HD 100453: An Evolutionary link between
Download
Report
Transcript HD 100453: An Evolutionary link between
HD 100453
An Evolutionary Link Between
Protoplanetary Disks
and Debris Disks
Karen Collins
Master’s Thesis Defense
April 24th, 2008
University of Louisville
Department of Physics and Astronomy
Supported by a Fellowship from the Kentucky Space Grant Consortium
Thesis Directors
Dr. Gerard Williger - UofL
Dr. Carol Grady - NASA GSFC
Journal Paper Co-authors
Co-authors(s)
Affiliation
Contribution
C. A. Grady
Eureka Scientific and NASA GSFC
overall direction, science mentor, HST and Chandra PI, and day-to-day support
K. Hamaguchi & R. Petre
X-ray Astrophysics Laboratory
NASA/GSFC
Chandra observations, data reduction, and results
J. P. Wisniewski
NASA/GSFC, NPP Fellow
HST ACS HRC observations, data reduction, and results
S. Brittain
Clemson University
Gemini South observations of warm CO, data reduction, and results
M. Sitko & W. J. Carpenter
SSI, University of Cincinnati
SED and modeling data, general support
G. M. Williger
University of Louisville
FUSE observations, data reduction, results, and general day-to-day support
R. van Boekel
Max-Planck-Institut für Astronomie
VLT NACO NIR observations, data reduction, common proper motion results, and
related photometric results
A. Carmona
Max-Planck-Institut für Astronomie,
ESO, ISDC & Geneva Observatory
VLT SINFONI NIR spectroscopy, data reduction, spectral typing, and other related
results.
M. E. van den Ancker
European Southern Observatory
VLT SINFONI NIR spectroscopy, data reduction, spectral typing, and other related
results.
G. Meeus
Astrophysikalisches Institut Potsdam
FEROS Ca II spectroscopic data
J. P. Williams,
G. S. Mathews
University of Hawaii
JCMT HARP CO spectroscopic observations, data reduction, dust mass calculations,
gas mass calculations, and related results
X. P. Chen
Max-Planck-Institut für Astronomie
VLT NACO Brγ common proper motion data reduction
B. E. Woodgate
NASA/GSFC
overall scientific interpretation
Karen Collins
Master's Thesis Defense
4/24/2008
Star Formation Overview
Start with molecular cloud
Four phases of collapse
dense rotating core forms
collapses from inside out
bipolar outflows
carry away angular momen. (L)
star and disk revealed
Shu et al. 1987
Conservation of L
cloud rotates slowly
star rotates more rapidly
High L material forms disk
disk accretes onto star
Wood 1997
Karen Collins
Master's Thesis Defense
4/24/2008
Pre-Main Sequence Stars
Pre-main sequence (PMS) stars
fully revealed stars
still gravitationally contracting toward main sequence
hydrogen fusion not started yet
PMS stars are called
T Tauri if
0.1 M < M < 2 M (M, K, G, F type stars)
Herbig Ae/Be if 2 M < M < 8 M (F, A, B type stars)
higher mass stars emerge from cloud on main sequence
Observable characteristics
Balmer emission lines in stellar spectrum (Hα, Hβ, Hγ, …)
transition (32, 42, 52, …)
infrared excess due to circumstellar dust (next slides)
Karen Collins
Master's Thesis Defense
4/24/2008
Spectral Energy Distribution
Spectral Energy Distribution (SED)
plot of radiated energy
vs. wavelength
Stellar photosphere
~blackbody
peaks in optical
Sun
5778 K
A-type stars
7500-10,000 K
M-type stars
3000-4000 K
Karen Collins
Master's Thesis Defense
4/24/2008
Infrared Excess
IR excess
total emission − stellar contribution
stellar contribution determined from a model fit to UV and Optical data
source is circumstellar dust
dust absorbs stellar radiation
re-radiates as thermal emission
IR excess source
inner disk
NIR (1 - 7 μm)
outer disk
MID to FIR (10 - 50 μm)
disk midplane
FIR to mm (>50 μm)
Karen Collins
adapted from M.Sitko simulation
Master's Thesis Defense
4/24/2008
Disk Evolution
Protoplanetary Disks (initial phase)
gas rich + small dust grains (submicron)
gas:dust ~100:1 (as in interstellar medium (ISM))
high accretion rates (> ~1108 M yr1)
gas and dust well mixed
hydrostatic equilibrium
dust material supported above midplane
