FIELD BLUE STRAGGLERS AND RELATED MASS TRANSFER ISSUES George Preston, ESO, Santiago, 2012.
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Transcript of FIELD BLUE STRAGGLERS AND RELATED MASS TRANSFER ISSUES George Preston, ESO, Santiago, 2012.
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FIELD BLUE STRAGGLERS AND
RELATED MASS TRANSFER ISSUES
George Preston, ESO, Santiago, 2012
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TO BEGIN: A LITTLE HOMAGE
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We stand on the shoulders of giants who pioneered stellar structure and evolution in interacting binaries
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G. P. Kuiper
O. StruveZ. Kopal
R. Kippenhahn
B. Paczynski
F. Hoyle
H. Bondi
W. H. McCrea
L. Lucy
A. Sandage
mass transfer giants
of the 20th century
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G. P. Kuiper
O. StruveZ. Kopal
R. Kippenhahn
B. Paczynski
F. Hoyle
H. Bondi
W. H. McCrea
L. Lucy
A. Sandage
mentor
mentor
friend friend
friend
mass transfer giants
of the 20th century
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G. P. Kuiper
O. StruveZ. Kopal
R. Kippenhahn
B. Paczynski
F. Hoyle
H. Bondi
W. H. McCrea
DetachedSemi-detached
Contact
gas streamsBeta Lyrae
Bondi-Hoyle accretion
Hoyle-Bondi accretion
The BS mass-transfer
model
CasesAB&C
Roche lobe overflow
Mass transfer
The Algol paradox
& more L. Lucy
The mostcamera-shy
giant known
A. SandageHe discoveredBlue stragglers
mass transfer giants
of the 20th century
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While reading papers on the subject of my talk, I was surprised to discover
…
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how often first-class astronomers ignore each other’s work!
Thus,Sandage (AJ 1953) first identified blue stragglers unambiguosly in M3
McCrea invented an explanation for Sandage’s blue stragglers 11 years later (MNRAS 1964) with no reference to Sandage.
Böhm-Vitense (ApJ 1980) confirmed operation of McCrea’s process 16 years later in the ζ Capricorni system with no reference to eitherSandage or McCrea.
McClure (ApJ 1984) brilliantly generalized Böhm-Vitense’s result 4 years later with no reference to Sandage or McCrea or Böhm-Vitense.
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how often first-class astronomers ignore each other’s work!
Thus,Sandage (AJ 1953) first identified blue stragglers unambiguosly in M3
McCrea invented an explanation for Sandage’s blue stragglers 11 years later (MNRAS 1964) with no reference to Sandage.
Böhm-Vitense (ApJ 1980) confirmed operation of McCrea’s process 16 years later in the ζ Capricorni system with no reference to Sandage or McCrea.
McClure (ApJ 1984) brilliantly generalized Böhm-Vitense’s result 4 years later with no reference to Sandage or McCrea or Böhm-Vitense.
Three decades of ignoring!
WTF!
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Finally, in 1989 Peter Leonard set the stage for this conferenceAJ 98, 217
CHRONOLOGICAL LISTOF HYPOTHESES
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HOW TO IDENTIFY FBS
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Of necessity, in the field we first identified metal-poor FBS by colorimetry.
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Preston et al. 1994
BM
P st
ars
HK Survey: Beers et al. 1985, 1992
MS [Fe/H] = 0
MS [Fe/H = 1
Metal poor stars near GC turnoff
BHB
W. W. Morgan would have calledthe BMP stars a“natural group”.
Of necessity, in the field we first identified metal-poor FBS by colorimetry.
Any photometricsystem with a
uv filter will work.
RHB
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BM
P st
ars
MS [Fe/H] = 0
MS [Fe/H = 1
Metal poor stars near GC turnoff
BHB
W. W. Morgan would have calledthe BMP stars a“natural group”.
Of necessity, in the field we first identified metal-poor FBS by colorimetry.
Any photometricsystem with a
uv filter will work.
RHB
FBS area subset of BMP
Preston et al. 1994
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In BMP domain isochrones with a wide range
of ages and metallicities overlap in a tangled mess.
