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NextNext GenerationGeneration VLBIVLBI

Michael Bietenholz York University TheThe RoleRole ofof VLBIVLBI

• Resolution! VLBI provides a resolution which cannot be routinely matched in any other band, typically 1 milliarcsec at 5 GHz, down to 20 micro-arcsec at 345 GHz • Sensitive to high brightness temperatures and thus mostly non- thermal emission. Radio is relatively extinction-free • Very wide range of science applications: AGN, explosive events (FRB, GRB, SNe, TDE...), masers, pulsars, radio stars • Astrometry: parallaxes, proper motions, ICRF • Canada was a pioneer in VLBI (Penticton & Algonquin, 1967) VLBI Developments • More VLBI-capable telescopes coming online: . MeerKAT / South Africa . ASKAP / Australia . African VLBI Network Sicaya, Peru . FAST / China • Sicaya / Peru Kuntunse, Ghana • Space-VLBI: Millimetron (Spektr-M) project • Calibration strategies (multi-view, wide-field observations with in-beam calibrators) millimetron.ru • Higher recording bandwidths • Using remote atomic clocks over optical fibre links

MeerKAT, South Africa FAST, China VLBI Astrometry

• Phase-referenced differential astrometry with VLBI today can measure positions with ~10 micro-arcsec or better • With SKA-1: accuracies of 3~5 micro-arcsec; parallaxes of ~4% out to Galactic centre; proper motions of 0.2 km/s in one year at 2 kpc • Accuracy better than that obtainable with GAIA • VLBI astrometry may be required to accurately calibrate GAIA parallaxes • VLBI is not affected by dust: can do Galactic centre and star-forming regions • VLBI is only feasible for brightness temperatures > 107 K, in other words, mostly non-thermal sources like masers, chromospherically active young stars (mostly low-mass), pulsars (and AGN; GAIA will see largely stars) • VLBI measurements allow – tomographic mapping of the star-forming regions and of the Galaxy. – Parallax accuracy at 3 kpc (~50pc) are sufficient to resolve structure in spiral arms which have widths of ~100's of pc VLBI of Galactic Sources

• Many of the sources (active stars, pulsars) are relatively faint. • Sensitive, long baselines, such as provided by MeerKAT or SKA with either European or Australian antennas, are crucial for astrometry of Galactic sources

Figure: a simulated population of 12 GHz masers

van Langevelde & Quiroga-Nu ñes Astrometry of Galactic Masers and Pulsars

• Early results from Reid et al. 2010 • Trigonometric parallaxes to masers in Galactic star-forming regions. Distance error bars mostly smaller than dots! 12 GHz Methanol masers

H2O masers

Reid et al 2009; Galaxy image R. Hurt: Pulsar Proper Motions

• Observing pulsars near the Galactic centre will allow tests of , determine the mass of the Galactic centre as well as characterize the interstellar medium near the Galactic centre • Accurate positions and proper motions (as well as pulsar timing) will be key to these science goals • Although many are expected to exist, none have so far been detected, so any pulsars near Galactic centre will be faint • Pulsars in the rest of the Galaxy have high proper Proper motion of the Galactic centre magnetar, motions (~250 km/s) thought to PSR J1745-2900, at only 0.1 pc from Sgr A*, be due to an initial "kick" measured by VLBI (Bower et al 2015) Scattering: Pico-arcsec Astrometry

Figure: Ue-Li Pen

 Radiation from pulsars is scattered and reaches the Earth via multi-path propagation. Recent VLBI observations (Brisken et al 2010) have shown that it is possible to use this scattering screen as a billion-km baseline, and resolve motions of ~50 pico-arcsecs (Pen et al 2014)  Low frequency: Penticton & Algonquin  Pulsar binary orbits  Pulsar magnetosphere structure  ISM structure  Pulsar timing arrays (obtain distances) VLBI for Transients Speed Distance Typical for … Angular velocity 20 km/s 10 kpc Star 0.4 mas/yr

5000 Nova, Cataclysmic 10 kpc 2 mas/week km/s Variable c 10 kpc Relativistic 0.7 mas/hour 20000 10 Mpc Supernova 0.4 mas/yr km/s c 100 Mpc Relativistic 0.6 mas/yr

VLBI follow-up will be crucial for determining the proper motions (including expansion) expected in a wide range of transients. Short transients are expected to be small because of light-travel time arguments, and thus of scales for which VLBI resolution is required for followup Recurrent Nova RS Ophiuci O’Brien et al. 2006 Relativistic Expansion: Gamma-Ray

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GRB 030329 was associated with supernova 2003dh VLBI measurements: by Taylor, Pihlstrom et al. show clear super-luminal motion, and then deceleration, with transition to non-relativistic regime at t ~1yr SN 1986J: Black Hole with Jets?

Speculative cartoon: 2003 Contours, red: 5 GHz Blue → white: 15 GHz

2014 5 GHz

• Could SN 1986J host an accreting black hole with jets, where the jets produce the NE hot-spot and the faint SW extension?

Bietenholz & Bartel, 2017 SN 1986J: Black Hole with Jets?

Speculative cartoon: 2003 Contours, red: 5 GHz Blue → white: 15 GHz

2014 5 GHz

• Could SN 1986J host an accreting black hole with jets, where the jets produce the NE hot-spot and the faint SW extension?

More generally: GRB & SN morphology, CSM structure, relation to SNe VLBI for Transients: Example • The most energetic known neutrino (2 PeV) was detected by the IceCube Neutrino Observatory at the South Pole in Dec 2012. It was officially called HESE-35, but known as "Big Bird" • A single particle – about as transient as you can get! • VLBI observations were crucial in identifying a variable PKS B1424-418 (z = 1.52) as the origin of Big Bird (Kadler et al., 2016) Image: IceCube Collaboration. Gravitational Lensing

• We’re on the verge of a z = 3.2 huge increase in source

known gravitational zlens = 0.35 lenses with Euclid LSST in optical/IR and ASKAP, MeerKAT, SKA in radio (Lens not • SKA1 MID will detect visible in 5 radio) 10 new, radio-loud M

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galaxy as well as dark matter profile Telescope

Sgr A*

Image: H. Falcke Use mm-wave (350 GHz) VLBI to obtain highest of SgrA*, M87 and other nearby SMBH: image black hole shadow