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The Stellar Initial Mass Function at the Epoch of Reionization (i.e. z>6). Ranga Ram Chary Spitzer Science Center, US Planck Center rchary@caltech.edu. Talk Outline. The evidence from gamma-ray bursts The evidence from stellar mass density in z~6 galaxies
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The Stellar Initial Mass Function atthe Epoch of Reionization (i.e. z>6) Ranga Ram Chary Spitzer Science Center, US Planck Center rchary@caltech.edu Chary, HMSF Townsville, Australia Sept 2010
Talk Outline • The evidence from gamma-ray bursts • The evidence from stellar mass density in z~6 galaxies • Future possibilities to constrain the IMF at z>6 robustly • Halpha • Thermal radio emission Chary, HMSF Townsville, Australia Sept 2010
Tanvir et al. 2009, Nature Salvaterra et al. 2009 GRB 090423 at z=8.26 • Gamma-ray burst on 23 April 2009; highest spectroscopically confirmed astrophysical object known; 600 Myr after the Big Bang. • The detection of even this one burst at z~8 is a surprise ! • - Not expected based on our estimate of SF in z>6 galaxies • Upper limit to the U-band luminosity of the host is ~8.8109L. In contrast L* at z=7.4 is ~1.8 1010L. So, as at lower redshift, the host is a sub-L* galaxy. Chary, HMSF Townsville, Australia Sept 2010
WFC3 UDF (Bouwens et al) RC, Berger & Cowie 2007 • Are we missing star-forming galaxies in deep surveys e.g. UDF ? • - Is it because of dust obscuration ? • Producing GRBs more efficiently because of lower metallicity ? • Is the stellar Initial Mass Function more top-heavy ? (Chary 2008 ApJ) Chary, HMSF Townsville, Australia Sept 2010
Astronomical Archaeology @ z=6 Chary, HMSF Townsville, Australia Sept 2010
Deep Spitzer Observations of z~6-7 galaxies Robustly Constrain Stellar Mass Labbe et al. 2010 Observed • The stellar mass is the integral of the past star-formation history • Star-formation is what keep the Universe ionized; need 3 photons/baryon Chary, HMSF Townsville, Australia Sept 2010
Data/fits from Bouwens et al. 08 • We cannot detect all galaxies, only the bright ones • So need to make a correction for the faint end • Thankfully, faint galaxies are blue i.e. young and have low M/L stellar populations Chary, HMSF Townsville, Australia Sept 2010
Balancing the Ionizing Photon Budget: A Simple Low Mass Cut in the IMF is Insufficient So, a top-heavy IMF at z>6 seems necessary. And that is consistent with the GRB Rate as well Chary, HMSF Townsville, Australia Sept 2010
<1 Billion Yr Old Universe M-1.6 Present-day Universe M-2.35 Nature promotes obesity!More massive stars earlier in the Universe Chary, HMSF Townsville, Australia Sept 2010
Are Large Hα EW in z~5 galaxies a Clue ? Chary et al. ’05 H. Shim, RC et al. ‘10 • Hα inferred from Spitzer broadband observations • Hα excited by UV continuum shortward of Lyman limit • A hard UV continuum can arise from a top-heavy IMF Chary, HMSF Townsville, Australia Sept 2010
Getting clues from the radio E. Murphy et al. 2010 Chary, HMSF Townsville, Australia Sept 2010
Future High Frequency Radio Surveys N Non-thermal Radio Emission: • LνNT ∝ ν-αqsnr TopHeavy/Kroupa ~ 2.32 Thermal Radio Luminosity: • LνT ∝ Te0.45 ν-0.1Q(H0) TopHeavy/Kroupa~ 5.68 Ratio of TOTAL radio luminosity at 1.4 GHz: • L1.4 THK/L1.4K ~ 2.82 (comparable to x2 scatter in current Radio/IR relationship) Chary, HMSF Townsville, Australia Sept 2010 E. Murphy et al. 2010
Conclusions • The GRB rate density suggests more massive stars forming at z>4 • Stellar mass density measured in z~6 galaxies is a x2 below what is required to account for reionization • Need more ionizing photons per unit mass of stars Top-heavy IMF • Our best estimate is dN/dM~M-1.6+/-0.2 average for z>6 • Currently seeing evidence for unusually strong Hα • Future 30-90 GHz radio surveys will measure the free-free emission which is strongly correlated with incidence rate of ionizing photons Chary, HMSF Townsville, Australia Sept 2010