disk can maintain scale height
disk expected to “flare”
Karen Collins
Master's Thesis Defense
4/24/2008
Flared Disk
"bowl" shaped disk
h r, where > 1.0
relatively flat SED in IR
inner rim NIR BB
disk surface MIR - FIR
disk midplane FIR - mm
Dullemond et al. 2006
Dullemond et al. 2006
Karen Collins
Master's Thesis Defense
4/24/2008
Disk Vertical Structure
inner-most part of the disk is dust free
beyond sublimation temperature
the inner rim is illuminated face-on from the star, the gas heats up
more and causes an increased scale height (i.e. it "puffs up")
as the disk ages, the dust grains grow in size
disk becomes vertically stratified
larger grains in midplane
smaller grains in upper layers
Dullemond et al. 2006
Karen Collins
Master's Thesis Defense
4/24/2008
Disk Evolution Continued
accretion rates ~10 - 100x lower than
protoplanetary disks
IR excess similar to pp disk at >10 μm
Van den Ancker 1999
Transitional Disks (intermediate phase)
Protoplanetary Disk
IR excess significantly less at <10 μm
result of less dust, or optically thin dust,
in the inner disk
Transitional Disk
photoevaporation
grain growth until optically thin
gap creation by massive planet
Karen Collins
Master's Thesis Defense
4/24/2008
Disk Evolution Continued
Protoplanetary Disk
Debris Disks (final phase)
accretion has stopped
moderate IR excess at >10 μm
very little to no IR excess at <10 μm
Transitional Disk
no inner disk at all
primordial dust has grown to rocks,
protoplanets, and terrestrial planets
remaining dust is second generation
gas-poor
Karen Collins
Master's Thesis Defense
Van den Ancker 1999
from collisions of massive bodies
Debris Disk
4/24/2008
Meeus Groups
Meeus et al. (2001) divided 14 Herbig stars into two groups
Group I
blackbody in MIR
high fraction of IR excess (LIR/L* ~ 0.5)
steep submm slope (i.e. small grains)
Group II
no blackbody in MIR
low fraction of IR excess (LIR/L* ~ 0.2)
shallow submm slope (i.e. larger grains)
Meeus et al. suggested Group I
sources evolve to Group II sources
Meeus et al. 2001
Karen Collins
Master's Thesis Defense
4/24/2008
Meeus Physical Model
3 components
disk midplane - optically thick
inner disk with scale height
outer disk
Group I
inner disk optically thin
outer disk is directly illuminated
outer disk heats & flares
creates MIR BB
Group II
inner disk optically thick
outer disk shielded
outer disk stays flat
no MIR BB
Karen Collins
Master's Thesis Defense
4/24/2008
Thesis Goal
Test idea that Meeus Group I sources
evolve to Meeus Group II sources
at time of Meeus et al. (2001) paper, many age
estimates were not available
accretion rates were not considered
(recall that accretion rate is tied to disk evolution)
Karen Collins
Master's Thesis Defense
4/24/2008
Thesis Approach
Compare ages and accretion rates between the groups
we focus on HD 100453 in this work because:
Herbig AeBe stars are difficult to date after about 5 Myr
low-mass stars are easier to date and often form together with A-stars
we can determine the age of the A-star from a companion low-mass star
a candidate low-mass companion was recently reported for HD 100453A
(Chen et al. 2006)
determine age and accretion rate for HD 100453A (this work)
determine age and accretion rate for other stars from the
literature
Karen Collins
Master's Thesis Defense
4/24/2008
HD 100453A
Southern Hemisphere
(Lower Centaurus-Crux Assn)
Distance 114 pc
v=7.78
(not visible by naked eye)
Spectral Type A9Ve
Age > ~10 Myr
Karen Collins
Master's Thesis Defense
4/24/2008
Summary of Observations
Instrument
Chandra
K. Hamaguchi
Direct
Image
HST ACS HRC
J. Wisniewski
HST ACS HRC
J. Wisniewski
HST ACS SBC
VLT NACO
C. Grady
K. Collins
R van Boekel
VLT SINFONI
A. Carmona
NIR
Spectral Type of Companion
FUSE
G.M. Williger
FUV
Accretion Rate
Phoenix
S. Brittain
NIR
Warm Gas Limits
JCMT HARP
J. Williams
G. Mathews
G. Meeus
K. Collins
Submm
Cold Gas Limits
Optical
Accretion Rate
FEROS
Karen Collins
Prime
Coron.
