Swift J : the EVN view Zsolt Paragi, Joint Institute for VLBI ERIC

Slides:



Advertisements
Similar presentations
Gabriele Giovannini Dipartimento di Astronomia, Bologna University Istituto di Radioastronomia - INAF EVN observations of M87 as follow-up on a recent.
Advertisements

Mapping HI absorption at z=0.026 against a resolved background CSO Andy Biggs, Martin Zwaan, Jochen Liske European Southern Observatory Frank Briggs Australian.
Gamma-ray burst afterglows with VLBI: a sensitivity quest Ylva Pihlström University of New Mexico.
Active Galactic Nuclei Very small angular size: point like High luminosity: compared to host galaxies Broad-band continuum emission: radio to TeV Strong.
Jets from stellar tidal disruptions by supermassive black holes Dimitrios Giannios Princeton University HEPRO3, Barcelona, June 30.
Modeling the X-ray emission and QPO of Swift J Fayin Wang ( 王发印) Nanjing University, China Collaborators: K. S. Cheng (HKU), Z. G. Dai (NJU), Y.
A rough guide to radio astronomy and its use in lensing studies Simple stuff other lecturers may assume you know (and probably do)
Dusty star formation at high redshift Chris Willott, HIA/NRC 1. Introductory cosmology 2. Obscured galaxy formation: the view with current facilities,
1 Arecibo Synergy with GLAST (and other gamma-ray telescopes) Frontiers of Astronomy with the World’s Largest Radio Telescope 12 September 2007 Dave Thompson.
Kinematics of parsec-scale radio jet in 3C48 Tao An 1, In collaboration with X.Y.Hong 1, M.J.Hardcastle 2, T.Venturi 3, D.Worrall 2,T.J.Pearson 4, Z.-Q.Shen.
S. Jorstad / Boston U., USA A. Marscher / Boston U., USA J. Stevens / Royal Observatory, Edinburgh, UK A. Stirling / Royal Observatory, Edinburgh, UK M.
The jet of Mrk 501 from millions of Schwarzschild radii down to a few hundreds Marcello Giroletti INAF Istituto di Radioastronomia and G. Giovannini, G.
8 th EVN Symposium: Exploring the universe with the real-time VLBI. 26 – 29 September 2006.Giuseppe Cimò – JIVE Interstellar Scintillation and IDV Twinkle,
Recent Results and the Future of Radio Afterglow Observations Alexander van der Horst Astronomical Institute Anton Pannekoek University of Amsterdam.
Four hot DOGs eaten up with the EVN Sándor Frey (FÖMI SGO, Hungary) Zsolt Paragi (JIVE, the Netherlands) Krisztina Gabányi (FÖMI SGO, Hungary) Tao An (SHAO,
P-L Relation Compared with the P-L relation from Whitelock & Feast (2000) VLBI results (black) show less scatter than the Hipparcos results (red) Source.
Gamma-Ray Bursts Energy problem and beaming * Mergers versus collapsars GRB host galaxies and locations within galaxy Supernova connection Fireball model.
Redshift, Time, Spectrum – Sándor Frey (FÖMI SGO, Hungary) In collaboration with: Leonid I. Gurvits (JIVE, The Netherlands) Zsolt Paragi (JIVE, The Netherlands)
Gamma-Ray Bursts: Open Questions and Looking Forward Ehud Nakar Tel-Aviv University 2009 Fermi Symposium Nov. 3, 2009.
Structure Formation in the Universe Concentrate on: the origin of structure in the Universe How do we make progress?How do we make progress? What are the.
Super Massive Black Holes The Unknown Astrophysics of their initial formation.
AGN: Linear and Circular Polarization
VHE  -ray Emission From Nearby FR I Radio Galaxies M. Ostrowski 1 & L. Stawarz 1,2 1 Astronomical Observatory, Jagiellonian University 2 Landessternwarte.
Brigthest Cluster Galaxies Unique class of objects  most luminous  most massive  extended source  some BCG shows multiple nuclei → galaxy merger →
Radio afterglows of Gamma Ray Bursts Poonam Chandra National Centre for Radio Astrophysics - Tata Institute of Fundamental Research Collaborator: Dale.
Tidal Disruption Events
The Host Galaxies of Dust-Obscured Gamma-Ray Bursts
Evidence from AGN for Binary Black Holes
Radio Loud and Radio Quiet AGN
EVN 2015 Starburst Galaxies
e-VLBI correlator mode: control interfaces
Transients and Robotic Triggering at 15 GHz with AMI
r = Ag / Aopt > 2 or more, so Compton dominance varies.
Gamma Rays from the Radio Galaxy M87
VLBI in China and the Collaboration with NL
黎卓 HB Perets, JC Lombardi Jr, SR Milcarek Jr JUNO会议,南京,2016/4/17-18
On behalf of the Radio-Agile AGN WG
Tao An (SHAO) & Zsolt Paragi (JIVE) et al.
"Constraining the Size of the Radio Counterpart
Probing Magnetized Turbulence in the Fermi Bubbles
Black Hole Binaries in Quiescence
Lecture 5 Multi-wavelength cosmic background
Virgo cluster survey with MXT
An Arecibo HI 21-cm Absorption Survey of Rich Abell Clusters
Paul Alexander Dave Green, Malcolm Longair, Julia Riley, Martin Krause
Relativistic outflows and GLAST
The Bursting Universe: New Tools for Cosmology and Physics
NRAO-CV Lunch Talk June 2017
L B V I The highest redshift radio quasars with the highest resolution
Radio-Optical Study of Double-Peaked AGNs: 3C 390.3
Paola Rodriguez Hidalgo High Energy Astrophysics
How to classify a Gamma -ray source as a Blazar
The origin nuclear X-ray emission in the nuclei of radio galaxy-FR Is
A Search for water masers in High-redshift un-beamed AGNs: T. Ghosh, S
(National Astronomical Observatory of Japan)
Risolvere il Background X al suo picco
ACTIVE GALAXIES and GALAXY EVOLUTION
Black Holes in the Deepest Extragalactic X-ray Surveys
Galaxies With Active Nuclei
Super Massive Black Holes
Millimeter Megamasers and AGN Feedback
Galaxies With Active Nuclei
Tight Liso-Ep-Γ0 Relation of Long Gamma-Ray Bursts
Lecture 7: Jets on all scales Superluminal apparent motions.
Dr. Jun Yang, Senior VLBI Support scientist
Compact radio jets and nuclear regions in galaxies
by S. van Velzen, G. E. Anderson, N. C. Stone, M. Fraser, T. Wevers, B
Constraining IMBH masses with VLBI
An MHD Model for the Formation of Episodic Jets
Borislav Nedelchev et al. 2019
Presentation transcript:

