The Dynamical Ejection of High Velocity Stars from Dense Stellar Regions

The Dynamical Ejection of High Velocity Stars from Dense Stellar Regions

The dynamical ejection of high velocity stars from dense stellar regions Alessia Gualandris Astronomical Institute & Section Computer Science University of Amsterdam Runaway stars D efinition: massive stars of spectral type O-B peculiar velocities exceeding 30 km/s often away from known clusters or associations Interpretation: born in stellar clusters or associations and later ejected with high velocity Statistics: 40% O stars and 10% of B stars are runaways 10% of OB runaways are binaries Runaways: two competing scenarios 1. The binary supernova scenario Primary component of a massive binary explodes as supernova system is unbound: kick velocity to the secondary star of the order of orbital velocity system remains bound: HMXRB This scenario alone fails to explain the total fraction of single runaway stars Runaways: two competing scenarios 2. The dynamical ejection scenario Stellar dynamical encounters in dense clusters: binary-single star encounters binary-binary encounters OB stars likely participate in dynamical encounters Dynamical ejection occurs in young and dense star clusters, where a large number of single and binary stars are concentrated in a small volume. i m Orionis, AE Aurigae, Columbae ] c p [ ⊙ D Hoogerwerf et al. 2001 AE Aurigae m Columbae O9.5 V O9.5 V/ B0V M = 16-22 M⊙ M = 16-22 M⊙ V = 115 km/s V = 103 km/s no evidence of binary evolution same kinematical age ( t = 2.5 Myr) same parent stellar cluster i Orionis O-type spectroscopic binary Porb = 29 days, a = 0.741 AU High eccentricity e = 0.76 Mass ratio q = 0.5 Spectral Mass Radius Age Orion nebula type (M⊙) (R⊙) (Myr) P O9 III 38.9 ± 9.7 15.8 ± 3.2 3.5 S B1 III-IV 18.9 ± 4.7 9.6 ± 1.9 7 ι Ori Different ages ⇩ the system is not co-evolved A dynamical encounter involving the 4 stars occurred 2.5 Myr ago in the Trapezium cluster Opposite velocities of AE Aur and m Col ¯ binary-binary encounter Age difference i Ori P and S ¯ exchange-ionization encounter { i Ori P + AE Aur} + { i Ori S + m Col} ⇓ { i Ori P + i Ori S} + AE Aur + m Col Ejection of runaway stars: numerical simulations Direct N-body code to simulate dynamical encounters between 2 binaries: scatter in the STARLAB package (McMillan, Hut, Makino, Portegies Zwart) http://www.manybody.org Choice of initial conditions (masses, velocities, radii, orbital separations, eccentricities, orientation and inclination, impact parameter) Ejection of runaway stars: numerical simulations Preservation Ejection of runaway stars: numerical simulations Exchange Ejection of runaway stars: numerical simulations Ionization Ejection of runaway stars: numerical simulations Triple A model for i Orionis, AE Aurigae, m Columbae: stellar and binary evolution calculations {i Ori S, m Col} t = 7 Myr {i Ori P, AE Aur} t = 3.5 Myr 22 M 18 M 44 M 18 M ⊙ ⊙ ⊙ ⊙ Ionization + Exchange interaction 2.5 Myr ago {i Ori P + AE Aur} + {i Ori S + m Col} 42 M 18 M 21.5 M 18 M ⊙ ⊙ ⊙ ⊙ ⇓ {i Ori P + i Ori S} + AE Aur + m Col 42 M 21.5 M 18 M 18 M ⊙ ⊙ ⊙ ⊙ Gualandris, Portegies Zwart, Eggleton 2004 Ejection of runaway stars: the velocity distributions Observed ejection velocity V= 18 km/s Observed ejection velocity V= 115 km/s Observed ejection velocity V= 103 km/s Gualandris, Portegies Zwart, Eggleton 2004 Ejection of runaway stars: the semi-major axis distribution Observed semi-major axis a=0.74 AU <a> = 0.54 0.01 AU apeak= 0.72 AU Gualandris, Portegies Zwart, Eggleton 2004 The runaway stars i Ori, AE Aur, m Col were ejected from the Trapezium cluster by a binary-binary encounter. Hyper-velocity stars: the first discovery HVS Vrad = 850 km/s Vspace ~ 1000 km/s m = 3 M⊙ B9 MS d = 71 kpc tMS = 350 Myr tD = 80 Myr Brown et al. (2005) Hyper-velocity stars: the ejection mechanism SN explosion Dynamical encounter with ªnormalº stars Vmax = 300-400 km/s ⇒ need a more massive target: a SMBH 6 1/2 1/2 Vej ~ 3000 km/s (M/10 M⊙) (1mpc/r) The Galactic Centre Sagittarius A The hyper-velocity star: the trajectory in the Galaxy Vr = 850 km/s m ~ 2 mas/yr Vt = 675 km/s V ~ 1085 km/s Hyper-velocity stars: the theoretical prediction Dynamical encounters with the SMBH stellar binary + SMBH tidal breakup Hyper-velocity stars: numerical simulations 6 Mbh = 3.5x10 M⊙ m = 3 M⊙ 0.05 AU < a < 1 AU Vrel = 100 km/s Hyper-velocity stars: cross-sections Hyper-velocity stars: velocity distribution Hyper-velocity stars: the theoretical prediction Dynamical encounters with the SMBH BBH + single star flyby Hyper-velocity stars: numerical simulations 6 Msmbh = 3.5x10 M⊙ 3 Mimbh = 3.0x10 M⊙ m = 3 M⊙ 2 AU < a < 1000 AU Vrel = 100 km/s Hyper-velocity stars: velocity distribution The velocity of the hypervelocity star is consistent with a dynamical encounter with the SMBH in the Galactic Centre. We predict a proper motion of about 2 mas/yr..

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