Koushik Sen
Nicolaus Copernicus University Torun
Astrophysics seminar of the PAU Astrophysics Committee, Krakow
April 5, 2023
Evolution of short-period massive binary stars in the Magellanic Clouds
Collaborators: Norbert Langer, Abel Schootemeijer, Tomer Shenar, Laurent Mahy, Goetz Grafener, Chen Wang, Hughes Sana, Athira Menon, Selma de Mink
The Magellanic Clouds
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Credit: J. C. Muñoz/ESO
Large Magellanic Cloud (LMC)
Small Magellanic Cloud (SMC)
Massive stars
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O type star
Early B type stars
Radiative envelope
Convective core
Multiplicity of massive stars
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Fraction of interacting binaries
Sana+2012
Moe+2017
Mass M1 (M )
What is the need?
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Kruckow+2018
Close binary evolution
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M1 = 20 M M2 = 12 M
Porb = 3 d
Images credit: Philip D. Hall - CC BY-SA 4.0
M1 = 20 M M2 = 12 M
M1 = 20 M M2 = 12 M
M1 = 16 M M2 = 16 M
M1 = 8 M M2 = 24 M
a
Algol binaries and the Algol paradox
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Credit: SpaceEngine
M1 = 0.7 M , R1 = 3.48 R
M2 = 3.2 M , R2 = 2.73 R Porb = 2.87 days
Wind-fed black hole high-mass X-ray binaries
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collapse
Stripped star
MBH = 21.2 M
MO = 40.6 M
Credit: NASA
Kruckow+2018
Binary evolution modelling
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Detailed binary evolution with MESA (Paxton+2011,13,15,18,19)
PART I: MASSIVE ALGOL BINARIES
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Algol binaries: Context
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Md = 8.7 M
Ma = 16.3 M
9.0
10.0
11.0
12.0
t [Myr]
Observations
Models
No comprehensive binary population synthesis study of massive Algol binaries
Sen+2022A&A...659A..98S
long mass transfer phase
Algol binaries: Method
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Mass transfer efficiency
Ꞷcrit = (GM/R3)0.5
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M, R, I, Ꞷi
ΔM?
ΔJ = (GMR)0.5 ΔM
ΔM/M = 𝒇 (rg2, Ꞷi/Ꞷcrit)
IꞶ
ΔM/M = 0.00-0.10 (Packet+1981)
I = rg2 MR2
In binaries, there are tidal forces!
Algol binaries: Results
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Sen+2022A&A...659A..98S
Algol binaries: Takeaways from Part I
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PART II: WIND-FED BLACK HOLE HIGH-MASS X-RAY BINARIES (HMXBs)
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BH high-mass X-ray binaries: Context
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Stripped star
collapse
Kruckow+2018
BH high-mass X-ray binaries: Method
A. Formation of an accretion disk
B. X-Ray flux above detection threshold
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Formation of an accretion disk
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RO
Racc
Matter is accreted from the stellar wind (vwind) of the O star
Accretion radius of the compact object (Davidson+1973)
Specific angular momentum (j) of the accreted matter (Shapiro+1976)
figure not to scale
a
Formation of an accretion disk
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Equating centrifugal force to gravitational force, Rdisk = j2 / GMBH
Formation of an accretion disk
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Equating centrifugal force to gravitational force, Rdisk = j2 / GMBH
[ 𝛾± = ⅙, 1, 3/2 ]
X-Ray luminosity (LX)
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-- mass accretion rate (Davidson & Ostriker 1973)
-- X-ray luminosity (Frank+2002, El Mellah 2017)
-- The Lx > 1035 erg s-1 to be observable (Wood+1984, Bradt+1991)
BH high-mass X-ray binaries: Results
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Black hole spin
Sen+2021A&A...652A.138S
For Cygnus X-1
MO star = 40.6 M , MBH = 21.2 M
Orbital period = 5.9 days
Non-rotating BH: Rdisk / RISCO = 0.20
Maximally rotating: Rdisk / RISCO = 1.23
BH high-mass X-ray binaries: Takeaways
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Outlook
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THANK YOU
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