Preston & Sneden 2000
Isochrones of various [Fe/H] values and ages overlap in a 2-color diagram of the BS domain.
RYI IsochronesGreen et al. (1987)
main sequence isochrones
subgiant isochrones
Turnoffs for: [Fe/H] = 2.2 ages 3 7,10 Gy
Hence, “straggle”
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In BMP domain isochrones with a wide range
of ages and metallicities overlap in a tangled mess.
Isochrones of various [Fe/H] values and ages overlap in a 2-color diagram of the BS domain.
main sequence isochrones
subgiant isochrones
Turnoffs for: [Fe/H] = 2.2 ages 3 7,10 Gy
Hence, “straggle”
Location in this trapezoid doesn’t tell us much about
age and composition
Preston & Sneden 2000
RYI IsochronesGreen et al. (1987)
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The cool (red) edge of the BS domain in any stellar system is defined by stars
that are not members of the domain
Mandushev, Fahlman, Richer 1997, AJ
MEMBERSHIP CRITERION
STRANGE DEFINITION
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The cool (red) edge of the BS domain in any stellar system is defined by stars
that are not members of the domain
STRANGE DEFINITION
Mandushev, Fahlman, Richer 1997, AJ
MEMBERSHIP CRITERION
what I see
what they did
mass transfer sequence
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MOST FBS COMPRISE A SUBSET OF A LARGER FAMILY OF MAIN SEQUENCE MASS-TRANSFER BINARIES
Mandushev, Fahlman, Richer 1997, AJ
Use of MSTO coloras a boundary
obscures this reality
STRANGE DEFINITION
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Mandushev, Fahlman, Richer 1997, AJ
Use of MSTO coloras a boundary
obscures this reality
MOST FBS COMPRISE A SUBSET OF A LARGER FAMILY OF MAIN SEQUENCE MASS-TRANSFER BINARIES
What happened here?
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We all do it!
MOST FBS COMPRISE A SUBSET OF A LARGER FAMILY OF MAIN SEQUENCE MASS-TRANSFER BINARIES
Struve - dodging
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12 Gy isochrone
surely FBS
CS 22949-008pri. & sec.
CASE IN POINTMetal-poor CEMP binaries below MSTO in hierarchical triples
Masseron et al. 2012, ApJ, 751:14
mass transfer sequence
CS 22964-161
= CEMP, literature
~ 3
mag
.
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Mandushev, Fahlman, Richer 1997, AJ
3 m
ag
CS 22949-008secondary
MOST FBS COMPRISE A SUBSET OF A LARGER FAMILY OF MAIN SEQUENCE MASS-TRANSFER BINARIES
mass transfer sequence
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Various tools have been devised to isolate field blue stragglers.Pier (1983) pioneered the identification of FBSs.
FBS
BHBD(0.2)
0.2
Ca II K line versus color Abundance calibration of Ca II K line
any Balmer line what it accomplishes
FBS
BHB
Manduca & Bell 1978
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Clewley et al. borrowed this one from extragalactic astronomy.The Sersic function
Y =
Galaxies are merely Balmer lines turned upside down
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Clewley et al. borrowed this one from extragalactic astronomy.Sersic (b,c) Balmer parameters isolate FBS particularly well.
Their use does not require knowledge of photometric colors.
FBS
BHB
Clewley et al. 2002
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Clewley et al. borrowed this one from extragalactic astronomy.Sersic (b,c) Balmer parameters isolate FBS particularly well.
Their use does not require knowledge of photometric colors.
FBS
BHB
Clewley et al. 2002
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An application of Sersic parameters to Sloan data in the distant halo
(n = 4985)
(n = many)
Xue et al. 2011
A nuisance for Xue et al.
“One man's trash is another man's treasure.”
- old English aphorism
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Sarajedini 1993, ASP Conf. Ser.
Globular clusters provide luminosity calibrationfor Galactic structure applications, e.g. halo (R)
Z = 0.0001 Z = 0.004
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MV) 0.5 mag/star(distance) 3 %/100 stars
Sarajedini 1993, ASP Conf. Ser.
