de Recherche Astronomique de Lyon, France 2 Instituto de Astronomia, Ensenada, UNAM, Mexico 2006 july 10th
Eskridge et al 2000 AJ 119, 536
Jogee et al. 2004 ApJ 615, L105
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Sheth et al. 2003 ApJ 592, L13
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Why studying barred galaxies?
Bars are the main drivers of evolution of disc galaxies between major merger events A stellar bar is able to:
Bring gas from the disc to the central region Enhance star formation Reshape the stellar disc Homogenize distribution of elements
Strong constraints on dark matter distribution
Slowdown rate of bar rotation is linked to halo concentration (dynamical friction ⇒ angular momentum bar → halo exchanges) z=0 bars slow of fast rotators ?
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Observation/simulation duality Observation of stellar bars Length
N-body simulations (Theory) Corotation radius
Relationship
Axis ratio (ellipticity)
Strength
1 ≤RCR/Rbar≤1.7 (obs) or 2.6 (sim) ~ correlation (trend)
Luminosity
Mass
M/L
Line-of-sight kinematics
3D kinematics
Dark matter
…
…
…
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Comparing simulations with observations Athanassoula & Misiriotis 2002 MNRAS 330, 35 Bar lengths
λ=1.4 (Kennicutt 1990) SFE = 0.1 creation of new stellar particles (remnants) SNII mechanical fraction of energy = 0.1
Maeder’s yields (1992) → metallicities cooling with solar abundances (Bohringer & Hensler 1989)
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Simulations parameters & calibration
5-6 105 stellar particles (initial pop.) → ~ 1.2 106 at the end 1-5 104 SPH particles Mg / M¹ ~ 0.1 – 0.3 initial disc scalelengths : 3.5 to 5.5 kpc initial disc scaleheights: 0.5 to 1 kpc Photometric calibration
SSP from Bruzual & Charlot (2000 release) Salpeter IMF 0.1 to 100 M~ Z of initial stellar pop = 0.004 initial age (4.4 to 10.4 Gyr) leads to z=0 at the end of the simulation
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10 kpc
16 kpc
Star formation rates Bar formation
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Measuring bar lengths… Ellipse-fitting methods: ---- Mass ---- B ---- K
max: used by e.g. Jogee et al. 2004 plateau: Michel-Dansac & Wozniak 2006 drop: used by e.g. Sheth et al. 2003
max
plateau
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Sheth et al. 2003 ApJ 592, L13
drop
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…and ellipticities.
max ellipticity
Mass density
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B
B + absorption
K
K + absorption
---- Mass ---- B ---- K
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Bar strength and ellipticity evolution
max ellipticity
---- Mass ---- B ---- K Combes & Sanders 1981 :
Qb
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Bar strength – ellipticity correlation Laurikainen et al. 2002 MNRAS 331, 880 2MASS galaxies
From MD&W 2006 simulations • Mass •B •K
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Resonances in barred galaxies
corotation radius (Rcr)
Ωb: pattern speed Ω: circular orbit frequency κ: radial epicyclic frequency
For each snapshot: • froze the potential • compute of orbits for several dynamical time ⇒ orbital frequencies (Ω,κ) κ ⇒ families of resonant particles ⇒ resonances location
Ωb 2006/07/10
Ω 15
Bar length and resonances evolution corotation ↔ ellipticity drop
---- Mass ---- B ---- K
UHR ↔ PA plateau
Radius (kpc)
ILR ≠ max ellipticity
Time (Gyr) 2006/07/10
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Fast or slow bars ? Aguerri et al. 2003 MNRAS 338, 465 Rautiainen et al. 2005 ApJ 631, L129 PA plateau
2006/07/10
ellipticity drop
Rcr = 1.4 Rbar
Rcr = Rbar
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Conclusions
Comparison observation/simulation :
Bar strength / ellipticity
need to calibrate simulations use of chemodynamical simulations
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