Evolution of Massive Stars - KU Leuven...Evolution of Massive Stars : Magetic Fields Norbert Langer...
Transcript of Evolution of Massive Stars - KU Leuven...Evolution of Massive Stars : Magetic Fields Norbert Langer...
Evolution of Massive Stars
Norbert Langer (Bonn University)
with
Matteo Cantiello (UCSB)
Chris Evans (Edinburgh)
Sung-Chul Yoon (Seoul)
Alex de Koter (Amsterdam)
Swetlana Hubrig (Potsdam)
Fabian Schneider (Bonn)
Luca Fossati (Bonn)
Alexander Heger (Melbourne)
Selma de Mink (Carnegie)
Hugues Sana (Amsterdam)
Rob Izzard (Bonn)
Ines Brott (Vienna)
Bruxelles, 2-12-13 – p.1/25
Evolution of Massive Stars : Magetic Fields
Norbert Langer (Bonn University)
with
Matteo Cantiello (UCSB)
Chris Evans (Edinburgh)
Sung-Chul Yoon (Seoul)
Alex de Koter (Amsterdam)
Swetlana Hubrig (Potsdam)
Fabian Schneider (Bonn)
Luca Fossati (Bonn)
Alexander Heger (Melbourne)
Selma de Mink (Carnegie)
Hugues Sana (Amsterdam)
Rob Izzard (Bonn)
Ines Brott (Vienna)
Bruxelles, 2-12-13 – p.1/25
Massive Star Evolution
Bruxelles, 2-12-13 – p.2/25
Three kinds of B-fields in OB stars
large scaledirectly observable, “dipoles”,spin-down
small scaleindirectly observable; “spots”
toroidalinternal, not directly observable,j-transport, mixing
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Toroidal fields: ubiquitous?
differential rotation → Spruit-Taylor dynamo?Spruit 2002, A&A, 381, 923
slowly rotating Solar coreEggenberger 2005, A&A, 440, L9
slowly rotating cores of red giantsMosser et al. 2012, A&A, 548, A10
slowly rotating WDs and NSsSuijs et al. 2008, A&A 481, L87
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Core spin-down in red giants
Mosser et al. 2012, A&A, 548, A10
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B-fields in “non-magnetic” stars
Suijs, NL, Poelarends, et al. 2008, A&A 481, L87Bruxelles, 2-12-13 – p.6/25
Low Mass Stars (< 1.5M⊙)
convective envelopes
rotation↑ ↔ B↑ ↔ age↓example: Sun
concerns 100% of starsexceptions: tidal binaries
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Low Mass Stars (< 1.5M⊙)
convective envelopes
rotation↑ ↔ B↑ ↔ age↓example: Sun
concerns 100% of starsexceptions: tidal binaries
αΩ-dynamoα ↓ or Ω ↓ → B↓
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Intermed. Mass Stars (< 10M⊙)
radiative envelopesrotation↓ ↔ B↑concerns ∼10% of stars Ap, Bp stars→ 90% are non-magnetic
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Intermed. Mass Stars (< 10M⊙)
radiative envelopesrotation↓ ↔ B↑concerns ∼10% of stars Ap, Bp stars→ 90% are non-magneticstable large scale fields (no dynamo)Braithwaite & Spruit 2004, Nature 431, 819
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Massive Stars (> 10M⊙)
convective envelopes
αΩ-fields → spots
in all stars
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Massive Stars (> 10M⊙)
convective envelopes
αΩ-fields → spots
in all stars
stable large scale fieldsin 10% stars
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Massive stars: convective envelops
Cantiello, NL, Brott et al. 2009, A&A 499, 279 Bruxelles, 2-12-13 – p.10/25
Massive stars: microturbulence
Cantiello et al. 2009 Bruxelles, 2-12-13 – p.11/25
Stochastic pulsations: KEPLER
Belkacem, Samadi, Goupil, et al. 2009, Science, 324, 1540 Bruxelles, 2-12-13 – p.12/25
Massive stars: magnetic spots
sub-surface αΩ-dynamo
buoyant rise of B-fieldsCantiello et al. 2009
localized, small scale: bright spots
Discrete Absorption Components→ ubiquitous in O stars!
no spin-down
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Massive stars: large scale fields
Grunhut, Wade et al. 2012, ASPC, 465, 42 Bruxelles, 2-12-13 – p.14/25
LMC early B stars
6.8
7
7.2
7.4
7.6
7.8
8
0 50 100 150 200 250 300 350
12 +
log
[N/H
]
v sini [km/s]
M ≤ 10 Msun10 < M ≤ 12 Msun
12 < M ≤ 15 Msun15 < M ≤ 20 Msun
M > 20 Msunbinary
1
10
100
1000
Num
ber
of s
imul
ated
sta
rs p
er b
in
Box 1(a)
(b)
Box 2 Box 4
Box 3
Box 5
Brott, Evans, Hunter, et al. 2011, A&A 530, A116Bruxelles, 2-12-13 – p.15/25
Box 2 - stars: magnetic?
10% of early B stars: very slowrotators, N-rich
similar population in the Galaxy:B-field detected in most of them!Morel, Hubrig & Briquet 2008, A&A, 481, 453
O-stars? –> ESO Tarantula Survey(PI: Chris Evans)
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The rotation rates: early B stars
Dufton, NL, Dunstall et al. 2013, A&A 550, A109Bruxelles, 2-12-13 – p.17/25
Origin of large scale fields
“fossil”: how? why 10%?
binary induced:binaries −→ 10%magnetic MS, WD: mostly singleMS WD NS: 10% magneticMS: N-enrichmentobs. examples (e.g., HD 148937;Plaskett’s star)
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Close binaries: O stars
eectivelysingle
envelopestrippingenvelopestripping
merge
accretion & spin up or CE
accretion & spin up or CE
~29%
~24%
~14%
~33%
Sana, de Mink, de Koter, NL, et al. , 2012, Science, 337, 444Bruxelles, 2-12-13 – p.19/25
Pre-MS merger
Korntreff, Kaczmarek & Pfalzner 2012, A&A 543, A126Bruxelles, 2-12-13 – p.20/25
HD 148937
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Dipoles from dynamical events?
binary merger: strong differential rotationimposed on dynamical time scale
Polars (=magnetic WDs in CVs) very tight:almost-mergerPotter & Tout 2010
ordinary neutron stars: dynamical collapsewith rotationDuncan & Thompson 1992
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Advanced evolution
Can stable large scale fields prevail?
intermediate mass stars:magnetic Herbig AeBe (10%) → Ap/Bp star(10%) → magnetic WD (10%)
massive stars:magnetic OB (10%) → magnetar (10% ?)
flux conservation: B-fields scale within uncertain-
ties
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Advanced evolution
Heger et al. 2000, ApJ 528, 368Bruxelles, 2-12-13 – p.24/25
Conclusions
torroidal fields ubiquitous in stars→ core spin-down
small scale fields: ubiquitous in low and highmass stars
strong large scale fields in ∼ 10% of: Herbigstars, intermdiate mass and massive mainsequence stars, WDs, NS (?)
binary merger → large-scale fields
rotating core collapse → NS fields (?)
survival of large scale fields: magnetic WDs& magnetars?
Bruxelles, 2-12-13 – p.25/25