G GMVA a A and S SMA O A Obser ervations o of M M 8 87 And S - - PowerPoint PPT Presentation

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G GMVA a A and S SMA O A Obser ervations o of M M 8 87 And S - - PowerPoint PPT Presentation

G GMVA a A and S SMA O A Obser ervations o of M M 8 87 And S An Status R Rep eport o of t the G e GLT P Projec ject Asada, K., Nakamura, M., Pu, H.-Y., et al. (ASIAA)) ~ 10 r s Academia Sinica, Institute of Astronomy and


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G GMVA a A and S SMA O A Obser ervations o

  • f M

M 8 87 An And S Status R Rep eport o

  • f t

the G e GLT P Projec ject

Asada, K., Nakamura, M., Pu, H.-Y., et al. (ASIAA))

~ 10 rs

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Academia Sinica, Institute of Astronomy and Astrophysics

  • Research Manpower:

42 research faculty 43 engineers 57 postdocs/contracted persons + students and administrative stuffs

  • Research Topics:

Extragalactic/Star Formation/

Interstellar Medium/Dust/Cosmology/ Planetary Sciences/radio and op<cal instrumenta<ons

  • Research Projects:

SMA/TAOS I, II/Computa<onal astronomy/

AMiBA/CFHT/SUBARU/ALMA/GLT, JCMT/VLBI

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Outline of this talk

  • Introduction of M 87 and GLT
  • Mass Accretion rate of M 8

87 with SMA observations

  • Collimation of M 8

87 jet with VLBI observations

  • Acceleration of M 8

87 jet with VLBI observations

Asada, K. & Nakamura, M. 2012, ApJ, 745, 28 Nakamura, M. and Asada, K. 2013, ApJ, 775, 118 Asada, K., Nakamura, M., and Pu, H.-Y. to be submitted Asada, K. et al. in prep. Nakamura, M. and Asada, K. 2013, ApJ, 775, 118 Asada, K. et al. 2014, ApJL, 781, 2 Kuo, C.Y., Asada, K. et al. 2014, ApJL, 783, 33 Asada, K., Rao, R., et al. in prep.

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Introduction

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Importance of M 87

  • 2nd brightest galaxy in Virgo cluster
  • Large BH mass
  • One of the nearest AGN
  • 2nd largest apparent size of rs (radius of non-rotating BH)

□ M 87 (Virgo A*)

1 mas = 0.074pc (= 125 rs)

Gebhardt and Thomas 09, 11 (e.g. Ford+94, Harms+ 94, Walsh 2013)

BH mass: 6 (3)× 109 M Distance: 16.7 Mpc

Jordan et al. 2005, ApJ, 634, 1002

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1st Discovered relativistic jet

□ M 87 (Virgo A*)

  • arcmin (~ 107 rs) to sub-mas (~ 10 rs)

Resolution:

  • Radio – optical – X-ray – γ-ray

Frequency: radio Optical X

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Low-Luminosity AGN

  • LX ~ 7 × 1040 erg s-1

Di MaVeo et al. 2003, ApJ, 582,133

  • With Chandra Observa<on

It’s sub-eddington, and Probably has a Radiatvely Inefficient Accre<on Flow (RIAF)

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X- and γ- ray flare

Chandra HST-1 Chandra core VLBA core VLA core VLA HST-1

Abramowski+ 2012 core core

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X- and γ- ray flare

Chandra HST-1 Chandra core VLBA core VLA core VLA HST-1

Abramowski+ 2012 HST-1

  • 1

Giroleb+ 2012, A&A, 538, L10 Hada+ 2014, ApJ, 788, 165

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Location of the Central Engine

Hada+ 2011, Nature, 477, 185

Central engine is located at (41±12) µas (6±2 Rs) eastward of the 43-GHz radio core.

