Disentangling the complexity of globular clusters: a chemical approach

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Disentangling the complexity of globular clusters: a chemical approach Valentina D Orazi Monash Centre for Astrophysics and Macquarie University Padova, 23 rd September 2013

Globular Clusters: benchmark for stellar evolution Globular Clusters look like an isochrone

Simple stellar Population (SSP): aggregates of single, coeval stars with the same initial chemical composition Location of stars in CMDs of globular clusters = function of the Mass and the chemical Composition of the star In nature, STELLAR CLUSTERS ARE THE BEST EXAMPLE of Simple Stellar Populations (Renzini & Buzzoni 1986)

Globular Clusters are NOT SIMPLE: Multiple MSs, RGBs, SGBs NGC 2808 Lee et al. 1999 Pancino et al. 2000 Bedin et al. 2004 Piotto et al. 2005, 2007 D Antona et al. 2005 Siegel et al. 2007 Zoccali et al. 2009 Anderson et al. 2009 Milone et al. 2008, 2011, 2012 ω Cen NGC 1851 47 Tuc M 22 M 54 NGC 6388

PECTROSCOPY

The Na-O anticorrelation NGC 6397 The Lick-Texas group (Kraft, Ivans, Sneden) Lind et al. 2011 [O/Fe] NGC 5139 (ω Cen) NGC 6121 (M4) Johnson & Pilachowski 2010 NGC 6205 (M 13) NGC 1786 NGC 2210 NGC 2257 Marino et al. 2008 Mucciarelli et al. 2009 Johnson & Pilachowski 2012

Signature of the activation of high-temperature proton capture reactions Giants observed by Ivans et al. (2001) and the Lick-Texas group (Sneden, Kraft, Langer) The NeNa cycle that enhances Na, is expected to operate in the same fusion zones in which the ON part of the CNO cycle is fully operative (Denisenkov & Denisenkova 1990; Langer et al. 1993). CNO: T > 20 MK NeNa: T~ 35 MK MgAl: T> 50 MK 24 Mg depletion: T~70 MK

The smoking gun of the PRIMORDIAL NATURE: The Na-O anticorrelation in GC dwarfs and subgiants Internal mixing is ruled out: Gratton et al. (2001) Cohen et al. (2002) negligible convective envelopes dominant H-burning cycle is p-p not CNO D Orazi et al. (2010a) at least TWO stellar generations

A PREVIOUS GENERATION of stars which synthesised in their interiors proton-capture elements are RESPONSIBLE for these chemical signatures in GC stars HOT hydrogen burning, where the ON, NeNa, and MgAl chains are operating - the ON reduces O, the NeNa increases Na (T ~ 30 million K), while the MgAl produces Al (T~65 million K) In this picture a fraction of the firstgeneration stars (FG, O/Mg/C-rich and Na/Al/N-poor) underwent nucleosynthesis through the proton capture (CNO, NeNa, and possibly MgAl) cycles and polluted the interstellar medium with the processed material via stellar winds. The second stellar generation (SG, O/Mg/C-poor and Na/Al/N-rich) formed from this enriched material, probably within a few hundred Myr Second generation stars (SG) First generation stars (FG)

Our Survey: Na-O abundances in 19 GCs FLAMES@VLT (Giraffe+UVES): more than 100 hours Fe-peak, Na, O, Mg, Al abundances derived for a grand total of about 1200 stars Carretta et al. (2009a)

Stellar generations in GCs: PIE groups E I P Primordial Intermediate Extreme P: [Na/Fe] < [Na/Fe]min+4σ I: [O/Na] > -0.9 E: [O/Na] >-0.9 SN nucleosynthesis Second-generation chemical composition

A feature so widespread among GCs must be related to their origin/formation mechanism (Carretta 2006) A NEW Definition: A bona fide GC is a stellar aggregate showing the Na-O anticorrelation (Carretta et al. 2010) GCs contain multiple stellar generations born in at least two episodes of star formation

Different clusters have different Na-O anticorrelations Different temperatures different polluter masses (?) The shape and the extent of the Na-O anticorrelation vary from GC to GC

The Al-Mg anticorrelation The Al-Mg anticorrelation is not present in ALL the GCs ( POLLUTER S MASS) Carretta et al. (2009b)

The O min = f ([Fe/H],M v ) Different [O/Fe] min + similar [Fe/H] [O/Fe] min depends on M v (mass) Larger average polluter mass..?

