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New tricks for a mature observatory: Chandra HETG/HRC-I observations of TW Hya probe the structure of accretion Hans Moritz Günther

New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

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Page 1: New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

New tricks for a mature observatory:

Chandra HETG/HRC-I observations of TW Hya probe

the structure of accretion

Hans Moritz Günther

Page 2: New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

Phases of star formation

Artist: McCaughrean

Page 3: New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

Classical T Tauri stars

Günther (2013)

Andrews et al.ApJL (2016)

Page 4: New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

He-like triplets

Günther et al., A&A (2006)

Page 5: New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

The accretion model

● 1D stationary

● optically thin

● no heat conduction

● Maxwell velocity distribution (different temperature for electrons / ions)

● magnetic field does not change dynamics

● non-equilibrium ionisation calculation

Günther et al., A&A (2008)Günther, AN (2011)

Page 6: New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

Problems with current models: Accretion interacts with the star

Brickhouse et al. ApJ (2010)Brickhouse et al. ApJ (2012)

Can we resolve the line kinematically?Can we measure time-resolved properties?

Page 7: New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

HST/COS

But, what do the X-rays do?

Page 8: New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

Multi-wavelength campaign of contemporaneous observations

● Chandra● HST/COS● Magellan/FIRE● FLWO/TRES● El-Trigre● SSO● ...

Page 9: New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

HETG/HRC-I: Why?

● ACIS-S contamination increases

● Energies < 1 keV hard to see● LETG has lower resolving

power● HETG/HRC-I might be best

combination for certain science targets:

– Need for best resolution

– Need to lines < 1 keV

– Line dominated spectrum

● No order-sorting– Order confusion– Higher background

(but less than HRC-S)

– HRC-I is flat

Page 10: New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

HETG/HRC-I: Status

● NOT a standard product in CIAO <= 4.12

● But can be reduced with CIAO tools with some monkeying

● Working on associated CALDB files, but might require custom RMFs

● MIGHT be fully supported in the future

Page 11: New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

TW Hya: Triplets with Chandra

O VII high density r i f

Ne IX: r i f high density

Page 12: New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

TW Hya: Changes in density

Ne IX: r i f high density

Page 13: New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

● Non-accreting TTS have two component C IV lines (Ardila et al. 2013)

How can we explain the C IV (and other hot ion line) shapes?

Page 14: New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

● Pre-shock: freefall velocity

● Post-shock: tubulence, <¼ freefall velocity

How can we explain the C IV (and other hot ion line) shapes?

Page 15: New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

● Splatter: turbulent, variablebulk < 100 km/sabsorbtion

How can we explain the C IV (and other hot ion line) shapes?

Page 16: New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

● Heated photosphere: 20,000 Kvaries with accretion

How can we explain the C IV (and other hot ion line) shapes?

Page 17: New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

C IV line profiles

Page 18: New tricks for a mature observatory: Chandra HETG/HRC-I … · 2019. 12. 16. · The accretion model 1D stationary optically thin no heat conduction Maxwell velocity distribution

Summary

● Use HETG/HRC-I for effective area < 1 keV

● Calibration / data reduction is experimental at this point

● TW Hya has variable f/i ratio

● C IV line profiles can be explained with combination of accretion and outflow