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This study explores the radiative feedback mechanisms and formation pathways of H2 in high redshift cosmological mini halos using the ZEUS-MP Reactive Flow Radiation Hydrodynamics Code. The results show the evolution of a single halo and its core density, velocity, and fate in the absence of radiation. The study also examines the impact of radiation on star formation and the key role of multifrequency transfer and chemistry in halo dynamics.
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Radiative Feedback by the First Stars Dan Whalen, T-2, LANL Whalen et al 2008, ApJ, 679, 925 Hueckstadt & Whalen, ApJ, in prep
Our Collaboration Daniel Whalen, T-2, LANL Rob Hueckstaedt, X-2, LANL Brian O’Shea MSU Joseph Smidt UC Irvine Alex Heger U Minn Michael Norman, UC San Diego
~ 200 pc Cosmological Halo z ~ 20
H2 Formation Pathways in High Redshift Cosmological Minihalos
The Universe at Redshift 20 128 kpc comoving
ZEUS-MP Reactive Flow Radiation Hydrodynamics Code • massively-parallel (MPI) Eulerian hydrocode with 1-, 2-, • or 3D cartesian, cylindrical, or spherical meshes • 9-species primordial H/He gas network coupled to photon • conserving multifrequency UV transfer • adaptive time step hierarchy enforces respective • Courant, heating, and chemistry times without holding • the entire algorithm hostage to the shortest time scale • Poisson solver for gas self-gravity • a separate array serves as a proxy for the dark matter • potential, which remains frozen in the course of these • calculations
40 energy bins < 13.6 eV, 80 bins from 13.6 eV to 90 eV • self-shielding functions of DB 96 corrected for thermal • Doppler broadening are used to compute H2 photo- • dissociation
Parameter Space of Surveyed Halos • We sample consecutive evolutionary stages of a single • 1.35 x 105 solar mass halo rather than the entire cluster • at a single redshift • Since halos in the cluster tend to be coeval, exposing • just one at several central densities spans the range of • feedback better than a few at roughly the same density • We chose this halo mass because it is the smallest in • which we expect star formation, so feedback would be • less prominent than in a more massive halo
Spherically-Averaged Enzo AMR Code Halo Radial Density and Velocity Profiles (O’Shea & Norman 2007b) z = 23.9, 17.7, 15.6 and 15.0
I-Front Structure monoenergetic: 20 - 30 mfp e, T 105 K blackbody: e, T T-Front quasar: e, T secondary ionizations by photoelectrons
Four Fates of Satellite Halos • complete core disruption • undisturbed cores • accelerated collapse • core drainage/partial disruption
059_500pc 40 solar mass star
Four Outcomes: • halos with nc < 2 - 3 cm-3 are completely destroyed anywhere in the cluster • halos with nc > 1000 cm-3 are insulated from radiation--collapse is unaffected • star formation in halos of intermediate density can be accelerated or delayed • depending on how the shock and shadow squeeze the core
Preliminary Conclusions • due to coeval nature of halos within the cluster, feedback • tends to be positive or neutral • halos with nc > 100 cm-3 will survive photoevaporation • and host star formation (accelerated in many instances) • feedback sign is better parameterized by central halo • density than halo mass • radiation drives chemistry that is key to the hydrodynamics • of the halo -- multifrequency transfer is a must • these results are mostly independent of the spectrum of • the illuminating star--more LW photons don’t make much • difference