Most favourite candidate polluters (alterations in light elements, heavier elements unmodified) Candidate Polluter Location of H-burning Mass involved Pollution Intermediate Mass AGB stars (IM-AGBs, Ventura et al. 2001) Hot Bottom Burning 4 8 M Slow winds and envelope ejection Fast Rotating Massive stars (FRMS, Decressin et al. 2006) Core Heburning 20 120 M Slow equatorial winds Other suggestions: MASSIVE BINARIES (de Mink et al. 2009, Izzard et al. 2013); NOVAE (Maccarone & Zurek 2012)

(Some) Open Issues 1. Relations of p-capture element variations with global GC parameters, e.g., the HB morphology? (see Raffaele s talk) NGC 2808 NGC 1851 NGC 6121 (M4) Gratton et al (2011, 2012) Marino et al. (2011)

(Some) Open Issues 2. The nature of the polluters 1. Relations with global GC parameters, e.g., the HB morphology? (see Raffaele s talk) Fast Rotating Massive Stars Intermediate-mass AGB stars PRO: May produce Y up to Y~0.4 CON: Timescales close to SNII (how do we avoid Fe variation?) NOT enough depletion in Mg (Prantzos et al. 2007; Ventura et al. 2011) NO Mg-Al anti-correlation and NO Mg-Si anticorrelation observed in e.g., NGC 6752, Yong et al. 2005 ) NO Li production PRO: No close over-imposition with corecollapse SNe They can produce discrete values Cannot Both produce candidates discrete value require GCs They burn were Mg initially much more massive They produce lithium (!!!) (preferentially lost of FG stars) or a very peculiar Siess et al. 2007) IMF CON: Y max at 0.36 dex (but see Super-AGBs, Hard to match the highest level of Na enhancement and/or O depletion unless fine-tuning of input physics (convection treatment + fast mass loss rate; Ventura & D Antona 2005, D Orazi et al. 2013a) Rb (s-process elements in general, D Orazi et al. 2013a,b)

Ask lithium It is expected that at CNO/NeNa cycle temperatures occur NO Li is left Polluting material (ejected from the first generation stars) has Li ~ 0 (under the assumption that there is NO Li production within the polluters) Na-poor, O-rich stars (FG stars) should be Li-rich Na-rich, O-poor stars (SG stars, formed from gas progressively enriched by the ejecta of the first population) should be Li poor LITHIUM AND OXYGEN ARE EXPECTED TO BE CORRELATED, AND LITHIUM AND SODIUM ANTICORRELATED While Fast Rotating Massive Stars can only destroy Li, the IM- AGB stars can also produce it via THE CAMERON-FOWLER MECHANISM ( 7 Be transport mechanism, Cameron & Fowler 1971) Any production of Lithium tends to erase the Li O(Na) (anti )correlation

A(Li) The case of M4 D Orazi & Marino (2010) Mucciarelli et al. (2011) [Na/Fe] NO Li O positive correlation and Li-Na anticorrelation: FG Stars and SG stars SHARE the same Li abundances Take-home message: Lithium has been produced between the First and the Second Generation (DILUTION is NOT the explanation!) IM-AGB stars as internal POLLUTERS (?)

1. 3. Relations Does with global SIZE GC matter? parameters, e.g., the HB morphology? (see Raffaele s talk) 2. The nature of polluters (Some) Open Issues Open Clusters vs Globulars GCs with Na-O anticorrelation Terzan 7 and Palomar 12 The Open clusters Berkeley 39 and NGC 6791 Open Clusters are known NOT to exhibit the proton-capture element variations (e.g., De Silva et al. 2009) Gratton, Carretta, Bragaglia (2012, originally from Carretta et al. 2010)

Berkeley 39 Bragaglia et al. (2012): FLAMES observations for 30 giants Abundance analysis for several elements, including Fe, Na, O The observations were optimised to look in particular for possible star-to-star variations in O and Na, which are indicative of the existence of multiple populations in this cluster, in analogy to what is is found for the higher mass, older GCs. No such scatter or anti-correlation was found, and we conclude that Be 39 is a normal, homogeneous, singlepopulation cluster

NGC 6791 Geisler et al. (2012): HIRES @Keck I observations for 5 early RGB stars + Hydra@WYIN for 19 stars in the upper RGB/RC/AGB We found a homogeneous [Fe/H]=+0.42±0.01. Surprisingly, stars are divided Abundance into analysis two subpopulations for Fe, Na, O with different mean O and especially Na contents. Thus, NGC 6791 becomes the first OC to display an intrinsic dispersion in any element and the first presumed OC discovered with multiple populations.

