Transcript Document

The First Cosmic Explosions
Daniel Whalen
McWilliams Fellow
Carnegie Mellon University
Chris Fryer, Lucy Frey
LANL
Candace Joggerst
UCSC/LANL
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~ 200 pc
Cosmological
Halo z ~ 20
Transformation of the Halo
Whalen, Abel & Norman 2004, ApJ, 610, 14
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Chemical Mixing Prior to Breakout
Core Collapse SN
PISN
Joggerst, Whalen, et al 2010, ApJ, 709, 11
Joggerst & Whalen 2010, ApJ in prep
Primordial SNe in Relic H II Regions
Whalen, Van Veelen, O’Shea & Norman ApJ 2008, 682,49
Reverse Shock
Collision with the Shell
Primordial SNe in Neutral Halos
Late Radiative Phase
Fallback
Conclusions I
• elemental yields of primordial SNe depend on both explosive
nucleosynthesis and mixing and fallback within the star
• metals mix with primordial gas on 3 characteristic spatial
scales in primordial SNe (inside the star, 10 - 15 pc and 100 200 pc)
• Salpeter-type IMF averages of 15 - 40 solar mass Pop III
core-collapse SNe are the best fit to EMP star abundances
thus far, although considerable work remains
• metal and dust cooling in Pop III SNe remnants may lead to
prompt second star formation
LANL Pop III Supernova Light Curve Effort
Whalen, Fryer & Frey, ApJ 2010a,b, in prep
• LANL ASC code RAGE (Radiation Adaptive Grid Eulerian)
• 1D RTP AMR radiation hydrodynamics with grey/multigroup
FLD and Implicit Monte Carlo transport
• 2T models (radiation and matter not assumed to be at the same
temperature)
• PISN, core-collapse, and hypernova models
• post process rad hydro profiles to obtain spectra and light curves
Post Processing Includes Detailed LANL Opacities
but the atomic levels are
assumed to be in equilibrium,
a clear approximation
PISN Shock Breakout
• X-rays (< 1 keV)
• transient (a few
hours in the local
frame)
Spectra at
Breakout
The spectra evolve
rapidly as the front
cools
Long-Term Light Curve Evolution
Late Time Spectra
spectral features after
breakout may enable us
to distinguish between
PISN and CC SNe
larger parameter study
with well-resolved
photospheres is now in
progress
Roadmap Ahead
• current models are grey FLD; next step is
multigroup FLD and then multigroup IMC
• advance from 1D RTP AMR calculations
to 2D cartesian AMR grids
• incorporate mixing from 2D models to
simulate core-collapse SNe (15 - 40 solar
mass stars, hypernovae)
• implement non-equilibrium opacities
• investigate progenitor environments on
LC and spectra (LBV brightening?)
• explore asymmetric explosion mechanisms
• evolve toward 2D AMR IMC rad hydro
with thousands of frequency bins -- eliminate
post processing
Conclusions II
• PISN will be visible to JWST out to z ~ 10 - 15; strong lensing may
enable their detection out to z ~ 20 (Holz, Whalen & Fryer 2010
ApJ in prep)
• dedicated ground-based followup with 30-meter class telescopes
for primordial SNe spectroscopy
• discrimination between Pop III PISN and Pop III CC SNe will be
challenging but offers the first direct constraints on the Pop III IMF
• complementary detection of Pop III PISN remnants by the SZ effect
may be possible (Whalen, Bhattacharya & Holz 2010, ApJ in prep)