Radiative Transfer for Simulations of Stellar Envelope Convection
The Stellar Velocity Ellipsoid and Multi-component Stability of...
Transcript of The Stellar Velocity Ellipsoid and Multi-component Stability of...
Kyle B. WestfallKapteyn Astronomical Institute, Groningen, Netherlands
The Stellar Velocity Ellipsoidand Multi-component Stabilityof Galaxy Disks
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Dynamics of Disk Galaxies 24 Oct 2013, 서울
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Outline
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David R. Andersen (HIA)
Matthew A. Bershady (UW)
Thomas P. K. Martinsson (Leiden)
Robert A. Swaters (NOAO)
Marc A. W. Verheijen (Kapteyn)
Kyle B. Westfall (Kapteyn)
The DiskMass Survey Team
• The Stellar Velocity Ellipsoid (SVE)• What is it?• Extragalactic Measurement Approach• Our Data• A Stepwise Approach • A Holistic Model• A Tests of Accuracy• Comparison with the literature
• Disk (in)Stability and Star-formation
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Dynamics of Disk Galaxies 24 Oct 2013, 서울
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The Stellar Velocity Ellipsoid
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• Ideally, we want f (x,v).- This distribution is complex in
the Milky Way.
• Extragalactic measurements require some simplifying assumptions.
• Characterize f (x,v) by its velocity-dispersion tensor.
• The SVE is its 3D surface.
Vx
Vy
Vz
Dehnen (1998)
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SVE Assumptions
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SVE Assumptions
• Galaxy is steady-state, axially symmetric.
• No strong streaming motions.
• Eigenvectors of velocity-dispersion tensor aligned with {R,θ,z}. (No vertex deviations)
• First-order dynamical equations hold:- Epicycle Approximation (EA)
- Simplified Asymmetric Drift Equation (AD)
- Circular-speed from a gas-pressure correction (Dalcanton & Stilp 2010)
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A “Simple” Approach
•Gerssen, Shapiro Griffen, Noordermeer, et al.- 2D Kinematics (N long-slit positions/IFU)
- Rotation curve (EA) gives one axial ratio
- σmaj, σmin difference gives the other
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σ LO
S
θ (deg)
Ger
ssen
& S
hapi
ro G
riffe
n (2
012)
σ2LOS = (σ2R sin2θ + σ2θ cos2θ) sin2i + σ2z cos2i
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Observational Data
• Sample size: 40 Sa-Sd galaxies• Integral-field Spectroscopy of all
(WIYN,CAHA)• Optical NIR/Imaging of all
(KPNO 2.1m, SDSS, 2MASS)• Mid-IR imaging of all
(Spitzer)• Far-IR imaging of 10
(Herschel)• 1- & 3-mm Radio Synthesis of 5
(IRAM, CARMA)• 21-cm Radio Synthesis of all
(Westerbork, VLA, GMRT)
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UGC 4368
DiskMass Survey“Phase-B” Sample
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Observational Data
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• Sample size: 30 Sa-Sd galaxies• Integral-field Spectroscopy of
all (WIYN,CAHA)• Optical NIR/Imaging of all
(KPNO 2.1m, SDSS, 2MASS)• Mid-IR imaging of all
(Spitzer; 24µm→ICO→ΣH2)• Far-IR imaging of 10
(Herschel)• 1- & 3-mm Radio Synthesis of 5
(IRAM, CARMA)• 21-cm Radio Synthesis of all
(Westerbork, VLA, GMRT)
DiskMass Survey “Phase-B” Sample
UGC 4368
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Dynamics of Disk Galaxies 24 Oct 2013, 서울
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A Stepwise Approach
• Disk-plane geometry- Circular rotation + TF
• Azimuthally average kinematics- Impose axial symmetry
• EA+AD leads to SVE
Thursday, October 24, 2013
Dynamics of Disk Galaxies 24 Oct 2013, 서울
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UGC 4368 • Disk-plane geometry- Circular rotation + TF
• Azimuthally average kinematics- Impose axial symmetry
• EA+AD leads to SVE
A Stepwise Approach
Thursday, October 24, 2013
Dynamics of Disk Galaxies 24 Oct 2013, 서울
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UGC 4368 • Disk-plane geometry- Circular rotation + TF
• Azimuthally average kinematics- Impose axial symmetry
• EA+AD leads to SVE
A Stepwise Approach
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Dynamics of Disk Galaxies 24 Oct 2013, 서울
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A Holistic Model
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UGC 4368
Analytic➡ Parametrized forms
➡ V*, σR, α=σz/σR, σg, Σg➡ Epicycle Approximation
➡ β=σθ/σR➡ Asymmetric Drift
➡ Vc➡ Gas Pressure Effects
➡ Vg
Bayesian➡ Parameter values and errors
sampled from the Bayesian posterior
Thursday, October 24, 2013
Dynamics of Disk Galaxies 24 Oct 2013, 서울
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A Holistic Model
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UGC 4368
Analytic➡ Parametrized forms
➡ V*, σR, α=σz/σR, σg, Σg➡ Epicycle Approximation
➡ β=σθ/σR➡ Asymmetric Drift