NO Na-O anticorrelation NGC 6791 according to Bragaglia et al. (2013, subm.) [Na/Fe]=0.28±0.03 (rms=0.15) [O/Fe]=-0.18±0.02 (rms=0.08)

(Some) Open Issues 1. Relations with global GC parameters, e.g., the HB morphology? (see Raffaele s talk) 4. Environmental effect Galactic vs extra-galactic GCs 2. The nature of polluters The Fornax globular clusters 3. Does size matter? Letarte et al. (2006): 2 out of 9 stars classified as SG (one in Fornax Cl1 and one in Fornax Cl3)

The LMC globular clusters Mucciarelli et al. (2009): Na-O anticorelation in 3 massive and old GCs (NGC 1786, NGC 2210 and NGC 2257) Mucciarelli et al. 2012 [Na/Fe] Johnson et al.(2006): NO hint of Na-O variations in the old LMC GCs (NGC 2005, NGC 2019, Hodge 11, NGC 1898) Hill et al. (2000) Spread in Al in three stars in NGC 2210

The Sagittarius dsph globular clusters Carretta et al. 2010: Na-O + Al-Mg anticorrelations in the (massive) GC M54 Tautvaiŝienė et al.(2004), Sbordone et al. (2007): No variation in Na,O, Al in Ter 7 Cohen et al. (2004): Homogeneous Na and O abundances in four giants in Palomar 12 [Fe/H]

Carretta et al. (2013, subm.): Giraffe spectra for 10 giants (Fe, Na)+UVES for six RGB (Fe, Na, O) in Terzan 8 None of the stars show O depletion and only one exhibits Na overabundance Ter 8 seems to host SG stars (actually, only one within our sample), although as a minority fraction, the opposite of what is found for higher mass MW clusters, and also at variance with other low-mass Sgr GCs, Pal 12 and Ter 7 (where no significant Na and O spread). Ter 8 may represent a candidate for the class of mainly-fg cluster, while the two other GCs can be considered as good candidates for FG-only clusters (Caloi & D Antona 2011), (but keep in mind that only a very few stars were analysed in the last two clusters)

Other issues include (BUT, unfortunately, are not limited to) 5. Continous vs discrete distributions in Na-O and/or Al-Mg planes? NGC 6121 from Marino et al. 2008 In M4 the distribution of the objects on the Na-O anticorrelation is clearly BIMODAL We provide two independent proofs that the distribution of giants in NGC 6752 is multimodal, with stars segregated into three distinct groups, according NGC 6752 to both from Strömgren photometry and high-resolution spectroscopy. Carretta et al. 2012

6. The exotic Globular Clusters: ω Centauri, M22, NGC 1851, M54.. Along with the the usual variations in elements affected by p-capture we detect significant variations in: [Fe/H], α-elements, s-process elements (to a different extent) ω Centauri (Marino et al. 2011) M22 (Marino et al.2012)

NGC 1851 (Yong & Grundahl 2008) In this peculiar GCs several episodes of star formation are required NGC 1851 (Carretta et al. 2011) Much more complex star formation histories: different timescales different (kind of) polluters involved M54 (Carretta et al. 2010)

That s NOT all folks! What about young massive star clusters? (Portegies-Zwart 2004; Vinko et al. 2009; Larsen et al.2011; Neguerela et al. 2011) Binary fraction and density environment (Milone et al. 2008; D Orazi et al. 2010; Vesperini et al. 2011) The GC formation scenarios (D Ercole et al. 2008, 2010; Bekki et al. 2007, 2011; Conroy & Spergel 2010, Valcarce & Catelan 2011) The different behaviour of AGB stars (Norris et al. 1981; Sneden et al. 2000; Gratton et al. 2010, Campbell et al. 2010, 2013) The GC Milky Way connection (Martell & Grebel 2010; Carretta et al. 2010; Sarah s talk)

The road is long and bendy BUT WE CARRY ON