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  • 1st discovered relativistic jet
  • Low-Luminosity AGN
  • High Energy activities
  • 2nd largest apparent size of rs (radius of non-rotating BH)

□ M 87 (Virgo A*)

Importance of M 87

Cur<s 1918, Publica<ons of Lick Observatory 13, 31 Typical AGN with radia<vely inefficient accre<on flow (RIAF) Up to TeV gamma-ray Miss-aligned Blaser?

It contains all contents of AGN !! Best Source to understand AGN !!

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Goal of the Greenland Telescope Project

PdBI IRAM 30 m LMT

Primary objec<ve: Image a shadow of black hole

  • f M 87 with sub-millimeter VLBI observa<on

includes Greenland Telescope, SMA/JCMT and phased ALMA at 230, 345 GHz and higher frequency.

From “INTERSTELLAR”

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Logistics of Greenland

  • Peak of the Greenland ice cap (3,200 m) at 72°35'46.4"N 38°25'19.1”W
  • Sponsored by the NSF, operated by CH2M Hill Polar Services (CPS)
  • Camp population: 5 (winter) up to 50 (summer)
  • Air National Guard provides LC-130 aircraft, twin otter aircraft or traverse.
  • Network: Satellite link
  • We have accessed the Summit Station since 2011 for the site testing.

Our radiometer at the site

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Logistics of Greenland

  • Peak of the Greenland ice cap (3,200 m) at 72°35'46.4"N 38°25'19.1”W
  • Sponsored by the NSF, operated by CH2M Hill Polar Services (CPS)
  • Camp population: 5 (winter) up to 50 (summer)
  • Air National Guard provides LC-130 aircraft, twin otter aircraft or traverse.
  • Network: Satellite link
  • We have accessed the Summit Station since 2011 for the site testing.

Our radiometer at the site

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Logistics of Greenland

  • Peak of the Greenland ice cap (3,200 m) at 72°35'46.4"N 38°25'19.1”W
  • Sponsored by the NSF, operated by CH2M Hill Polar Services (CPS)
  • Camp population: 5 (winter) up to 50 (summer)
  • Air National Guard provides LC-130 aircraft, twin otter aircraft or traverse.
  • Network: Satellite link
  • We have accessed the Summit Station since 2011 for the site testing.

Our radiometer at the site

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Logistics of Greenland

  • Peak of the Greenland ice cap (3,200 m) at 72°35'46.4"N 38°25'19.1”W
  • Sponsored by the NSF, operated by CH2M Hill Polar Services (CPS)
  • Camp population: 5 (winter) up to 50 (summer)
  • Air National Guard provides LC-130 aircraft, twin otter aircraft or traverse.
  • Network: Satellite link
  • We have accessed the Summit Station since 2011 for the site testing.

Our radiometer at the site

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Plan for 2016 and beyond

  • Antenna shipping to Thule (2016).
  • Antenna re-assemble and test at Thule, including VLBI test

(2016-2019).

  • Single-dish & VLBI first light at Thule (2017-2018).
  • Transport antenna across ice sheet (2019).
  • First light at the Summit Station (2019/20).
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Accretion flow onto SMBH of M 87

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M 87 and its Accretion Flows

  • Low-Luminosity AGNs are subclass of AGN. (L < 10-3 Ledd)
  • LLAGNs (Ho et al. 1997) are considered to accommodate RIAF
  • M 87 is categorized as LLAGN.

LLAGN No Big Blue Bump

(Ho et al. 2009)

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Accretion flow of LLAGNs

Three types of RIAFs:

ADAF

(Ichimaru 1977; Narayan & Yi 1995)

ADIOS

(Blandford & Begelman 1999)

CDAF

(Igumenshchev & Abramowicz 1999)

Structure

M

~ (r/rB)0 ~ (r/rB)0-1 ~ (r/rB)1

rB: Bondi radius (~ 104-6 rs)

  • Substan<al decrease of the mass accre<on rate

can be expected for ADIOS and CDAF !!

Mass Accre<on Rate is fundamental parameter to consider energy balance between Lacc and Lrad or Ljet.