Globular clusters provide luminosity calibrationfor Galactic structure applications, e.g. halo (R)
Z = 0.0001 Z = 0.004
68% within 1
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GROUP PROPERTIES OF FBS
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It is easy to find binaries among FBS candidates
RV-constant stars Binary stars
A child can do it
JD - 2400000
10 years
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A high % of FBS are members of spectroscopic binaries
Preston & Sneden 2000
4 km/s
20 km/s
vertical scales are not uniform
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Very high (70% vs 15%)
Preston & Sneden 2000, AJ
A high % of FBS are members of spectroscopic binaries
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But a low % of FBS are in double-lined spectroscopic binaries
Very low (essentially zero)
≤
The one DLSB, CS 22873-139, included here is contested by Spite et al. 2000, A&A, 360, 1077
Preston & Sneden 2000, AJ
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FBS & CEMP binaries have distinctive orbital characteristics
Normal MS binaries disk = xhalo = o
BMPblue metal-poor
C, s-process rich
Preston & Sneden 2000, AJ
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FBS & CEMP binaries have a high % of small orbital eccentricities, deficits of short periods, and no P > 4000 d
deficit of short periods
excess of low eccentricities
Normal MS binaries disk = xhalo = o
BMPblue metal-poor
C, s-process rich
Preston & Sneden 2000, AJ
COROTATIONcircularization
Vrot 50R/Porb
Porb Vrot
25 2 10 5 5 10 1 50
no BMP, CEMPbinaries
with P > 4000 d
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and their small mass functions suggest companions with white dwarf masses (~ 0.6M).
f1 = K13 P / (2 π G) = M2
3 (sin3 i) / (M1 + M2)2
FBS Ba, CH cousins
Preston & Sneden 2000, AJ McClure & Woodsworth 1990, ApJ
FBS BaII
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All of the preceding:High binary fractionDeficit of short (and very long) periodsLow orbital eccentricitiesSmall mass functionsNo visible secondaries *And Thank You, Erika, for Capricorni
tell us that FBS are a species sui generis
* Hierarchical triples excepted
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white dwarfflux red wing of L
in white dwarf
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All of the preceding:High binary fractionDeficit of short periodsLow orbital eccentricitiesSmall mass functionsFew (no) visible secondariesAnd Thank You, Erika, for Capricorni
tell us that FBS are a species sui generis
My perspective:Wide binary disruption is main reason
for the specific frequency deficitin GCs relative to the Galactic field
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4.0
FBS
FBS
Specific frequency of FBS appears to be the upper bound of a sequence defined by OCs (DeMarchi et al 2006) and GCs (Piotto et al 2004)
This is a lo
garithm
This isn’t
Something like “concentration” must be what matters
Preston & Sneden 2000, AJ
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visualbinaries
c.p.m.binaries{
radial velocitybinaries P<4000 d
This 13% of radial velocity binaries with P 5 d merge in less than a Hubble time (Vilhu, 1982, A&A, 109, 17). Hence, the deficit of short period binaries in the field.
These more frequent wide binaries are largely disrupted in GCs. Hence, the relatively low specific frequency of blue stragglers in globular clusters.
This interpretation follows fromthe presumption that the
Duquennoy-Mayor (1991, A&A)period distribution is universal.
Ockham’s Razor, etc
William of Ockham1248-1307
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DUSTING
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DUSTING
Wind accretion
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How do you hide it?
DUST: The thin layer that you notice on tables
just before your guests arrive
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In the house use this
DUST: The thin layer that you notice on tables
just before your guests arrive
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In stars redistribute by thermohaline mixing.
DUST: The thin layer that you notice on tables
just before your guests arrive
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Reconciliation of theory and observation
Observational facts & procedures:
Census of orbital parameters for MS and post-MS C and Ba starsDetection criteriaDetection threshholds bias incompletenessObserver persistence (w/r RV)
Theory:
Mass transfer by winds Including details like solving the Davies-Pringle (1980) puzzle.