Swift J1644+5734: the EVN view Zsolt Paragi, Joint Institute for VLBI ERIC Jun Yang, Onsala Space Observatory Alexander van der Horst, George Washington University Leonid Gurvits, Joint Institute for VLBI ERIC Bob Campbell, Joint Institute for VLBI ERIC Dimitrios Giannios, Purdue University Tao An, Shanghai Astronomical Observatory Stefanie Komossa, MPIfR-Bonn IAU Symposium 324 on BH astrophysics Ljubljana, 2016 Sep 13

IAU Symposium 324 on BH astrophysics Outline I will explain the figure below – why is it interesting, how the VLBI data were obtained, what constraints it puts on relativistic ejecta from TDE, and how the EVN and VLBI with the SKA will contribute to the field? “No apparent superluminal motion in the first-known jetted tidal disruption event Swift J1644+5734” Yang et al. 2016, MNRAS 462, L66 IAU Symposium 324 on BH astrophysics Ljubljana, 2016 Sep 13

IAU Symposium 324 on BH astrophysics Why TDE are important? They may give a clue on the massive BH population (MBH<106 M) To understand supermassive BH formation we must now the BH demographics – but massive BH below ~106 M are hard to find. Where are the left-over seed BH required by structure formation models? How do they grow? We can study jet formation in a pristine environment Also relevant for AGN feedback. VLBI will have a crucial role in this, since milliarcsecond resolution is needed. MBH   relation Barth, Greene & Ho (2005) IAU Symposium 324 on BH astrophysics Ljubljana, 2016 Sep 13

What is the expected TDE rate? Take Swift J1644+5734 as prototype for predictions in the X-ray and radio bands: Donnarumma et al. (2015) BH mass function (G and Gz models adopted) Shankar et al. (2013) Intrinsic rate NTDE~ a few x10-5 per yr per galaxy M = [106 - 108 Msun ] From intrinsic to jetted TDE rate: rescaling R(z) by a factor (2Γ)−2 Must understand jet efficiency and measure Lorentz factors in TDE IAU Symposium 324 on BH astrophysics Ljubljana, 2016 Sep 13

Swift J1644+5734: the first jetted TDE Zauderer et al (2011, 2013) Berger et al. (2012), Wiersema et al. (2012) Within 0.2 kpc of the host galaxy nucleus X-ray lightcurve follows t −5/3 Total X-ray energy ~1053 fbeam erg X-rays: rapid variability (100s), non-thermal spectrum, high Eddington luminosity => inner jet close to the BH Radio: non-thermal, no rapid variability => shock interaction with ISM? IAU Symposium 324 on BH astrophysics Ljubljana, 2016 Sep 13

