observations of globular clusters (of relevance for the modest collaboration) giampaolo piotto...
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Observations of Globular Clusters
(of relevance for the MODEST collaboration)
Giampaolo PiottoDipartimento di Astronomia
Universita’ di Padova
Collaborators: Jay Anderson, Luigi R. Bedin, Santi Cassisi, Francesca De Angeli, Ivan R. King, Yazan Momany, Marco Montalto, Alejandra Recio Blanco, Sandro Villanova
Recent Instrumental Advances
A stro m etry P h oto m etry (?)w ith A C S
HST (!)
P h oto m etry
P re -F la m es P ro pe r M o tion
A stro m etry
W FI
V elo c ities A b un d an ces
FLAMES@ VLT
New Observational Facilities
New instruments for both imaging and spectroscopy have strongly affected the research topics in globular cluster astronomy. We have also started to take advantage of the 20-25 year baseline of images on solid state digital imagers and, overall, of more than 10 year baseline of HST imaging for for high accuracy proper motions!
High Precision Astrometry on WFPC2/ACS HST Images
Just the random error remains ~0.02 pxl on the WFPC2 (~0.01 pxl on the ACS)
which correspondsto 1 mas (PC) on a single imagewith N images:
N: ~1 mas /sqrt(N) (in the PC case)
(Anderson and King 2002, 2003)
(Bedin, Anderson, King, Piotto 2001, ApJL, 560, L75)
Hunting the bottom of the Main Sequencedown to the hydrogen burning limit (HBL)
NGC6121=M4
Astrometry (1):Identify clustermembers for deep surveys
Luminosity-Radius Relation Luminosity-Radius Relation (LRR)(LRR)
The modelscannot fit themain sequence at intermediateand highmetallicities (Bedin et al. 2001)
NGC 6397
M4
low [M/H]
intermediate [M/H]
King, Anderson, Cool, Piotto, (1999)
Bedin et al. 2004, in prep
Mass functionsin differentradial bins:
Observationalconstrainton mass segregation.Set constraintson the clusterdynamical model.NGC 6121 = M4
Cluster Camera [Fe/H] NGC6397* WFPC2 -2.2NGC6121* WFPC2/ACS -1.2
NGC104 ACS -0.7NGC6791 ACS +0.4
NGC5139 ACS -1.6/-0.5
Ongoing projects
Bedin, Piotto, King, Anderson, in prep.
GO9444
GO9648
Example:47 Tucanae
CMD spanningmore than 17 magnitudes,from the RGB tip downto Mv~15,close to the HBL
ABSOLUTE MOTIONSAstrometry (2):Measure proper motions
(U,V,W)LSR = ( 53+- 3, -202+-20, 0+- 4)Km/s
, LSR = ( 54+- 3, 16+-20, 0+- 4)Km/s
…of M4:
Once corrected l cos b and b
for the Sun peculiar motion we can get
Bedin, Piotto, King, Anderson 2003, AJ, 126, 247
Astrometry (3):GEOMETRICAL DISTANCESOF GLOBULAR CLUSTERS
This is our major project, at the moment
Globular cluster age measurement error is dominated by uncertainty on distance, which is at
least ~10% => 0.2 mag distance modulus,
which translates in a >25% error in age!!!
Direct measurements of distances are several years away (GAIA, SIM,…)
and we have to rely on standard candles, whose luminosiy is still
poorly known, and sometimes strongly dependent on other parameters
as metallicity (e.g. RR Lyrae).
We need reliable measures of distancesfor as many GGCs as possible,
covering a wide range of metallicitiesin order to measure accurate ages
Our method is very simple (…in principle… )
we compare the dispersion of the internal proper motions
(an angular quantity)with the dispersion of
the radial velocity(a linear quantity)
it is not a new idea, but now…
INTERNAL DYNAMICS
(Bedin et al. 2003)
…and thanks to instrumentslike the highresolutionmultifiberspectrographFLAMES@VLT:
We get thousands of radial velocities per
night!!!
The main source of error is the sampling error: 1/sqrt(2N).
For a typical sample of 3,000 stars this implies an error of 1.3% in the distance.
The distance scale obtained will not be only sound, but its uncertainty will no longer contribute to the uncertainty on the age estimates.
NGC 2808
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Error budget is very important!
This is a preliminary calculation!!!This is a preliminary calculation!!!
Harris 2003: 2.2 kpc… Diff= 20% closer!!! Better agreement with Peterson, Rees & Cudworth et al. d=1.72+/-0.14 kpc
(Formula from Pryor & Meylan 1993)
The sources of systematic errors are: - estimates of the observational errors
PLUS
- mass segregation - rotation MODEL !!! - anisotropies
We fit the observed radial velocities and internal proper motions with a superposition of orbits constructed with an axisymmetric dynamical model (Schwarzschild models). The orbit library is generated using the code developped by Gebhardt et al. (2000).