AGB theory and practice of Busso & Gallino andConvective envelopesGravitational settling and stabilizing molecular gradientsDilution with and without thermohaline mixing
those
those
all
otherItalian
s
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those
all
How many MS CEMP survive the RGB ascent?
INNOCENT QUESTION:
Is the observed density ratio (RGB)/(MS) OK?
MS
CEMP(RGB)
CEMP(MS)
(kpc-3) = space densityn = nuclear time scale
relative volumes searched (in apparent magnitude limited surveys)
RGB
IF (crude example) LRGB /LMS ~ 40
i. e.,Volume ratio = VR ~ 250
and withn(RGB)/n(MS) ~ 102
OBTAIN(RGB)/(MS) ~ VR*n~ 2.5
Is this OK?
M
V ~ 4 m
ag
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those
all
How many MS CEMP survive the RGB ascent?
INNOCENT QUESTION: Is the observed density ratio (RGB)/(MS) OK?
MS
CEMP(RGB)
CEMP(MS)
relative volumes searched (in apparent magnitude limited surveys)
RGB
In other words,Do
Thesemapinto
Those?
THE QUESTION:Does
This populationmapinto
That population
?
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those
those
all
Stars with “no-dilution” solutions
dilution dil = log MCE/MAGBacc
x
dilutions from Bisterzo et al. 2012, MNRAS, 422, 849
All the CEMP stars with “no-dilution” solutionslie near or above MSTO; ~ half are FBS)
MSTO
n(RGB)/n(MS) ~ 2.5 in Bisterzo et al. sample. Agreement not so bad. I was a bit surprised.
dilu
tio
n
pure AGB
Vertical lines indicate ranges of solutions
No dilution
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2012
FBS 7000ºK no dilution RGB 5280ºK dil = 0.7, 1.7
adjust model parameters to minimize residuals 0.2 dex
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We have very little information about wind accretion at large distances from an AGB donor.
[s]
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Regression below is anchored by two long-period SLSBswith primaries originally classified as ordinary GK giants!
Griffin 1985
G8 III
K0 III
[s]
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Regression below is anchored by two long-period SLSBswith primaries originally classified as ordinary GK giants!
Griffin 1985
G8 III
K0 III
Want more candidates? See McWilliam 1990, ApJS, 74
23/671= 4% of GK giantsV(mag) 6.0, [s] > 0.2
Expect 20,000 more in HD (V<11)
[s]
0.2
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A bunch of calculations for MS stars with various
ages and [Fe/H]
Pinsonneault, DePoy, & Coffee 2001, ApJ
FBS convection zone rapidly disappears at Teff > 6500 K
He, Sr, Ba, sink in M2 prior to AGB evolution of M1.
Negative –gradient inhibits thermohaline mixingWhat happens when a Ba-rich long-P FBS ascends RGB?
Will we recognize it, or will it disappear?
7000
-3.5
-4.0
Humoris still alive in
the USA!
FBS live here
loga
rith
ms!
!
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VB
CPM
The period distribution of Ba stars declines at P > 2000 d and dies at P ~ 5000 d, but the period distribution of MS binaries peaks at P > 10000 d.
(Jorissen & Van Eck 2001)
Extant data provide a clue.
F-G binaries ofDuquennoy & Mayor 1991
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(Jorissen & Van Eck 2001)
F-G binaries ofDuquennoy & Mayor 1991
VB
CPM
The period distribution of Ba stars declines at P > 2000 d and dies at P ~ 5000 d, but the period distribution of MS binaries peaks at P > 10000 d.
Extant data provide a clue.
observer persistence problem?
or what?
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Orbital speeds at P = 10000 days are easily measured by modern spectrographs.
An unavoidable conclusion: winds “run out of gas” at some long P. Which?
2 3 4 5 6
log P(days)
0
5
10
15
20
K1 (k
m/s
)
m1 = 0.8, m2=0.5
K13P = constant
Newton’s laws are very tolerant of long orbital periods.