Image
Spectra
Wavelength
Scientific Purpose
X-ray
Accretion Rate
Optical
Companion Location &
Photometry
Optical
Disk Detection & Photometry
FUV
Companion Detection
NIR
Companion Proper Motion &
Photometry
Master's Thesis Defense
4/24/2008
Test of Companion Status
To date an A-star from a low-mass companion, we need to know
that they are physical companions
Two tests:
determine motion of A-star & candidate companion
If motion through space is common,
they are likely physical companions
determine spectral type of companion
for the brightness contrast between the two stars,
a physical companion would be a low-mass star
Karen Collins
Master's Thesis Defense
4/24/2008
The Candidate Companion
HST optical direct image
B located 1.05 @ 126° east of north
mv = 15.87 (A:B = 1500:1 contrast)
optical
HST ACS HRC F606W
Karen Collins
Master's Thesis Defense
4/24/2008
Candidate Companion Spectral Type
Need high spatial resolution spectroscopy
to separate the light from the two stars
Optical Spectroscopy is first choice
need A/O for ~1 separation
none available
NIR is good second choice
SINFONI on VLT with A/O
Integral Field Spectrograph
0.8 x 0.8 field of view
J, H, K band gratings (NIR)
Karen Collins
Master's Thesis Defense
4/24/2008
Candidate Companion Spectral Type
Compare to 4 standard stars
M3.5V
M4.0V
M4.5V
M5.0V
Find closest match to
features in all 3 bands
Spectral Type is
M4.0V - M4.5V
Karen Collins
Master's Thesis Defense
4/24/2008
Relative Proper Motion
Determine movement of A star over 3 years
Hipparcos data 0.111 ± 0.003
Determine relative motion of candidate companion over 3 years
use VLT NACO Brγ imagery
2003 data (Chen et al. 2006)
2006 data (this work)
compare change in position
of B w.r.t. A 0.020 ± 0.010
Common proper motion
confirmed
Residual could be
orbital motion
Karen Collins
Master's Thesis Defense
4/24/2008
Candidate Confirmation
Common proper motion
suggests both stars originated from same cloud
suggests physically companions
Spectral Type M4.0V - M4.5V
class “V” not a distant red giant (high luminosity)
A9:M4 has proper contrast ratio
Confirmation that candidate companion
is a physical companion
Karen Collins
Master's Thesis Defense
4/24/2008
Companion Photometry
Object
Mode
Filter
magnitude
HD 100453B
Direct
mF606W
15.6
HD 100453B
Coron
mF606W
15.8
HD 100453B
Combined
mF606W
15.7 0.2
Notes
(prime)
HST HRC
(J. Wisniewski)
HST HRC
(J. Wisniewski)
(J. Wisniewski)
HD 100453B
Direct
Ks
10.66 0.1
HD 100453B
Coron
L
10.13 0.1
HD 100453B
Coron
M
9.99 0.1
HD 100453B
Calculated
V
15.87 0.2
(Chen et al. 2006)
VLT NACO
(R. van Boekel)
VLT NACO
(R. van Boekel)
(K. Collins)
HD 100453B
Calculated
K
10.64 0.1
(K. Collins)
HD 100453B
Calculated
L
10.27 0.1
(K. Collins)
• Key Point: Candidate companion has NO IR Excess
Can use K-band in H-R diagram for age estimate
Karen Collins
Master's Thesis Defense
4/24/2008
Age Determination (from A-star)
PMS H-R diagram - derived from Siess et al. stellar models
if we know magnitude and effective temperature
we can determine age and mass
HD 100453A
