelThe source growth in an ambient

medium with a King-like profile:

Asymmetries cannot be

reproduced

v t -1/2 (NLR)

Const (ISM)

L t 5/8 (NLR)

t -1/2 (ISM)

ncl

n0

n r -β

t3 t2 t1 t0 t1 t2 t3

Jet-cloud interaction:

ncl

n0

Lj,c l

9 8

2ncl

n0

vj,c v

Constraining the radio source evolutionConstraining the radio source evolution

Page 11: On the nature of  High  Frequency  Peaker  radio sources

Magnetic fieldMagnetic fieldFrom equipartition:

Heq ~ 0.16 G

Direct measurement:

H ~ 0.150.03 G

From X-ray luminosities:

H ~ 0.14 G

Consistent with a source in equipartition condition with X-ray luminosity due to Synchrotron Self-Compton

Constraining the physical conditionsConstraining the physical conditions

RXJ1459+3337