Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:0806.2235.

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Evolution of low-mass binaries with black- hole components L. Yungelson et al. Ref: arXiv:0806.2235

Transcript of Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:0806.2235.

Page 1: Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:0806.2235.

Evolution of low-mass binaries with black-hole components

L. Yungelson et al.Ref: arXiv:0806.2235

Page 2: Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:0806.2235.

1. Model- Formation of black holes with low-mass companions

• Population of zero-age LMBHB code: SEBA 250000 initial binaries M10>25Msun

a 50% binarity (2/3 of stars in binaries) for the CE phase: αCE×λ=2

Page 3: Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:0806.2235.

1. Model- Angular momentum loss

• Low mass components KV/MV spectral type AML via MSW:

AML via GWR:

Eqs.(1)+(2)- a “standard” model

)1(12

102

1ln2

1

42

3/1

3/2

3/10228

fM

RM

GPk

dt

Jd t

1~1.0~2 fk

Page 4: Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:0806.2235.

1. Model - Population of unevolved LMBHB

• Within Hubble time(13.5 Gyr) 49000 BH+MS Porb < 2 day M20<1.6Msun

Page 5: Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:0806.2235.

MBH=12Msun

MBH=4Msun

In standard model: overflow < 15 hr → shorter period

Page 6: Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:0806.2235.

2. Evolution of LMBHB

• In the figures below, q=M2/M1≥0.02• q=M2/M1<0.02: - circularization radius of accretion stream>outer

radius of accretion disc - how mass transfer occurs ? - Porb ≤ 2 hr mass-transfer rate < 10-10 Msun yr-1

• In “standard” model 75% q<0.02

Page 7: Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:0806.2235.

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

Page 8: Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:0806.2235.

2. Evolution of LMBHB - Reduced angular momentum loss?

Page 9: Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:0806.2235.

2. Evolution of LMBHB - Observational parameters of short-period LMBHB

Page 10: Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:0806.2235.

a. Effective temperatures• Essential information of donor: spectral type• Emission of the cool star is contaminated by

radiation from disc and hot spot

Page 11: Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:0806.2235.

b. Masses of donors

Page 12: Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:0806.2235.

c. Mass-transfer rate

• Non-stationary quiescent accretion disc:

• According to DIM, disc is in cold thermal equilibrium if :

Page 13: Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:0806.2235.

48.0 tcirctin frfr

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

Page 14: Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:0806.2235.

3. Cold, stable system

Page 15: Evolution of low-mass binaries with black-hole components L. Yungelson et al. Ref: arXiv:0806.2235.

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 ,Rin •

2CE