Compact Radio Structure of Fermi-detected Radio-loud NLS1s

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Compact Radio Structure of Fermi- detected Radio-loud NLS1s CHEN YONGJUN, GU MINGFENG Shanghai Astronomical Observatory, CAS

description

Compact Radio Structure of Fermi-detected Radio-loud NLS1s. CHEN YONGJUN, GU MINGFENG Shanghai Astronomical Observatory, CAS. Definition of RL NLS1s. H  slightly broader than forbidden lines (OIII, NII, SII), but generally < 2000 km/s Relative weakness of OIII: [OIII]/H

Transcript of Compact Radio Structure of Fermi-detected Radio-loud NLS1s

Page 1: Compact  Radio Structure of Fermi-detected   Radio-loud NLS1s

Compact Radio Structure of Fermi-detected Radio-

loud NLS1s

CHEN YONGJUN, GU MINGFENGShanghai Astronomical

Observatory, CAS

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Definition of RL NLS1s

H slightly broader than forbidden lines (OIII, NII, SII), but generally < 2000 km/s

Relative weakness of OIII: [OIII]/H<3 Presence of emission lines from FeII or higher

ionization lines (Goodrich 1989) RL means: f(1.4GHz)/f (B) 10, a criteria from

Komossa & Voges 2006) (F5/FB )The narrowest Balmer lines, strongest FeII

emission and lowest ratios of [OIII]/H

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Fundamental Features for RL NLS1s

Reverberation mapping and experimental relation from BLS1s systematically lower black hole mass (e.g. Boroson 2002) (X-ray variability, steller velocity & bulge luminosity)

High accretion rates close to or even above the Eddington rate (e.g. Komossa 2006): soft and hard X-ray

Host Galaxies: generally spiral First Fermi detected NLS1s: PMN J0948+0022,

7 with TS > 16, Third class of Gamma-ray AGN

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Fermi Detected RLNS1s with TS>16

Source Red-shift

γ rays (ph cm-

2 s-1)Mon

TS Radio Morph.

1H 0323+342* 0.061 (1.60±0.06)×10-7 34 45 Core-jet (MOJAVE)

SBS 0846+513

0.584 (2.3±0.2)×10-7 36 560 Core-jet (MOJAVE)

PMN J0948+0022*

0.585

(3.2±0.2)×10-7 52 259 Core-jet (MOJAVE)

B2 1111+32 0.189

(2.4±0.3)×10-9 22 16 Core-jet (VLBA)

PKS 1502+036*

0.409

(7.3±2.4)×10-8 24 27 Core-jet (MOJAVE)

FBQS J1644+2619

0.145

(7.5±1.6)×10-8 51 27 Core-jet (VLBA)

PKS 2004−447*

0.240

(1.0±0.9)×10-9 3 10(43)

Core-jet (VLBA)

* With much larger TS shown in Abdo et al. (2009)

TS: http://www.brera.inaf.it/utenti/foschini/gNLS1/catalog.html

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Radio Structure of 1H 0323+342 and SBS 0846+513

MOJAVE PROGRAMMOJAVE PROGRAM

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Radio Structure of PMN J0948+0022 and

1502+036

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VLBA OBSERVATION OF B2 1111+32

AT 2.3 AND 8.4 GHz Data: NRAO ARCHIVE Epoch: 2010 Nov 9-11, 20 min with 4

SCANS Instrumental Calibrator: 1749+096 Data Reduction: Standard method

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VLBA Imaging Results

S Band X Band

D C D C

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Radio Structure of FBQS J1644+2619 PKS 2004-

447

From Orienti et al. 2012From Doi et al. 2011

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Core Nature of The Radio Structures

Source Flux (mJy) Brightness Temperature (K)

Spectral Index

Log(R)

1H 0323+342* 355.30 5.58e11 2.39

SBS 0846+513

284.33 1.16e12 ~0.0 3.16

PMN J0948+0022*

861.33 7.25e12 0.82 2.55

B2 1111+32 38.59 <5.50e10 -1.26

PKS 1502+036*

578.59 4.21e11 0.66 3.19

FBQS J1644+2619

82.4 (1.7 GHz)