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Probing Accretion Flow with SED fitting

Yuan et al. 2003 (e.g., Narayan et al. 1995; Manmoto et al. 1997)

M ~ 4 × 10-8 M yr-1

SED can be contaminated/dominated by jet….

  • Very succeeded method for Sgr A*
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Probing Accretion Flow with Faraday Rotation

BH Observer

n(r) ∼ ( r rs )−β T(r) ∼ ( r rs )−1

β = 1/2 (ADAF) = 3/2 (CDAF) = 1/2 − 3/2 (ADIOS)

With RIAF model:

Marrone et al. 2006, ApJ, 640, 308

Polarized emission (innermost AF or Jet) ~ 1012 K Magnetized Plasma (RIAF) ~ 107-9 K

Agol 2000, Quataert & Gruzinov 2000, Bower et al. 2003, Marrone et al. 2006, Macquart et al. 2006

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SMA Polarimetry towards Sgr A*

RM observa<on with SMA towards Sgr A*

  • RM = (5.6 ± 0.7) × 105 rad m-2

M = 2 × 10-7 - 2 × 10-9 M yr-1

Marrone et al. 2006, ApJ, 640, 308

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In the case of M 87

  • Apply the same scheme to M 87
  • rB ~ 230 pc (3 × 105 rs)
  • PB ~ 7 × 1045 erg s-1
  • MB ~ 0.12 M yr-1
  • With Chandra Observa<on

Di MaVeo et al. 2003, ApJ, 582,133

Back light would be innermost jet, not AF

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RM fitting towards M 87

EVPA [degree] λ2 [mm2]

2014, Jan. 09 2014, Feb. 28 2013, Jan. 27 2014, May 13

  • 2.1 × 105 rad m-2

1.5 × 105 rad m-2

  • 1.9 × 105 rad m-2
  • 3.2 × 105 rad m-2

Preliminary

12 mon. 1.5 mon. 3 mon.

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Mean RM and Mass accretion rate

Assuming no time variation,

<RM> = (-1.8 ± 0.3) × 105 rad m-2 !! First “soli lid d detection” n” of RM !! M = (3.6 ± 1.1) × 10-4 M yr-1 (at 21 rs) M = (2.9 ± 0.9) × 10-3 MB (at 21 rs)

Our “ALMA b band nd 3 3” and “SMA at 230 and 345 GHz”

  • bservations were conducted in 2015!!
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RM fitting towards M 87

R/Rs ˙ M/ ˙ MB Pj/η ˙ MBc2

BAF / ADAF GADAF C D A F

2D HD sim. 3D MHD sim. 1 101 102 103 104 105 10-6 10-5 10-4 10-3 10-2 10-1 1 Jet power

ADIOS

Substan<al decrease of the mass accre<on rate. Probably very strong constraint on RIAF !!

M = (2.9 ± 0.9) × 10-3 MB (at 21 rs)

This work!!

Pang et al. 2011, MNRAS, 415, 1228 Yuan et al. 2012, ApJ, 761, 130

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Comparison with Jet Power

Accre<ng Power :Pacc (= Mc2) ~ 2 × 1043 erg s-1

Li+ 2009, ApJ, 699, 513

Even if 10 % of Pacc used for jet, it’s slightly smaller than Ljet Another possibili<es to support jet power: Jet would be supported by “BH spin” !!

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Collimation of M 87 jet

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Bondi radius ISCO VLBA at 43 GHz VLBA at 15 GHz EVN at 1.6 GHz MERLIN at 1.6 GHz

Revisit structure of M 87 jet

(a) MERLIN image at 1.6 GHz (b) EVN image at 1.6 GHz (c) VLBA image at 15 GHz

  • Jet can described with two power-law lines

Parabolic stream with z = r1.7 ( - 105 rs) Conical stream with z = r1 (105 rs – )

  • Transition at ~ 105 rs !!

