Transcript 02-880-6627

Topics in Astronomical Spectroscopy : Evolution of
Chemical Abundances based on the High Resolution
Stellar Spectroscopy
2010, 1 학기 대학원
이상각
19동 317
02-880-6627
[email protected]
Aims :
• Evolution of Chemical Abundances based on the
High Resolution Stellar spectroscopy is the
subtitle of this course
• and aims to cover the recent developments of
the understanding of chemical evolution of the
cosmos as a whole, as well as that of the Galaxy.
• This leads into the outline of the recent studies
of the high resolution stellar spectroscopy for
investigation of the history of matter
• from the Big Bang to the present,
• based on the Big Bang Nucleosysthesis,
Supernovae and Stellar Nucleosynthesis.
References
• The recent papers on the subject of evolution of chemical
abundances for each class discussion will be announced in
the class bulletin board.
• There is no text book for this course.
• However the following reference books may be useful.
• Nucleosynthesis and Chemical Evolition of Galaxies, 2nd
Edition, B. J. Pagel, 2009 Cambridge,
• Supernovae and Nucleosynthesis , D. Arnett, 1996,
Princeton
• An Introduction to Cosmochemistry, C. Cowley, 1995,
Cambridge
Credits
• The classes will be mainly the round table
discussing seminar.
• All enrolled students have to present the
review of an assigned paper and conduct
the class by leading discussion with other
students and report his or her review in
written form.
• It will be graded for 45% of the course
credit.
• Mid & final exam : 50%
class attendance : 5%
Basic topics
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I. Big Bang Nucleosythesis
II. Early Universe
III. Pop III Stars, First Stars
IV. Metal-Poor Stars
V. Milky Way
VI. Galaxies
VII. n-processes
VIII. Stellar Nucleosythesis
IX. Sne : SNe II, PISNe, SN Ia
a) the large abundances of H and He;
b) the deep “hole” coresponding to Li/Be/B;
c) a series of peaks, particularly prominent for the α nuclei, corresponding to the
products of stellar burning between mass 12 and mass ∼ 40;
d) a mass peak near Fe, A ∼ 56-60;
e) rare heavier elements, but with mass peaks near A ∼ 130 and A ∼ 195.
Cosmic Abundance
Five groups of elements
• 1. The dominant elements : H & He
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by mass : 1H ∼ 0.75, 4He ∼ 0.25
•  primarily to nuclear and weak interaction processes occuring in
the first few minutes after the big bang
• 2. the lighter “1p-shell” nuclei (He < < C) : relatively rare, lower by 810 orders of magnitudes
• 6Li ∼ 7.75E-10 7Li ∼ 1.13e-8
• 9Be ∼ 3.13E-10 10B ∼ 5.22E-10 11B ∼ 2.30E-9
can be produced in the Big Bang. Li, Be, and B can also be
produced in the interstellar medium, when energetic cosmic-ray
protons collide with elements like C, N, and O.
• Li, Be, and B can also be synthesized by core-collapse supernovae,
directly by the interactions of neutrinos in the carbon shells of such
stars.
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7Li
The evolution of galactic Li as a function of
metallicity
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Li abundance plateau – called the Spite
plateau – at low metallicity, indicating
that some baseline of Li existed when
the first stars were formed. This is
assumed to be the primordial value.
Note the great spread of values for
stars of solar metallicity. The two circles
correspond to the expected standard
solar model Li (the high value) and the
measured Li. The sun managed to
destroy mosts of its Li – most likely by
dredging Li to depth (to high
temperatures, where it can be burned) –
during some past epoch.
Also shown are various theoretical
mechanisms proposed for synthesizing
Li.
From Ryan et al., astro-ph/9905211/.
Li
α -stable elements
• 3. α -stable elements C, N, O, Ne, Mg, Si, a
multiple of 4He, (N,Z)=(2,2).
•  An important property of the nuclear
force is pairing: nucleons are fermions with
spin ½. The α-stable nuclei are more tightly
bound than their neighbors with broken
pairs.  thermodynamically-favored
products of nuclear burning
14N ∼ 0.94E-3
• 12C ∼ 3.87E-3
• 16O ∼ 8.55E-3 20Ne ∼ 1.34E-3
• 24Mg ∼ 0.58E-3 28Si ∼ 0.75E-3
Iron group and n-processes
elements
• 4. peak near iron-group nuclei:
Elements near Fe and Ni have the largest binding
energy/nucleon.
•  the last possible products of a sequence of fusion
reactions
• 5. heavy elements, A ∼> 100
• Many of these elements are very rare, but a function of A
or N shows interesting patterns – several abundance peaks.
each peak is actually a double peak, with the two
components split by ∼ 10 mass units.
•  (n,γ) reactions : weak neutron sources, extremly high
neutron densites.
Binding Energy
Nuclear transformation
Neutron and proton capture
detailed view of solar system heavy element
abundances : From Truran et al., astro-ph/0209308
how are the differences in abundances
among these groups explained?
• wide variety of nucleosynthetic
signatures : analysis and interpretation of
the chemical signatures and enrichment
histories revealed by stellar spectra
Imprints in spectra
• Top : a) carbon star X Cancri
with 12C/13C ~4 from Hburning by the CNO cycle and
enhanced Zr
• b) peculair C star HD137613
without 13C and H-deficient c)
C star HD52432 with 12C/13C
~4
• Middle; a) normal C star
HD156074 showing CH and Hg
b) peculiar(H-poor) C star
HD182040 showing C2 but
weak Hg
• bottom: a) normal F b) HD
19445 metal-poor star
Imprints in spectra
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a) normal G
b) BaII starHD 46407
c) M giant 56 Leo showing TiO
d) S type AGB, R And showing Zr
• Bottom : c) Tc in R And which
indicate s-process and dredge-up
within a few half-lives of Tc 99 (2*
105 yr)
Cosmic Chemical Evolution