~1e11 0.38 2.97

PKS 2004−447*

530.00 -0.67

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Gamma and Radio Nature of

1H 0323+ 342 1H 0323+342 emits Gev, and even possibly

Tev radiation in a region very close to central black hole

MOJAVE shows an obvious one-sided structure with mild brightness temperature

A radio remarkable flare ever detected by a factor 3 with flat spectrum

Accretion rate: 90% Emission might be mildly Doppler-boosted

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Gamma and Radio Nature of

SBS 0846+513 -ray luminosity~1048 erg s-1Doppler boosted

Core-jet structure on pc and unresolvable on kpc scale with superluminal motion 8.2c

Very bright core with TB above Comptom limit

Flat radio spectrum Radio and -ray emission

are both Doppler boostedFrom D’Ammando et al (2012)

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Gamma and Radio Nature of PMN J0948+0022

The first source detected -ray emission and burst with ~1048 erg s-1presence relativistic jet (1.5e8 solar mass)

Very compact (~10 pc), very bright, core jet structure and strong polarization (3%)

Invert radio spectrum, the Comptom dominance is more extreme in SED relative to 3C273 (Forschini et al. 2010)

Yang, High accretion rate, Relativistic Jet

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Gamma and Radio Nature of

B2 1111+32 B2 1111+32 is detected by fermi with

ts 16 The maximum core brightness

temperature: 5.50e+10 K Simultaneous core spectral indice:

= -1.260.07 for VLA obs. = -0.330.07 for VLBA obs. = -1.200.12 for EVN

It’s more like a GPS source with compact structure

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VLA-A Structure at Epoch 1992 Dec. 20

FQ =1.43 GHzBEAM = 1.62 X 1.39 at -3.6

X

Unresolvable on subarcsec scale

S Band X Band

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Doppler Boosting?

Komossa et al.(2006): = -0.56 (0.33 GHz and 1.4 GHz) = -1.24 (1.4 GHz and 4.85 GHz) Roughly agreement with our results Radio structure, spectral indices,

core brightness temperature GPS

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With Non-simultaneous Data

Ghisellini et al. (1993)

X-ray data : 2002 Jun VLBA data: 2010 Nov 0.85The result argues against relativistic hypothesis

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Gamma and Radio Nature of B2 1111+32

VLA-A and EVN with 5 an observations show compact radio structure, no extended emission was detected

Multi-frequency VLBA observation shows a signature of core-jet radio structure

Brightness temperature, spectral indices, flux variability and a rough estimate of Doppler factor argue more for GPS hypothesis with relatively strong radio emission

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Gamma and Radio Nature of

PKS 1502+036 L0.1−100GeV = 7.8×1045 erg s−1

Unresolvable on VLA and core jet on vlbi scale

Invert radio spectrum 0.66, quite bright with T~4e11K

Superluminal motion not detected (multi-epoch)

Yang and slightly Doppler boosted From D’Ammando et al (2013)

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Gamma and Radio Nature of FBQS J1644+2619

Intermediate -ray luminosity

Core-jet on pc and double structure on kpc scale

Flat spectrum, intermediate brightness temperature

Mildly Dopper-boosted

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Gamma and Radio Nature of

PKS 2004-447 Relatively small Gamma-ray

luminosity with high confidence Unresolvalbe on ATCA scale and core-

jet-like structure on pc scale Steep above 8.4 GHz (-0.67) and

flatter (-0.33) below 4.8 GHz Like a CSO source and small Doppler

effect is expected as B2 1111+32

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SUMMARY

For the 7 RL NLSY1s, two are strongly Doppler-boosted, 3 are mildly and 2 are trivially Doppler-boosted

Even for Fermi-detected RL NLSy1 sources, some are intrinsically radio and possibly -ray loud, some are Doppler boosted

All these Fermi-detected RL NLSY1s are expected to young objects with small black mass and high accretion rates

NLSy1s are younger and more Comptom dominant in comparison with Blazar objects

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