VB CPMRV source of data
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THOSE YOUNG A-TYPE STARS FAR FROM THE GALACTIC PLANE
ANOTHER INCONVENIENT TRUTH
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This began long ago with Charles Perry and Alex Rodgers
Perry*1969 Rodgers*1971; Rodgers*, Harding*& Sadler 1981
I circled and boxeddata for
metal-rich A starsthat stray far from
Galactic plane
AVG = 5250 AVG = -0.23
* People I have known forever
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This all began with Perry and Rogers, Harding & Sadler
Perry 1969 Rogers, Harding & Sadler 1981
I circled and boxeddata for
metal-rich A starsthat stray far from
Galactic plane
AVG = 5250 AVG = -0.23
Santos et al. 2009, A&AThe average [Fe/H] for these A-Stars 5 kpc from the Galactic plane is slightly lower
than the average value near the sun.
* People I have known forever
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Perry 1969 Lance 1988
north south
log
g
= 5040/T
W(A stars) = 62 km/sW(thick disk) = 42 km/s
Lance (1987): Early A-type stars far from the Galactic plane
two-slope density signature, larger W, hotter than BMP
700
0
800
0
900
0
100
00
Teff
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Perry 1969 Lance 1988
They are apparently quite youngIf they are blue stragglers, what do they straggle behind?
north south
log
g
= 5040/T
W(A stars) = 62 km/sW(thick disk) = 42 km/s
isochrone fort = 5.0E+8 y
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isochrone fort = 5.0E+8 y
Rodgers/Lance hypothesis: star formation during recent interaction
of a metal-poor, gas-rich satellite with the disk of the Milky Way.
They are apparently quite youngIf they are blue stragglers, what do they straggle behind?
log
g
= 5040/T
W(A stars) = 62 km/sW(thick disk) = 42 km/s
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Rodgers/Lance hypothesis: widely ignored in discussions of Milky Way halo
widely accepted in discussions of distant mergers
Young GCs in NGC 7252
(Schweizer & Seitzer 1998)
Lots of young stars In these globular clusters!
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Rodgers/Lance hypothesis: widely ignored in discussions of Milky Way halo
widely accepted in discussions of distant mergers
H imageTrue Color
youn
g fie
ld s
tars
1st p
ass
over
lap
regi
ondu
st o
bscu
red
2nd
pass
even
you
nger
sta
rs2n
d pa
ss
(Whitmore et al. 1999)
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CHEMICAL ABUNDANCES ABOVE AND BELOW
THE MSTO
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Deep mixing accompanying merger, collision, mass transferburns 7Li to 4He ash low Li is a straggler signature.
BUT confirmation requires a big telescope for most FBS.
data from Thorburn 1994, ApJ, 421
M
ST
O
TERRITORY
BLUE STRAGGLER
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Deep mixing accompanying merger, collision, mass transferburns 7Li to 4He ash low Li is a straggler signature.
BUT confirmation requires a big telescope for most FBS.
data from Thorburn 1994, ApJ, 421
M
ST
O
NB: Li deficiencies also occur below MSTO
Mass transfer sequence again
?
!!!
BLUE STRAGGLER
TERRITORY
?
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data from Preston & Sneden 2000, AJ
Galactic FBS
dSph red giants
halo stars
Compare dSph red giants to Galactic stars – Venn et al. 2004, AJ
thick disk
thin disk
What we might learn from the -elements.
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What we might learn from the -elements.
data from P&S 2000, AJ
Galactic FBS
dSph red giants
halo stars
Compare dSph red giants to Galactic stars – Venn et al. 2004, AJthick disk
thin disk
RV-constant BMP stars: Intermediate-Age captures
from a dSph satellite like Carina?
