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Published byNelson Franklin Modified over 9 years ago
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Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:0806.2235
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1. Model - Formation of black holes with low-mass companions Population of zero-age LMBHB code: SEBA 250000 initial binaries M 10 >25M sun a 50% binarity (2/3 of stars in binaries) for the CE phase: α CE ×λ=2
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1. Model - Angular momentum loss Low mass components KV/MV spectral type AML via MSW: AML via GWR: Eqs.(1)+(2)- a “standard” model
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1. Model - Population of unevolved LMBHB Within Hubble time(13.5 Gyr) 49000 BH+MS P orb < 2 day M 20 <1.6M sun
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M BH =12M sun M BH =4Msun In standard model: overflow < 15 hr → shorter period
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2. Evolution of LMBHB In the figures below, q=M 2 /M 1 ≥0.02 q=M 2 /M 1 <0.02: - circularization radius of accretion stream>outer radius of accretion disc - how mass transfer occurs ? - P orb ≤ 2 hr mass-transfer rate < 10 -10 M sun yr -1 In “standard” model 75% q<0.02
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2. Evolution of LMBHB - Luminous persistent LMBHB? Irradiated discs are hot and stable if accre -tion rate exceeds No persistent LMBHB with Porb<4 hr are observed Stable model : 370 objects 2900 objects
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2. Evolution of LMBHB - Reduced angular momentum loss?
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2. Evolution of LMBHB - Observational parameters of short-period LMBHB
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a. Effective temperatures Essential information of donor: spectral type Emission of the cool star is contaminated by radiation from disc and hot spot
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b. Masses of donors
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c. Mass-transfer rate Non-stationary quiescent accretion disc: According to DIM, disc is in cold thermal equilibrium if :
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Menou et al. 1999 MNL MNL point out that if the truncation radii were slightly larger than estimated to fit observations of quiescent SXTs the discs would be globally stable
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3. Cold, stable system
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4. Conclusion Under various assumptions about the AML “standard” model unobserved persistent LMBHB pure GWR only transient systems Mass-transfer rate consistent with upper limits on Mdot Truncation of discs at radii close to Rcirc make disc cold and stable, in this case not relate to DIM “external factors” – enforced mass transfer,R in
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