Swift J1644+5734: the first jetted TDE Estimate from interstellar scintillation: Γjet ~ 5 (multi-frequency radio monitoring; Zauderer et al. 2011). Γjet ~ 7 – 2, i.e. decreasing with the time in a collimated jet by analogy to GRB afterglows. The jet will be resolved (~0.2 mas) with VLBI at 22 GHz in 6 years assuming a jet opening angle ~5 deg (Berger et al. 2012). Berger et al. 2012 Possible VLBI strategies for Swift J1644+5734 Choice 1: wait for 6 years, measure size (if source still bright) with VLBI at high frequency Choice 2: probe superluminal jet via proper motion βapp with VLBI (not necessarily highest frequency) Constraints on Lorentz factor Γjet = (1 −β2int )−1/2 and viewing angleΘ will be: Γmin = (β2app + 1)1/2 cos θmax = ( β2app − 1) / (β2app + 1) IAU Symposium 324 on BH astrophysics Ljubljana, 2016 Sep 13

European VLBI Network (EVN) observations Initial real-time e-VLBI observations to establish strategy Deep follow-up observations at 5 epochs within three years Choose 5 GHz for excellent astrometry, great sensitivity and longer source detectability (as opposed to high frequencies) Central Processor: JIVE, Dwingeloo, NL The main reference source source was ICRF J1638+5720, 55 arcmin away Bright blazars often vary and have unstable cores – must be careful! Ljubljana, 2016 Sep 13 IAU Symposium 324 on BH astrophysics

Observational strategy Blabla Calibration of faint sources in VLBI: phase-referencing Swift J1644+5734: in-beam phase-referencing (for small dishes), to minimize phase-referencing errors ICRF J1638+5720 ~55 arcmin FIRST J1644+5736: Confirmed by short e-VLBI observations Small dish beam Narrow-beam telescopes (Wb, Ef, Jb1) Nodding observations 2.8 arcmin Swift J1644+5734 Ljubljana, 2016 Sep 13 IAU Symposium 324 on BH astrophysics

The target field with VLBI resolution Ljubljana, 2016 Sep 13 IAU Symposium 324 on BH astrophysics

Ultra-high precision astrometry ICRF frame: standard deviation is 50 μas in RA and 260 μas in DEC; similar to Berger et al. (2012) TDE-FIRST source relative astrometry: 13 μas in RA and 11 μas in DEC – best ever achieved with the EVN for a continuum source Ljubljana, 2016 Sep 13 IAU Symposium 324 on BH astrophysics

Strong constraint on proper motion => Small viewing angle If Γjet = 2 (Zauderer et al. 2013) , then Θv< 3° (“Tip of the iceberg”, or “cosmic conspiracy”?) => Or strong deceleration Γjet ≤ 2, due to dense circum-nuclear medium / no constraint on viewing angle. ncnm ≥ 5 Eiso,54 cm-1 at radius ~1pc Ljubljana, 2016 Sep 13 IAU Symposium 324 on BH astrophysics

Supporting alternative views? Sadowski & Natarayan (2015) Kara et al. (2016) Highly super-Eddington, fully radiative pressure driven jets can explain the high luminosity jets in (most) TDE and ULXs βint ~ 0.3c X-rays may be a result of reverberation off a super-Eddington accretion flow, not dominated by a jet. No relativistic jet is needed to explain X-rays (but what about the transient radio emission?) Ljubljana, 2016 Sep 13 IAU Symposium 324 on BH astrophysics

IAU Symposium 324 on BH astrophysics The case of ASASSN-14LI Relativistic jet from an off-axis thermal TDE? But note pre-existing AGN Image reliability issues: faint structure to be confirmed At odds with van Velzen+16 claim of jet deceleration within 0.1 pc? Romero-Canizales et al. 2016 arXiv 1609.00010v1 Ljubljana, 2016 Sep 13 IAU Symposium 324 on BH astrophysics

IAU Symposium 324 on BH astrophysics Concluding remarks Knowledge of jet efficiency and typical Lorentz factor is important to be able to predict TDE rates Donnarumma et al. (2015) predicts TDE will be a unique probe of quiescent SMBH at high redshifts, especially in the low-mass tail of the SMBH mass function (LTDE  MBH−1/2)! Future surveys in the optical (LSST), X-rays, radio (SKA) have great potential to detect a large number of events VLBI and especially when SKA1-MID added as a phased array will be a great tool to study jetted TDE (SKA-VLBI, Paragi et al. 2015) Ljubljana, 2016 Sep 13 IAU Symposium 324 on BH astrophysics