mv = 7.7
A9Ve Teff = 7400 K
Results
age: 10 Myr - ZAMS
mass: 1.6 - 1.8 M
Age is not well constrained
because of compressed
isochrones at >10 Myr
Karen Collins
Master's Thesis Defense
4/24/2008
Age Determination (from Companion)
Note wider separation of isochrones for low-mass stars
HD 100453B (input data)
mK = 10.64 ± 0.1
M4.0V – M4.5V
Teff = 3300 K – 3400 K
Results (Siess Model)
age: 10 15 Myr
mass: 0.21 0.23 M
Results (Baraffe Model)
age: 11 18 Myr
mass: 0.24 0.30 M
Results (Combined)
age: 14 ± 4 Myr
mass: 0.21 0.30 M
Karen Collins
Master's Thesis Defense
4/24/2008
Mass Accretion onto A-star
Mass accretion rate gives insight into the
evolutionary phase of the disk
We investigate the following accretion indicators:
enhanced FUV continuum
Herbig-Haro knots in Lyα
enhanced emission of
Ca II λ8662 Å
Hard X-rays
Hα (6563 Å)
Brγ (2.166 μm)
Karen Collins
Master's Thesis Defense
4/24/2008
Accretion - FUV Continuum
FUV continuum upper limit
from FUSE spectra
<1.51015 ergs s1 cm2 Å1 (1σ)
(-14.8 in log space)
Karen Collins
Master's Thesis Defense
4/24/2008
Accretion - FUV Continuum
Plot accretion rate vs. FUV continuum
accretion rates based on Brγ
(Garcia Lopez et al. 2006)
FUV values from literature
note power law trend
except HD 100453
Karen Collins
Master's Thesis Defense
4/24/2008
Accretion - FUV Continuum
Plot accretion rate vs. FUV continuum
accretion rates based on Brγ
(Garcia Lopez et al. 2006)
FUV values from literature
note power law trend
except HD 100453
relocate HD 100453 to fit trend
log (Accr Rate) < -9.6
< 2.5x10-10 M yr-1 (1σ)
Stellar activity can also be a source of Brγ emission
HD 100453 Brγ emission is contaminated by stellar activity
Karen Collins
Master's Thesis Defense
4/24/2008
Accretion - Herbig-Haro Knots
HH knots from jets
FUV
Are Lyα bright in FUV
Use scaling argument
HD 163296 has HH knots
(Wassell et al. 2006)
F122M = 2.0 cnts s1 arcsec2
accretion ~1×107 M yr1
HD 100453 - no knots detected
HST ACS SBC F122M
3σ upper limit
<1.1x10-4 cnt s-1 arcsec-2
scaling ~<6×1011 M yr1
Karen Collins
Master's Thesis Defense
4/24/2008
Accretion- Ca II 8662 Å emission
Use scaling argument again
HD 163296
Ca II 8662 Å EW = 4.18 Å
(Hamann & Persson 1992)
accretion rate ~1×107 M yr1
(Wassel et al. 2006)
HD 100453
in absorption
find emission upper limit
Ca II 8662 Å EW <410-3 Å
assume linear relation
accretion rate <1×1010 M yr1 (4σ)
Karen Collins
Master's Thesis Defense
4/24/2008
Accretion - Hα
HD 100453 Hα emission
variable, weak
lowest EW of 91 Herbig Ae/Be stars
(Manoj et al. 2006)
at best a very weak accretor
Karen Collins
Master's Thesis Defense
4/24/2008
Accretion - X-ray
Chandra
In A-stars:
accretion produces hard X-rays
winds produce soft X-rays
HD 100453A produces soft X-rays
not a strong accretor
Chandra X-ray
HD 100453A
HD 100453B
energy (keV)
Karen Collins
1
red
0.35 − 0.70 keV
green 0.70 − 0.90 keV
blue 0.90 − 2.00 keV
2
Master's Thesis Defense
4/24/2008
Accretion Rate Summary
Accretion Indicator
Accretion Level
Significance
FUV Continuum
< 2.5×1010 M yr1
1
Lack of Ca II 8662 Å emission line