Parabolic MERLIN at 1.6 GHz EVN at 1.6 GHz VLBA at 15 GHz Conical Asada & Nakamura 2012, ApJ, 745, 28

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Bondi radius ISCO VLBA at 43 GHz VLBA at 15 GHz EVN at 1.6 GHz MERLIN at 1.6 GHz

Revisit structure of M 87 jet

Parabolic Conical

VLBA core at 43 GHz VLBA core at 86 GHz

VLBA 86 GHz

  • VLBI core = innermost jet with

τ = 1 surface at observing freq.

Nakamura and KA 2013, ApJ, 775, 118

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Bondi radius ISCO VLBA at 43 GHz VLBA at 15 GHz EVN at 1.6 GHz MERLIN at 1.6 GHz

Revisit structure of M 87 jet

Parabolic Conical Doeleman et al. 2012 Science, 338, 355 Size ~ 40 µas

VLBA core at 43 GHz VLBA core at 86 GHz VLBI core at 230 GHz

  • VLBI core = innermost jet with

τ = 1 surface at observing freq.

  • Same power-law index for 6 order !!

Nakamura and KA 2013, ApJ, 775, 118

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Revisit structure of M 87 jet

VLBA at 43 GHz (Asada & Nakamura 2012) VLBA at 15 GHz (Asada & Nakamura 2012) EVN at 1.6 GHz (Asada & Nakamura 2012) VLBA core at 43 GHz (Nakamura & Asada 2013) VLBA core at 86 GHz (Nakamura & Asada 2013) EHT core at 230 GHz (Doeleman et al. 2013) VLBA core (Hada et al. 2013)

Core shiz results (Hada et al. 2011) + Core size measurements

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VSOP images

Innermost jet: Three ridges are clearly seen. Presumably “Spine” and “Sheath”. Downstream of jet: Only two ridges and central dim.

3 days difference

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Bondi radius ISCO VLBA at 43 GHz (Asada & Nakamura 2012) VLBA at 15 GHz (Asada & Nakamura 2012) EVN at 1.6 GHz (Asada & Nakamura 2012) VLBA core at 43 GHz (Nakamura & Asada 2013) VLBA core at 86 GHz (Nakamura & Asada 2013) EHT core at 230 GHz (Doeleman et al. 2013) VLBA core (Hada et al. 2013) VSOP central ridge at 5 GHz (Asada et al. to be submitted) VSOP central dim at 5 GHz (Asada et al.to be submitted) VSOP sheath at 5 GHz (Asada et al. to be submitted)

Updated Streamline with VSOP image

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GMVA image

Possible bump !!

~ 10 rs

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Acceleration of M 87 jet

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Kovalev et al. 2007: VLBA at 15 GHz Reid et al. 1989: Gloabal VLBI at 1.6 GHz Cheung et al. 2007: VLBA at 1.6 GHz Biretta et al. 1999: HST Biretta et al. 1995: VLA at 15 GHz Ly et al. 2007; VLBA 43 GHz (area) Walker et al. 2008: VLBA 43 GHz Acciari et al. 2009: VLBA 43 GHz

HST monitoring (Biretta+99) 0.84 - 6.14 c (for HST-1) 2.7 - 5.1 c (for knot D) 3.9 c (for knot E) VLA monitoring (Biretta+95) 0.41 - 2.51 c (for knot D) 0.48 - 0.51 c (for knot A) 0.62 - 1.25 c (for knot B) VLBA monitoring (Kovalev+07) 0.00 - 0.05 c (< 21 mas) VLBI monitoring (Reid+89) 0.28 c (knot L) VLBA monitoring (Junor & Biretta 95) 0.01 c (< 21 mas) VLBA monitoring (Chueng+07) 0.47 - 4.3 c (HST-1)

HST-1 D E ABC D E F A B C HST-1

Merlin image EVN image

10 arcsec 100 mas

Velocity Field of the M 87 jet

???

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Three epoch EVN and Merlin observations at 1.6 GHz from 2007 March to 2009 March. HST-1

EVN observations

No proper motions within 160 mas from the core. Superluminal motions of 2.5 - 3.5 c in HST-1 region.