➡ Vc➡ Gas Pressure Effects
➡ Vg
Bayesian➡ Parameter values and errors
sampled from the Bayesian posterior
Thursday, October 24, 2013
Dynamics of Disk Galaxies 24 Oct 2013, 서울
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UGC 4368
Analytic➡ Parametrized forms
➡ V*, σR, α=σz/σR, σg, Σg➡ Epicycle Approximation
➡ β=σθ/σR➡ Asymmetric Drift
➡ Vc➡ Gas Pressure Effects
➡ Vg
Bayesian➡ Parameter values and errors
sampled from the Bayesian posterior
A Holistic Model
δAD= Vg2-V✴2
σ✴2
δGP= Vc2-Vg2
σg2
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Tests against an N-body modelwith Elena D’Onghia & Carlos Vera-Ciro
A Test of Accuracy
Thursday, October 24, 2013
Dynamics of Disk Galaxies 24 Oct 2013, 서울
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Tests against an N-body modelwith Elena D’Onghia & Carlos Vera-Ciro
A Test of Accuracy
Thursday, October 24, 2013
Dynamics of Disk Galaxies 24 Oct 2013, 서울
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A Test of AccuracyTests against an N-body model
with Elena D’Onghia & Carlos Vera-Ciro
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Dynamics of Disk Galaxies 24 Oct 2013, 서울
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A Test of Accuracy
Bulge Effects
σ Rσ θ
σ zσ z
/σR
σ θ/σ
R Particle Data
Fit
Tests against an N-body modelwith Elena D’Onghia & Carlos Vera-Ciro
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Dynamics of Disk Galaxies 24 Oct 2013, 서울
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SVE vs. Hubble Type
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From RC3: Unbarred (S)
Barred (SB)
Weakly barred (SA)
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SVE vs. Hubble Type
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From RC3: Unbarred (S)
Barred (SB)
Weakly barred (SA)
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Dynamics of Disk Galaxies 24 Oct 2013, 서울
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SVE vs. Hubble Type
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From RC3: Unbarred (S)
Barred (SB)
Weakly barred (SA)
Thursday, October 24, 2013
Dynamics of Disk Galaxies 24 Oct 2013, 서울
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SVE vs. Hubble Type
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From RC3: Unbarred (S)
Barred (SB)
Weakly barred (SA)
Thursday, October 24, 2013
Dynamics of Disk Galaxies 24 Oct 2013, 서울
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SVE vs. Hubble Type
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From RC3: Unbarred (S)
Barred (SB)
Weakly barred (SA)
Thursday, October 24, 2013
Dynamics of Disk Galaxies 24 Oct 2013, 서울
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SVE vs. Hubble Type
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From RC3: Unbarred (S)
Barred (SB)
Weakly barred (SA)
Thursday, October 24, 2013
Dynamics of Disk Galaxies 24 Oct 2013, 서울
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SVE vs. Hubble Type
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From RC3: Unbarred (S)
Barred (SB)
Weakly barred (SA)
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Dynamics of Disk Galaxies 24 Oct 2013, 서울
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• Single component fluid disk
• Correction for a collisionless fluid
• Disk thickness corrections
• Two-component disk solution
The Stability Criterion
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(Too
mre
196
4)(R
omeo
&
Wie
gert
2011
)
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Dynamics of Disk Galaxies 24 Oct 2013, 서울
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The Stability Criterion
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The marginalized two-component stability at 1.5 scale lengths is QRW = 2.0 ± 0.9.
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Dynamics of Disk Galaxies 24 Oct 2013, 서울
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Star-Formation Law(s)
• Trends with SFR qualitatively consistent with theory
- ΣSFR anti-correlated with QRW (Li et al. 2006)
- SFE proportional to √Σ✴ (Ostriker et al. 2010)
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Shi+2011
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Dynamics of Disk Galaxies 24 Oct 2013, 서울
ConclusionsWe have developed a holistic, Bayesian approach to modeling the SVE in the disks using our two-dimensional data.- The approach fairs very well when tested against an
“observed” N-body simulation.
- We find results consistent with previous measurements, but find that the trend of α=σz/σR with Hubble type is not trivial.
- We find the marginalized two-component stability is QRW = 2.0 ± 0.9 at 1.5 scale lengths.
- We find disks with larger star-formation activity have lower QRW and higher Σ✴, consistent with theoretical predictions.
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감사합니다
Thursday, October 24, 2013