< 1.0×1010 M yr1
4
Lack of HH Knots in Ly
< ~6×1011 M yr1
factor of 10
weak accretor
not strong accretor
H
X-ray
Karen Collins
Master's Thesis Defense
4/24/2008
Constraints on Disk Structure
From Meeus et al. 2001, 2002
strong IR excess blackbody in NIR
inner rim < ~0.5 AU
From Habart et al. 2006
M. Sitko, private communication
spatially resolved PAH features
out to ~0".3 (~40 projected AU)
disk outer radius > ~40 AU
Habart et al. (2006)
Karen Collins
Master's Thesis Defense
4/24/2008
HST ACS Coronagraphy
Need ~1x106 contrast to image disk around A star
Use coronagraph to block light from central star
Use psf-subtraction to reduce remaining stray light
ACS HRC provides contrast of:
~1x105 in direct mode
~1x106 in coronagraphic mode
~1x107 in coronagraphic mode with psf-subtraction
HRC has 0".9 radius spot size, but psf-subtraction
residuals out to ~2-3"
Clampin et al. 2003
Karen Collins
Master's Thesis Defense
4/24/2008
Constraints on Disk Structure
HST ACS HRC Coron w/psf-sub
HD 100453 psf-subtracted
coronagraphic image
(HST ACS HRC F606W)
HD 100453
Limiting surface brightness from
azimuthally averaged radial profile
No detection of disk
in scattered light
psf residuals dominate to ~2-3"
scattered light disk < ~250 AU
Karen Collins
Master's Thesis Defense
4/24/2008
Constraints on Disk Structure
Third object in field
HST ACS - 2003 (red)
HST ACS - 2003 (red)
VLT NACO - 2006 (blue)
VLT NACO - 2006 (blue)
Overlay aligned by
diffraction spikes
B positioned according to
relative motion determined
previously
C has retrograde relative
motion compared to B
C proper motion ~ zero
Likely a background star
Disk is optically thin in the
optical and IR by a projected
distance of ~90 AU
Karen Collins
Master's Thesis Defense
4/24/2008
Disk Structure Summary
Line of Sight
Outer Edge Optically Thin
<90 proj. AU (star C)
Inner Rim
<0.5 AU (NIR BB)
A
Scattered Light
Outer Radius <250 AU
Companion
120 proj. AU
Outer Radius
>40 AU (PAH)
i?
B
Gap (SED dip)?
C
Karen Collins
Master's Thesis Defense
4/24/2008
Gas and Dust in Inner Disk
Carmona et al. (2008) found no evidence for
molecular hydrogen emission
upper limit of ~0.2 MJ of optically thin warm H2 (150 K)
upper limit of ~0.007 MJ of optically thin hot H2 (300 K and above)
NIR BB in SED hot dust
We detected no warm CO emission (4.97 μm)
unlike other HAeBe with
hot dust
Could have optically thick gas
in disk midplane
Low accretion rate suggests
little optically thick or thin gas
dust-rich gas-poor
inner disk
Karen Collins
(after Brittain et al. 2007)
Master's Thesis Defense
4/24/2008
Gas and Dust in Outer Disk
Cold gas (from submm emission line)
we found no CO J = 32 (868 m) emission toward HD 100453
cold gas mass of < 0.2 MJ (1000x depletion)
Cold dust (from mm continuum)
Strong 1.2 mm continuum flux of 265 mJy (Meeus et al. 2003)
cold dust mass ~0.1 MJ
Gas:dust upper limit is 2:1 (for 1000x depletion)
typical protoplanetary disk is 100:1 (like ISM)
Gas-poor outer disk
Karen Collins
Master's Thesis Defense
4/24/2008
Where Does It Belong?
