the star formation history of the local universe a/prof. andrew hopkins (aao) prof. joss...
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The star formation history of the local
universe
A/Prof. Andrew Hopkins (AAO)Prof. Joss Bland-Hawthorn (USyd.)
& the GAMA Collaboration
Madusha L.P. GunawardhanaDurham University
DEX X workshop - Durham - 09/01/2014
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Evolution of star formation
UV[OII]Hα/Hβsub-mm, radio, FIR & others
Hopkins A.M., 2004, ApJ, 615, 209Hopkins A. M. & Beacom J., 2006, ApJ, 651, 142
★ There are various probes of star formation - Nebula emission lines: [OII], [OIII], Hα, Hβ- Photometric measures: UV, mid-IR, far-IR, radio ★ Each indicator has its advantages and drawbacksUV is a direct tracer of young (>5Mʘ) stars but dust obscured systems are missed in UV samples, making FIR, a tracer of dusty systems, a valuable complementary to UV.
★ There are also survey selection and calibration biases- narrowband vs broadband surveys- flux/magnitude limits- surveys area (cosmic variance)- dust/AGN corrections
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★ Covers a wide range in SFR (0.001<SFR(Mʘ yr-1)<100) AND in stellar mass (107<M/Mʘ<1012) AND extends up to z ≈ 0.35
★ The properties of lowest SFR galaxies are investigated in Brough et al. (2011)
Evolution of star formation in Hα
★ Balmer decrement is used to estimate obscuration corrections
SFR vs redshift
Luminosity-dependent obscuration
★ Aperture corrections are based on fibre and Petrosian r-band magnitudes
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Hα Luminosity Functions
Gunawardhana et al., 2013, MNRAS, 433, 2764
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Schechter vs Saunders functional fits
★ Saunders et al. (1990) function is better suited at fitting the bright-end
of the Hα LF
★ Salim & Lee (2012) also find that the underlying SFR distribution is
better described by a Saunders function than a Schechter function.
Gunawardhana et al., 2013, MNRAS, 433, 2764
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Cosmic star formation history
UV[OII]Hα/Hβsub-mm, radio, FIR & others
Hopkins A.M., 2004, ApJ, 615, 209Hopkins A. M. & Beacom J., 2006, ApJ, 651, 142
★ Jurek et al., (2013, MNRAS) find that the bright end of the WiggleZ survey
UV LF is not well described by a Schechter function due to an excess of
UV luminous galaxies.
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Local Star Formation History
Gunawardhana et al., 2013, MNRAS, 433, 2764
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Bivariate Hα/Mr Distribution
★ For GAMA, the r-band apparent magnitude limit combined with
requirement for Hα detection leads to an incompleteness due to missing
bright Hα sources with faint r-band magnitudes
100 Mʘyr-1
10 Mʘyr-1
1 Mʘyr-1
★ The lowest-z (z<0.1) sample is the most complete with SFRs reaching as
low as 0.001 Mʘ yr-1
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Bivariate LHα/Mr Luminosity functions
0.01 Mʘ/yr
0.1 Mʘ/yr
1 Mʘ/yr
100 Mʘ/yr
Gunawardhana et al., (MNRAS, submitted)
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Bivariate functional fit vs Copula approach
★ Bivariate functional fit: Ψ(2)(LHα, Mr) = Φ Schechter(Mr) x Φ (LHα, Mr)
★ Bivariate distribution constructed using a Gaussian Copula following the method of
Takeuchi (2010, MNRAS, 406, 1830)
ρ = 0.9
Gunawardhana et al., (MNRAS, submitted)
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SFR density plot
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SFR density plot
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Conclusions★ Star formation in galaxies follows a Saunders (or two-power law) distribution, NOT a Schechter function.
★ GAMA and SDSS Hα luminosity functions confirms this for the first time, making Hα finally consistent with other wavelength estimators of SFR such as IR and radio.
★ Bivariate selection influence ANY star forming sample drawn from a magnitude limited survey. As a consequence the resulting SFRDs are underestimated.
★ One way to correct this is to model the bivariate distribution
★ GAMA website (http://www.gama-survey.org/)
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Aperture corrections
★ Aperture corrections are based on fibre and petrosian r-band magnitudes
Aperture correction vs redshift