De Detection o n of p proper mo motions ns b between 1 n 160 ma mas a and nd H HST-1

  • 1 !

!!

Asada, K. et al. 2014, ApJL, 781, 2

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Kovalev et al. 2007: VLBA at 15 GHz Reid et al. 1989: Gloabal VLBI at 1.6 GHz Cheung et al. 2007: VLBA at 1.6 GHz Biretta et al. 1999: HST Biretta et al. 1995: VLA at 15 GHz Ly et al. 2007; VLBA 43 GHz (area) Walker et al. 2008: VLBA 43 GHz Acciari et al. 2009: VLBA 43 GHz

Updated Velocity Field of M 87 jet

Asada, K. et al. 2014, ApJL, 781, 2

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Superluminal motions upstream of HST-1 for the first time !! This velocity field is a direct evidence for the acceleration region !!

Updated Velocity Field of M 87 jet

Kovalev et al. 2007: VLBA at 15 GHz Reid et al. 1989: Gloabal VLBI at 1.6 GHz Cheung et al. 2007: VLBA at 1.6 GHz Biretta et al. 1999: HST Biretta et al. 1995: VLA at 15 GHz Ly et al. 2007; VLBA 43 GHz (area) Walker et al. 2008: VLBA 43 GHz Acciari et al. 2009: VLBA 43 GHz This work: EVN at 1.6 GHz

Asada, K. et al. 2014, ApJL, 781, 2

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Updated Velocity Field of M 87 jet

Kovalev et al. 2007: VLBA at 15 GHz Reid et al. 1989: Gloabal VLBI at 1.6 GHz Cheung et al. 2007: VLBA at 1.6 GHz Biretta et al. 1999: HST Biretta et al. 1995: VLA at 15 GHz Ly et al. 2007; VLBA 43 GHz (area) Walker et al. 2008: VLBA 43 GHz Acciari et al. 2009: VLBA 43 GHz This work: EVN at 1.6 GHz

[Γ – 1] Asada, K. et al. 2014, ApJL, 781, 2

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Kovalev et al. 2007: VLBA at 15 GHz Reid et al. 1989: Gloabal VLBI at 1.6 GHz Cheung et al. 2007: VLBA at 1.6 GHz Biretta et al. 1999: HST Biretta et al. 1995: VLA at 15 GHz Ly et al. 2007; VLBA 43 GHz (area) Walker et al. 2008: VLBA 43 GHz Acciari et al. 2009: VLBA 43 GHz This work: EVN at 1.6 GHz

HST-1 D E ABC

Streamline and Acceleration of the jet

VLBA at 43 GHz VLBA at 15 GHz EVN at 1.6 GHz MERLIN at 1.6 GHz ISCO Bondi radius

distance from the core z [r ] jet radius r [r ]

s s

Asada & Nakamura 2012, ApJ, 745, 28

Nakamura & Asada 2013, ApJ,

Vz ∝ Z 2/α Γ ∝ Z (α-1)/α

Komissarov et al. 2009 MNRAS, 394, 1182

In rela<vis<c regime, In non- rela<vis<c regime,

Z (α-1)/α

α: power-law index of streamline (= 1.7)

Vz ∝ Z 2/α Asada, K. et al. 2014, ApJL, 781, 2

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Summary

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Summary

  • SMA polarimetry to measure RM associated with AF of M 87
  • M is es<mated to be 3.6 ± 1.1 × 10-4 M yr-1
  • M is substan<ally decreased, consistent with CDAF/ADIOS
  • Accre<ng Power may not be enough to support Kine<c Power of Jet.
  • VLBI observa<ons to probe accelera<on and collima<on proper<es
  • Parabolic streamline up to 105 rs, while conical streamline beyond.
  • Transi<on is corresponds to Bondi radius
  • Gradual accelera<on of proper mo<ons up to 105 rs as well.
  • Simultaneous accelera<on and collima<on indicates MHD mechanism
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Extra

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The same food with different way of eating

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