14 ± 4 Myr transitional disk character
High NIR excess protoplanetary disk character
Low accretion rate transitional or debris disk character
Gas-poor disk debris disk character
High total IR excess flared disk? requires gas?
HD 100453A does not fit in any
classically defined disk group
(protoplanetary, transitional, debris)
Karen Collins
Master's Thesis Defense
4/24/2008
Thesis Results
Recall we set out to test idea that
Meeus Group I sources evolve to Group II ...
by comparing ages & accretion between the groups
determine for HD 100453
collect new and updated data from literature
Karen Collins
Master's Thesis Defense
4/24/2008
Thesis Results
Group I sources are
slightly older than
Group II on average
(but are within 1σ)
Group I accretion rates
are slightly lower than
Group II accretion rates
on average
(but are within 1σ)
Karen Collins
Master's Thesis Defense
4/24/2008
Thesis Results
Age range significantly
overlaps between the two
groups
Accretion slows as star ages
in both groups
Meeus suggested star and disk
evolution may be decoupled
for this sample
We find that the star, accretion rate, and disk evolve together.
We conclude that the hypothesis suggesting Meeus Group I
sources evolve to Meeus Group II sources does not hold.
Karen Collins
Master's Thesis Defense
4/24/2008
Possible Physical Explanation
HD 100546 example (Group I)
after Bouwman et al. 2003)
cavity confirmed by interferometry & STIS
(Lui et al. 2003) (Grady et al. 2005)
inner rim of inner and outer disk creates
NIR and MIR blackbody components in SED
and high Lexcess/L*
possible giant planet in gap is causing
collisional cascade
collisions produce small dust grains
radiation pressure blows the grains onto
surface of cold outer disk
small grains cause steep submm slope
Meeus groups may be more representative of differences in
disk structure rather than differences in disk evolution.
Karen Collins
Master's Thesis Defense
4/24/2008
Future Directions
To lift disk structure degeneracy allowed by SED
need high contrast, high spatial resolution imaging
high spatial resolution interferometry
NICMOS on HST (coron. imaging, 0.075 pixel1 , 0".3
hole)
My collaborators have submitted a proposal (March
2008) for NICMOS observations of several T Tauri
and Herbig Ae/Be stars, including HD 100453.
Near-term prospects
HST SM4 (8/2008) set to repair other key instruments
ACS (down since June 2006)
coron. imaging mode, 0.025 pixel1, 0".9 radius spot
STIS (down since 2004)
coron. imaging mode, 0.05 pixel1, 0".5-2.8" wedges
Karen Collins
Master's Thesis Defense
HD 141569 (from Krist 2004)
We can do this with existing instrumentation
4/24/2008
Long -Term Prospects
Atacama Large Millimeter Array (ALMA)
0.3 - 9.6 mm (cold dust and gas)
0".01 resolution, no occulter needed
64 x 12-meter antennas
completion expected in 2012
Simulation
0.5 M star
1 MJ planet
5 AU orbit
Mdisk = 10 MJ
Wolf & D'Angelo 2005
Karen Collins
Master's Thesis Defense
4/24/2008
Thank You!
A possible view of the HD 100453 system?
adapted from NASA/JPL-Caltech/T. Pyle (SSC)
Karen Collins
Master's Thesis Defense
4/24/2008