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The i process and CEMP stars - INDICO-FNAL (Indico)CEMP stars: heavy elements Lugaro et al. (2012),...

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The i process and CEMP stars Credit: HST/NASA/ESA Melanie Hampel Monash University
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  • Theiprocessand

    CEMPstars

    Credit:HST/NASA/ESA

    MelanieHampel

    MonashUniversity

  • Withthanksto…

    Credit:HST/NASA/ESA

    RichardJ.Stancliffe

    MariaLugaro

    (Budapest)

    BradleyMeyer

    (Clemson)

  • CEMPstars:heavyelements

    Lugaroetal.(2012),datafromMasseronetal.(2010)

    highBa

    highBaandEu

  • CEMPstars:heavyelements

    Lugaroetal.(2012),datafromMasseronetal.(2010)

    CEMP-s

    CEMP-s/r,-r/s,-r+s,…,-i

  • FormaRonofCEMP-sstars

    1 2

    MSMS

    Credit:CarloAbate

  • FormaRonofCEMP-sstars

    Credit:CarloAbate

  • FormaRonofCEMP-sstars

    1 2

    white dwarfMS

    CEMP star

    Credit:CarloAbate

  • BinaryevoluRon+AGBnucleosynthesis?

    Abateetal.(2015)

  • BinaryevoluRon+AGBnucleosynthesis?

    Abateetal.(2015)

    Atomicnumber

    CEMP-s

  • BinaryevoluRon+AGBnucleosynthesis?

    Abateetal.(2015)

  • BinaryevoluRon+AGBnucleosynthesis?

    Abateetal.(2015)

    Eu

    [hs/ls]

    heavyRE

  • BinaryevoluRon+AGBnucleosynthesis?

    Abateetal.(2015)

    Atomicnumber

    CEMP-s

    CEMP-s/r

  • R-processpre-enhancement?

    Lugaroetal.(2012)

    IniRal

    r-process

    enrichment:

    atleast

    [r/Fe]>1dex

  • R-processpre-enhancement?

    Bisterzoetal.(2012)

    IniRal

    r-process

    Enrichment:

    [r/Fe]=1.5dex

  • R-processpre-enhancement?

    Bisterzoetal.(2012)

    IniRal

    r-process

    Enrichment:

    [r/Fe]=1.5dex

    [hs/ls]

    heavyRE

  • R-processpre-enhancement?

    Bisterzoetal.(2012)

    IniRal

    r-process

    Enrichment:

    [r/Fe]=1.5dex

    HowdoCEM

    P-s/rform?

    ??

  • R-processpre-enhancement?

    Bisterzoetal.(2012)

    IniRal

    r-process

    Enrichment:

    [r/Fe]=1.5dex

    Modifiednucleosynthesis?

    Intermediateneutroncaptureprocess?

    HowdoCEM

    P-s/rform?

    ??