F. De Angeli PhD thesisPreliminary results for 47Tuc
Model predictions
O Data
Ongoing work on proper motions: example
HST observations completedlast month
GO9899, PI: Piotto
Ongoing work on radial velocities: example
NGC2808: 2000 stars observed
(FLAMES@VLT, PI: Piotto)
In addition: NGC6121 (2600*) NGC6397 (1700*) NGC6752 (1500*)
Geometrical distance project priority list
NGC 6121 Least model dependent!NGC 2808NGC 6752NGC 6397NGC 5139NGC 104
plus 7 other clusters with at least two epoch HST observations
Why should all this beof interest for MODEST?
From the various proper motion projects we get:
1) Accurate proper motions AND radial velocities for up to a few thousand stars, from the cluster center to many core radii from the center;
2) Mass functions, in a few cases down to 0.1 solar masses;
3) Mass segregation;4) For a selected number of clusters, accurate distances
and ages;5) In some cases, absolute motion
Accurate Reddening and Metallicity measurement with GIRAFFE/UVES+FLAMES@VLT
Cluster Giraffe UVES Ongoing ESO program(PI Gratton)
Targets:Metallicities with 0.03dexuncertainties (UVES data)
Reddening with 0.005 mag.uncertainty (GIRAFFE data
Coupled with the geometric distance project we should be able to measure GC ages with a few 100 Myr uncertainties
• 74 GC cores observed with the WFPC2 in the F439W and F555W band [all clusters with (m-M)B<18];
•Data reduced with DAOPHOT and ALLFRAME;
•Data calibrated to both HST Flight and standard Johnson B, V systems following Dolphin (2000);
•Completeness available for all the CMD branches (7100 experiments with more than 5 million artificial stars)
•Photometric data and completeness are available at http://dipastro.pd.astro.it/globulars
• The database has proven to be a mine of information
Piotto et al. (2002), A&A, 391, 945
Relative Ages of Galactic Globular Clusters
Within each single bin, GCs are coeval,with an age dispersion less than1Gyr (smaller forthe most metal poorclusters).
Clusters with [Fe/H]<-1.5 appears1.5-2 Gyr younger,but this second results is totallymodel dependent.
Omega Centauri:the population puzzle goes deeper
Astrometry (4):Omega Centauri.
Accurate astrometry implies accuratephotometry!
Bedin, Piotto et al. 2004, ApJL, 605, L125
The problem of the double MS and ofthe multiple SGBs and TO
While the multipleTO could be understood in termsof a metallicity (andage) spread,the doublemain sequence represents a realpuzzle.
Is it a structure inthe background?
Bedin, Piotto, Anderson et al. 2004, ApJL, 605, L125
Leon, Meylan, & Combes 2000
Bedin et al. (2004) have proposed an alternative explanation for the Omega Centauri double main sequence: It represents a population of super-helium rich stars (Y>0.30), which might be originated by material polluted by intermediate mass (1.5-3 solar masses) AGB star ejecta.
This would be consistent with: 1) The increase of s-process elements with metallicity found by Smith et al. (2000) 2) The anomalously hot horizontal branch 3) The lack of correlation between period shift and metallicity among RRLyr stars (Gratton et al. 1986)ESO DDT project (PI Piotto) approved for 15hr at FLAMES@VLT in order to verify this hypothesis3 HST extra orbits allocated on DDT (GO10101, PI King)
17 blue main sequence17 red main sequence33 upper SGB32 middle SGB23 lower SG
FLAMES+GIRAFFEObservatiosin June2004
First results: the double main sequence
Piotto et al., ApJL, in preparation
17x12=204 hours i.t.
RedMS:Rad. Vel.: 235+-11km/s[Fe/H]=-1.56
BlueMS: Rad. Vel.: 232+-6km/s[Fe/H]=-1.27It is more metal rich!
Other chemical elements:
Red Main Sequence:
[C/Fe]=0.0[N/Fe]~1.0[Ba/Fe]=0.4
Blue Main Sequence
[C/Fe]=0.0[N/Fe]~1.0[Ba/Fe]=0.7
The blue main sequence stars are richer in Ba (s-process element), but NOT carbon rich. This is the second important result.
The fact that there is no significant radial velocity difference and no significant difference in proper motion make the background object explanation even more unlike.The only other possibility is indeed a strong He overabundance
An overabundance of helium (Y~0.40) indeed can reproduce the observed blue main sequence.
The fact that the more metalrich, and possibly helium richer stars are not carbonrich seems to exclude that the cloud has been contaminated by AGB ejecta.
According to Thielemann et al. (1996) SNe from 8-12 solar mass stars should produce a huge amount of helium. Material pollutedby these SNe could in principle originate stars with the chemical content of the blueMS stars in Omega Centauri.
Future Plans:
Observations:1) Reduce the new ACS/HST images (foreseen for June 2005)to follow the two MSs in Omega Cen down to the hydrogen burning limit; Use the first epoch of the same field for accurateproper motions of the stars in the two MSs
2) With improved ACS photometry search for main sequence splits and/or broadening in other globular clusters.
Theory (of interest for MODEST!)1) Investigate the fraction of material ejected by SNe from 8-12 solar mass stars that can be retained within the cluster (see also proposal at the end of the talk).
