Nuclear Astrophysics
Physics and Astronomy Department at the University of Washington



Elemental Abundances (lecture by Wallerstein)

6.1 Unevolved stars

Fundamental paper:

Aller and Chamberlain    1951
Found 2 stars metal-poor by factors of factors tex2html_wrap_inline88100

Two important reasons to study unevolved stars:

1 - Need to model such stars in globular clusters, and in nearby galaxies of various types.
2 - Can provide a great deal of information on the nucleosynthesis and mass loss in the Galaxy prior to the formation of other stars of interest.

Examples:
tex2html_wrap_inline90 Sun
tex2html_wrap_inline92 10 Mtex2html_wrap_inline94 stars (type B)
tex2html_wrap_inline90 metal-poor stars (subdwarfs)

Hot, young, massive (tex2html_wrap_inline8810 - 15 Mtex2html_wrap_inline100) stars (see table)
tex2html_wrap_inline90 He possibly enhanced
tex2html_wrap_inline90 CNO
tex2html_wrap_inline90 Mg, Al, Si a little low
tex2html_wrap_inline90 hard to understand

Metal-poor stars
McWilliam et al. 1995, API 109, 2736.

Relative Abundance Distributions

Metal Poor Stars
tex2html_wrap_inline110 - 2.0


tabular9
Data are from McWilliam et al. AJ 109, 2757.


tabular13

Gummersbach et al.

Astron and Ap. 338, 881, 1998.

Important observation log N(S) since S tends to avoid grains.

Note: CNO abundances are hard to understand. Could it be grain chemistry? It is not an effect of CNO cycling.

Composition of stars

August Comte tex2html_wrap_inline88 1810
Frauenhofer tex2html_wrap_inline88 1812
Bunsen (flame tests) and Kirehoff: atomic line lists

Astronomers get into the act:
Secchi: Observed Type III TiO bands and Type IV C-bands:
tex2html_wrap_inline170 first sign of different composition for different stars

Quantitative work:
tex2html_wrap_inline90 1928 Henry Norris Russel: proposed an abundance scale where arbitrarily Ntex2html_wrap_inline174 = 12
tex2html_wrap_inline90 we know now He tex2html_wrap_inline88 11
O tex2html_wrap_inline88 9
N tex2html_wrap_inline88 8
Eu tex2html_wrap_inline88 1

Isotopes from meteorites allow very accurate determinations <1%

Are all stars the same, e.g., hot young stars vs. the sun?

e.g. Hot young stars vs. sun?

Unsold (1939): In a pioneering effort, he argued for abundances around solar values. He was convinced this was universal and seemed to believe all important synthesis occurred in the Big Bang, as in the Alpher, Bethe, Gamow paper of the late 40s.

6.2 Evolved, low-mass stars

References: RMP 1997 69, 995.
Sections by Champagne and by G.W.

The reactions of importance are (see figure)

1. tex2html_wrap_inline188O (p,tex2html_wrap_inline190F(tex2html_wrap_inline192O
followed by tex2html_wrap_inline194 O(p,tex2html_wrap_inline196N etc. tex2html_wrap_inline198 CNO bicycling

2. tex2html_wrap_inline200Ne tex2html_wrap_inline202Na tex2html_wrap_inline204Ne and NeNa cycle

3. tex2html_wrap_inline206Mg tex2html_wrap_inline208Al tex2html_wrap_inline210 Mg and MgAl cycle

Reference RMP Review Oct. 1997 esp. section by Champagne

In M13 a globular with [Fe/Htex2html_wrap_inline214 -1.5, a large spread in [OI/Fe] was found: the spread is from + 0.4 tex2html_wrap_inline220 -0.5. Similar relationships in other cluster but to a varying degree.

This spreading NOT PRESENT IN FIELD STARS:
Why only globulars?

Most recent and detailed effort:
Cavallo et al., ApJ 492 (575) 1998

Background (for physicists) on composition of stars in globulars

tex2html_wrap_inline90 have 10tex2html_wrap_inline224
tex2html_wrap_inline90 round and compact
tex2html_wrap_inline90 found in halo and galactic center
tex2html_wrap_inline90 halo: typical of Baade's pop II
no galactic rotation
low metals
very old tex2html_wrap_inline88 10tex2html_wrap_inline234yrs
tex2html_wrap_inline90 galactic center or disc population:
small rotation
medium metals
almost as old

Quantitative results

1958 HWG M92 [Fe/H] = -2.3
M13 [Fe/H] = - 1.3
From 1 - 3 night exposure with 200 - inch

Not much progress until new detectors become available until 1970's

Slowly, J. G. Cohen, R. Peters, GW and Leep and Oke:
Found spreads in [O/Fe], [Na/Fe], [Al/Fe]

But poor signal/noise made these results doubtful (except perhaps to the authors, of course).

BaII stars (type K pec)
(They do not show Tc)

Cameron 1955: Fundamental paper
suggesting heavy element
production by n-capture
source tex2html_wrap_inline258C(tex2html_wrap_inline260 tex2html_wrap_inline188O. He later suggested tex2html_wrap_inline264Ne (tex2html_wrap_inline260 tex2html_wrap_inline268Mg
tex2html_wrap_inline258C needs tex2html_wrap_inline88 Ttex2html_wrap_inline274 = 150
tex2html_wrap_inline264Ne needs tex2html_wrap_inline88 Ttex2html_wrap_inline274 = 300

Predicting s-process abundances

tex2html_wrap_inline282

For equilibrium tex2html_wrap_inline284

tex2html_wrap_inline286

Total neutron exposure


displaymath288

tex2html_wrap_inline290       tex2html_wrap_inline290

neutron   relative velocity

density    n's and targets

High tex2html_wrap_inline294 makes heavy s-process elements
low tex2html_wrap_inline294 makes low s-process elements
by looking at ratio of hs/tex2html_wrap_inline298s you can determine tex2html_wrap_inline300. Stellar models can tell you time interval, tex2html_wrap_inline302, and so Ntex2html_wrap_inline304 can be estimated.

low tex2html_wrap_inline294 Ttex2html_wrap_inline308 150, Ntex2html_wrap_inline310 tex2html_wrap_inline258C source
high tex2html_wrap_inline294 Ttex2html_wrap_inline308 300, Ntex2html_wrap_inline318, tex2html_wrap_inline264Ne source

Abundances (as [m/Fe]) in an s-process and an r-process star.


tabular66

s-process in stars

Obs. see Section by V. V. Smith in RMP 1997 review
Also section by Kaeppeler in same.

most tex2html_wrap_inline340's have been measured

Can we determine Ntex2html_wrap_inline304 from abundance data: YES

There branching points. Some nuclei have tex2html_wrap_inline344 decay half-lives similar to n-capture time scales.

If Ntex2html_wrap_inline304 is low they tex2html_wrap_inline344-decay
If Ntex2html_wrap_inline304 is high they n-capture

Example - show diagram

Branching at tex2html_wrap_inline352Kr (half-life = 10 years) produces either tex2html_wrap_inline352Rb or capture n and produces tex2html_wrap_inline356Rb.

The ratio tex2html_wrap_inline358

so low Rb tex2html_wrap_inline198 log Ntex2html_wrap_inline362 6
   high Rb tex2html_wrap_inline198              8

Show diagram

Most stars have low Rb tex2html_wrap_inline198 log Ntex2html_wrap_inline372 tex2html_wrap_inline258C (tex2html_wrap_inline260 tex2html_wrap_inline188O is source of neutrons.





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Last update: July 10, 1999