  • iprocess:n≈1015cm-3

    15 2010

    slow

    neutron

    captures

    n≈107cm-3

    rapid

    neutron

    captures

    n>1020cm-3

    intermediate

    neutron

    captures

    n≈1015cm-3

    logn

  • sprocess:n=107cm-3

    1.0e-2

    1.0e-3

    1.0e-4

    1.0e-5

    1.0e-6

    1.0e-7

    1.0e-8

    1.0e-9

    1.0e-10

    1.0e-11

    1.0e-12

    1.0e-1t = 3.15e+12 sT = 1.5e+08 Krho = 1600 g/ccn = 1.0e+07 /cctau = 5.0 /mb

    44 46 48

    50

    52

    54 56

    58

    60

    62 64

    66 68

    70 72 74 76

    78

    80 82

    84

    86 88

    90 92

    94

    96

    34

    36

    38

    40

    42

    44

    46

    48

    50

    52

    54

    56

    58

    60

    62

    64

    Z

    N

    massfracRon

    low

    high

  • HigherneutrondensiRes:n=1010cm-3

    1.0e-2

    1.0e-3

    1.0e-4

    1.0e-5

    1.0e-6

    1.0e-7

    1.0e-8

    1.0e-9

    1.0e-10

    1.0e-11

    1.0e-12

    1.0e-1t = 2.94e+09 sT = 1.5e+08 Krho = 1600 g/ccn = 1.0e+10 /cctau = 4.6 /mb

    44 46 48

    50 52

    54

    56

    58

    60 62

    64 66

    68 70

    72 74 76

    78

    80

    82

    84

    86

    88 90

    92 94

    96

    34

    36

    38

    40

    42

    44

    46

    48

    50

    52

    54

    56

    58

    60

    62

    64

    Z

    N

    massfracRon

    low

    high

  • HigherneutrondensiRes:n=1012cm-3

    1.0e-2

    1.0e-3

    1.0e-4

    1.0e-5

    1.0e-6

    1.0e-7

    1.0e-8

    1.0e-9

    1.0e-10

    1.0e-11

    1.0e-12

    1.0e-1t = 2.79e+07 sT = 1.5e+08 Krho = 1600 g/ccn = 1.0e+12 /cctau = 4.4 /mb

    44 46 48 50

    52

    54 56

    58

    60

    62 64

    66 68

    70 72

    74 76 78

    80

    82

    84

    86

    88

    90

    92

    94

    96

    34

    36

    38

    40

    42

    44

    46

    48

    50

    52

    54

    56

    58

    60

    62

    64

    Z

    N

    massfracRon

    low

    high

  • HigherneutrondensiRes:n=1014cm-3

    1.0e-2

    1.0e-3

    1.0e-4

    1.0e-5

    1.0e-6

    1.0e-7

    1.0e-8

    1.0e-9

    1.0e-10

    1.0e-11

    1.0e-12

    1.0e-1t = 3.06e+05 sT = 1.5e+08 Krho = 1600 g/ccn = 1.0e+14 /cctau = 4.8 /mb

    44 46 48 50 52

    54

    56

    58

    60

    62 64

    66

    68

    70

    72

    74

    76 78 80 82

    84

    86

    88

    90

    92

    94

    96

    34

    36

    38

    40

    42

    44

    46

    48

    50

    52

    54

    56

    58

    60

    62

    64

    Z

    N

    massfracRon

    low

    high

  • HigherneutrondensiRes:n=1015cm-3

    1.0e-2

    1.0e-3

    1.0e-4

    1.0e-5

    1.0e-6

    1.0e-7

    1.0e-8

    1.0e-9

    1.0e-10

    1.0e-11

    1.0e-12

    1.0e-1t = 3.20e+04 sT = 1.5e+08 Krho = 1600 g/ccn = 1.0e+15 /cctau = 5.0 /mb

    44 46 48 50 52

    54

    56

    58

    60

    62

    64

    66

    68

    70 72

    74

    76

    78

    80 82

    84

    86

    88 90

    92 94

    96

    34

    36

    38

    40

    42

    44

    46

    48

    50

    52

    54

    56

    58

    60

    62

    64

    Z

    N

    massfracRon

    low

    high

    Hampeletal.(2016)

  • HigherneutrondensiRes:n=1015cm-3

    1.0e-2

    1.0e-3

    1.0e-4

    1.0e-5

    1.0e-6

    1.0e-7

    1.0e-8

    1.0e-9

    1.0e-10

    1.0e-11

    1.0e-12

    1.0e-1t = 3.20e+04 sT = 1.5e+08 Krho = 1600 g/ccn = 1.0e+15 /cctau = 5.0 /mb

    44 46 48 50 52

    54

    56

    58

    60

    62

    64

    66

    68

    70 72

    74

    76

    78

    80 82

    84

    86

    88 90

    92 94

    96

    34

    36

    38

    40

    42

    44

    46

    48

    50

    52

    54

    56

    58

    60

    62

    64

    Z

    N

    135I massfracRon

    low

    high

    Hampeletal.(2016)

  • iprocess:decays

    1.0e-3

    1.0e-4

    1.0e-5

    1.0e-6

    1.0e-7

    1.0e-8

    1.0e-3

    time(s) = 23815.4 T9 = 0.15 ⇢(g/cc) = 1600 flowmax = 2.47241e � 11

    138Ba

    138Cs

    139Ba

    131I

    136Xe

    131I

    135Ba

    134Ba

    137Ba

    136Ba

    133I

    132I

    135I

    134I

    133Xe

    132Xe

    135Xe

    134Xe

    135Cs

    133Cs

    T1/2=6.6hrs

    T1/2=2.3Myr

    T1/2=9.15hrs

    27

  • Credit:HST/NASA/ESA

  • iprocessabundancepagern

    135I 135Ba

    Hampeletal.(2016)

    -  Higher[Ba/Fe]veryligle138Ba

    -  Higher[Eu/Fe]-  Same[Sr/Fe]

    à higher[hs/ls]

    also,[Ba/La]>0

  • CEMP-istar:LP625-44

    Hampeletal.(2016)

  • CEMP-istars:Residuals

    obs-m

    od

    Hampeletal.(2016)

  • Theiprocess…•  …isnotanewideaàCowan&Rose(1977)

    •  …needsasourceofneutrons:

    Thei process…

    • … isnotanewideaà Cowan&Rose(1977)

    • … needsasourceofneutrons:

  • Theiprocess…•  …isnotanewideaàCowan&Rose(1977)

    •  …needsasourceofneutrons:

  • Producingneutrons

    12C 13C

    (p,γ)

    (β+)

    (α,n)

    13C(α,n)16O

    •  Take 12C and add protons:

    12C(p, γ)13N(β+)13C

    •  Need high temperatures

    •  Proton abundance determines neutron density

    •  It’s a bit messy…

    14C

    13N 14N 15N

    16O 14O 15O

  • NeutronProfiles

    Hampel+2018inprep.

    H

    H

    H

    H

    H

    H

    H

  • drgdfgdfgdfgdfg

    NeutronProfiles:LessisMore!

    ToohighprotonfracRons

    àtooligleneutronexposure

    H

    H

    H

    H

    H

    H

    H

    H

    H

    H

    H

    H

    H

    H

    Totalneutronexposure:

  • CEMP-istar:LP625-44

    Hampel+2018inprep.

  • Conclusions

    •  CEMP-s/rstarsnotreadilyexplainedbyacombinaRonofs-andr-process

    •  Anintermediaten-captureprocessdoesamuchbegerjob! àCEMP-i

    •  NeedtoidenRfyapossiblesourceàprotoningesRonepisodes

    –  LowZAGBstars(e.g.Fujimotoetal.1990, seeSimonCampbell’stalk…)

    –  SuperAGBstars(Jonesetal.2016)–  MassiveStars(seeBanerjee’stalk)–  …


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