Stetson et al. 2011, ESO Messenger
13 Gy
8 Gy
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CH
The “non-variable” spectrum is the
mean of three stars
The FBS binary CS 29497-030 illustrates how the carbon signature responds to an increase in Teff
C I
Enter the AGB: Carbon and n-capture elements
G-band becomes inconspicuous
Atomic C becomesbetter signature
Sneden, Preston, & Cowan 2003, ApJ
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Note similarities of Fe-peak lines
versus disparities of the Ba and Pb lines
The “non-variable” spectrum is the mean
of three stars
CS 29497-030 = FBS (B-V)0 = 0.30
CS 29497-030 = FBS (B-V)0 = 0.30
OTHER DIAGNOSTICS
Sneden, Preston, & Cowan 2003, ApJ
Lead-rich binary CS 29497-030
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The “non-variable” spectrum is the mean of
three stars
Question:Is this a FBS?(B-V)0 = +0.30(U-B)0 = - 0.14[Fe/H] = - 2.6
CS 29497-030 = FBS (B-V)0 = 0.30
CS 29497-030 = FBS (B-V)0 = 0.30
MSTO color vs [Fe/H]
Every FBS has its own red color boundary
Answer: Yes
Lead-rich binary CS 29497-030
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So, use [Fe/H], (B-V)0 to identify FBS, star-by-star
Question:Is this a FBS?(B-V)0 = +0.40(U-B)0 = - 0.14[Fe/H] = - 2.2
MSTO color vs [Fe/H]
Answer: No
hypothetical FBS candidate x
Hypothetical FBS candidate
DÉJÀ VU ALL OVER AGAIN!
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neutron/seed ratio decreases
X = IA pop = BS pop
x
Orbit dimensions, RGB, AGB mass transfer FBS binaries ( ): n-capture normal abundances (low [C/N], high 13C/12C )
mass transfer only during RGB evolution
FBS binaries ( ): n-capture over-abundances (low [C/N], high 13C/12C ) mass transfer during RGB & AGB evolution
FBS single stars (X): n-capture normal abundances (high [C/N], low 13C/12C ) no mass transfer
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FBS PULSATORSFBS PULSATORS
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Pulsation like this would produce chaos in FBS binary RV curves,so we know that such pulsators are rare among FBS binaries.
30 km
/s
ORBIT
PULSATION
ΔV ~ 0.1 mag.
Shift due toorbital motion
Preston & Landolt 1999 AJ
54 minutes
317 days
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30 km
/s
54 minutes
Conclusion: Such pulsation is rare among metal-poor FBS(like 1/42 2 or 3 %) although most FBS lie in instability strip
ORBIT
PULSATION
Preston & Landolt 1999 AJ
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HADS confined to narrow band in the instability strip.McNamara (1997), Petersen & Dalsgaard (1999)Kepler data confirm (Balona & Dziembowski 2011)Pulsator fraction: ~ 0.5 only in HADS band < 0.5 everywhere else
Sct instability strip
McN
amar
a’s
field
sta
rs
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Poretti et al. 2008, ApJ
RR Lyraes fill their instability strip, but SX Phe stars in Fornax II probably are confined to McNamara’s HADS strip.
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RR Lyraes fill their instability strip, but SX Phe stars in Fornax II probably are confined to McNamara’s HADS strip.
Poretti et al. 2008, ApJ
RR Lyr
SX Phe
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STARS THAT DON’T FIT
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2500 3000 3500 4000 4500 5000 5500
Julian Date
-60
-50
-40
-30
-20
-10
0
10
20
30
RV
(km
/s)
TY Gru 2003 - 2010
C & s-process rich stars that don’t fitC & s-process rich stars that don’t fit
1 km/s
20 years
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2500 3000 3500 4000 4500 5000 5500
Julian Date
-60
-50
-40
-30
-20
-10
0
10
20
30
RV
(km
/s)
TY Gru 2003 - 2010
C & s-process rich stars that don’t fitC & s-process rich stars that don’t fit
After so many years of this– NADA!
1 km/s
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2500 3000 3500 4000 4500 5000 5500
Julian Date
-60
-50
-40
-30
-20
-10
0
10
20
30
RV
(km
/s)
TY Gru 2003 - 2010
C & s-process rich stars that don’t fitC & s-process rich stars that don’t fit
After so many years of this– NADA!
1 km/s
Tengo 82 anos – no mas para mi. I quit!
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Typical FBS
CS 22949-008
Not yet
Lyrae
Evans, D. 19XX (GWP can’t find reference)