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Radiation-SPH Simulations on the Radiative Feedback of POPIII Stars. Hajime Susa (Rikkyo,JPN) Collaborator: Masayuki Umemura (Tsukuba). Radiative Feedback. Processes photoionization photoevaporation enhance H2 formation H2 dissociation by Lyman-Werner (LW) Band photons H2 destruction
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Radiation-SPH Simulations on the Radiative Feedback of POPIII Stars Hajime Susa (Rikkyo,JPN) Collaborator: Masayuki Umemura (Tsukuba) EANAM2006(大田)
Radiative Feedback • Processes • photoionization • photoevaporation • enhance H2 formation • H2 dissociation by Lyman-Werner (LW) Band photons • H2 destruction • H2+, H- destruction • Outcome • self-regulation of SF in the early universe • Source of reionization Abel et al. 2006 EANAM2006(大田)
Three phases of Radiative feedbackfrom dark to luminous ages • Phase I: local feedback from single POPIII(ionization+dissociation) e.g. Omukai & Nishi 1999; Glover & Brand 2001;Susa & Umemura 2006; Ahn & Shapiro 2006; Yoshida et al.(2006) • Phase II: diffuse LW background (built up by many stars) e.g. Haiman et al. 1997; Ciardi et al. 2000; Oh & Haiman 2003 ; Mesinger ,Bryan, Haiman 2006 • PhaseIII: diffuse ionizing photon background →Reionization of the univ. e.g. Barkana & Loeb 2000; Kitayama et al. 2000,2001; Susa & Umemrua 2004ab EANAM2006(大田)
Local H2 photodissociation feedback in uniform gas cloud Uniform low mass host clouds are totally Photodissociated by single POPIII star. Omukai & Nishi 1999 EANAM2006(大田)
H2 photodissociation feedback on clumpy cloud Glover & Brand 2001 Dense clouds are able to survive the photodissociation feedback by another nearby star. • Dynamically collapsing cloud ? • Photoionization? Radiation hydrodynamics simulations EANAM2006(大田)
Numerical Methods H. Susa, PASJ 58, 445 (2006) • Tree • SPH • RT of Ionizing photons by Ray Tracing • RT of Lyman-Werner photons by Ray Tracing ( Self-Shielding function) • Implicit solver for reactions and energy equation • H2 (no He) • Everything parallelized utilizing MPI EANAM2006(大田)
FIRST 240 nodes 480 CPU + 240 Blade-GRAPE 480 Xeon : 2.9 Tflops Blade-GRAPE:8.7 Tflops Memory:512GB Now available EANAM2006(大田)
Uniform dense clump Run-away collapsing Core Turn on the nearby star Setup SPH particles Uniformly Distributed EANAM2006(大田)
Parameters Property of the Source Star c.f. size of the first star forming halos are several ×10pc EANAM2006(大田)
LW feedback (without ionization) Susa 2006 in prep. EANAM2006(大田)
Failed Collapse ( H2 fraction ) LW photons sweep the dense core and prevent the cloud from collapsing. Core bounce EANAM2006(大田)
Survived prestellar core (H2 fraction) H2 is self-shielded Collapsed core EANAM2006(大田)
Time evolution of Central density collapse bounce Turn-on EANAM2006(大田)
H2 reformation Evolution of central density & tempetarute Three different initial Tof collapsing cloud collapse Bounce EANAM2006(大田)
Analytic cooling condition Once the collapsing core satisfy above condition, the collapse cannot be stopped. EANAM2006(大田)
D=20pc RUN AWAY REGION Bounce collapse Susa, in preparation (2006) EANAM2006(大田)
Comparison with the condition tdis > tff ( Glover & Brand 2001) Importance of dynamical effect (H2 recovery) EANAM2006(大田)
LW + Ionizing photons Susa & Umemura (2006) Susa & Umumura in prep. EANAM2006(大田)
Photoevaporation (less dense core) • All of the gas is • photoevaorated and • the dense clump disappers • The I-front propagates as • R-type. EANAM2006(大田)
Self-shielding condition for Static Core EANAM2006(大田)
Disrupted Core by shock M-type IF induce shock, that destroy the core. EANAM2006(大田)
H2 shell formation&Enhancement of H2 in the core Bounce EANAM2006(大田)
Competition of various effects • H2 dissociation • Photoevaporation (thermal pressure / shock) • Self-shielding (LW / ionizing photons) • Enhanced H2 formation in the core (→Ahn) • H2 shell formation EANAM2006(大田)
Summary of Runs (non-D plane) LW only LW + ION Effects of photoionization alleviates the negative feedback of photodissociation EANAM2006(大田)