NEXT STEP FOR ASTROMETRY:GROUND-BASED ASTROMETRY
Example: [email protected] ESO ~12 mas/frameA post doc (Ramakant Singh Yadav)full time dedicated in Padova
NG
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IN JUST ~2.8yrIN JUST ~2.8yr
Blue Stragglers from the snapshot catalog
•Blue stragglers (BS) are present in all of our 74 CMDs;•Almost 3000 BSs have been extracted from 62 GCs;•The location of BSs in the CMD depends on metallicity;•The brightest BSs have always a mass less than 1.6 solar masses;
•In all GCs, BSs are significantly more concentrated than other cluster stars.
Piotto, De Angeli et al. (2004, ApJL, 605, L125)
Ns represents the density of stars in a cluster.(i.e. the observed number of stars has been divided by the fraction of the cluster light sampled by our WPFC2 images, and then divided by the total cluster light).
There is a significant correlation between the BSS frequency and the total cluster luminosity (mass)and a very mild anticorrelation with the central collision rate.
Here, we plot theestimated total numberof stars, obtained from the observed counts, divided by the fraction of the cluster light sampled by our images
Note that:
1) The total number of HB stars scales linearly with Mv,or the total mass,as expected.
2) The number of BSis largely independentfrom the total massand the collision rate.
Evolutionary pathway to produce Blue Stragglers in GCs
Davies, Piotto, De Angeli 2004, MNRAS, 349, 129
A more massive main sequence star exchanges into a binary containing two main sequence stars.The primary evolves off the mainsequence and fills the Roche lobe.The secondary gains mass and becomes a blue straggler.
Blue stragglers will form earlier inbinaries containing more massivestars, i.e. in high collision rate clusters.
Given the finite lifetime of a blue straggler, the blue straggler population (from primordial binaries) in the most crowded clusters today could be lower than in very sparse clusters.
Production of Blue Stragglers in GCs
Davies, Piotto, De Angeli 2004
Blue Straggler Luminosity Function
On the basis of ourmodel, we expect tofind predominantlyBS produced by collisions in clusterswith Mv<-8.8.These BS areexpected to bebrighter(Bailyn andPinsonneault 1995)
This prediction seems to be confirmed bythe observed luminosity function.
We have extended our investigation to open clusters…
GCs
Open clusters
NEW!!!!
The trendscontinues into the mass regimes of (relatively) old open clusters(age>0.5Gyr).
(The high noisefor open clustersis mainly due tothe small numberof red clump stars.)
Log(age)
Total Absolute Magnitude
BSS in Open Clusters
If we include the totalcluster sample, theanticorrelation with the total magnitude (mass) iseven more evident(extending the trendalready observed for GCs).
Apparently, there is also a correletion with the cluster age, with older clusters having more BSS
Extended horizontal branches
22 out of the 74 clusters of the snapshot database show a blue tail which extendsto Te>=20.000K, entering into the EHB regime.
A number of these have been identified as EHB clusters within the snapshot project.
In practice, 25-30% of the clusters of our sample have a blue tail extended to Te=20.000K or more.
EHB are not so rare, after all!
WHY?
Horizontal Branch Extension
For each cluster wefitted a model to obtain the temperature ofits hottest stars, as an index of the HBextension.
Then we started byexploring simplepairwise correlations.
Metallicity: the first parameter
Clearly there is acorrelation betweenthe HB extension andmetallicity. The metallicity is the firstparameter, afterall.
There is also a large dispersion. Indeed, The metallicity explains only 32% of the total variance.Basically, this is the“second parameterproblem.”
New important correlations: the total absolute magnitude
The total absolutemagnitude accountsfor 19% of the totalvariance.
Note the if we remove the mostmetal rich clusters(for which the metallicity effect dominates), thecorrelation betweenthe HB extension and the total absolutemagnitude (mass) ismuch stronger.
No correlation with the central density or otherrelevant cluster
parameters
Multicomponent Analysis
PCA analysis confirms that the HB extensioncorrelates with [Fe/H] and Mv(i.e. total mass)
Why the dependence on the total cluster mass?A possible explanation could be related to what we have found in Omega Centauri:
self pollution!IF a significant fraction of the material lost by intermediate mass AGB stars and/or SNe can be retained by the cluster and contaminate the medium from which less massive stars are still forming,we would end with low mass stars richer in helium. Stars richer in helium would become bluer HB stars.
In this scenario: more massive clusters
would be able to retain material from the AGB/SNe ejecta than
less massive ones, and therefore would end with
more extended HBs as observed!
D’Antona et al. (2002)
A proposal for MODEST collaboration
The new results in Omega Centauri and on the extension of thedependence of the horizontal branch in globular clusters on thecluster total mass rise a number of questions.
1) Can the ejecta from SNe generated by 8-12 solar mass stars be retained inside a globular cluster?
2) Can the ejecta from intermediate mass AGB stars be retainedinside a globular cluster?
3) Which is the fraction of retained ejecta as a function of thecluster mass, mass function, etc.?
4) Which is the resulting chemical contamination?