The abundance of Be in the lowest-metallicity stars is a probe of Big
Bang Nucleosynthesis, and its abundance in halo and disk stars is a pr
obe of galactic evolution and stellar structure. We present observatio
ns of the Be II resonance lines in 14 halo stars and 27 (mostly old) d
isk stars with [Fe/H] from - 2.7 to + 0.13. The spectra were obtained
at the Canada-France-Hawaii 3.6 m telescope and have a measured resolu
tion of 0.13 angstrom and a median signal-to-noise ratio of approximat
ely 50. For 18 of the 41 stars we have also made observations of the O
I triplet at the Palomar 5 m telescope, the UH 2.2 m telescope, and t
he CFH telescope. Stellar parameters of T(eff), log g, and [Fe/H] were
carefully determined from several independent estimates. Abundances a
re determined for log N(Be/H) and [O/H] from measured equivalent width
s, model parameters, and Kurucz (1991) model atmospheres with the RAI1
0 model atmosphere abundance program. The agreement with previously pu
blished Be detections is very good (a mean difference of 0.05 dex) for
five of six determinations in four halo stars and in four of five dis
k stars. Our typical internal error from uncertainities in the stellar
parameters and the S/N ratio of the observed spectra is 0.10 dex. The
agreement with very recently published O abundances is 0.07(5) dex. I
t is plausible, but far from conclusive, that there is a plateau in th
e amount of Be present in the lowest metallicity stars: log N(Be/H) ap
proximately - 12.8 for [Fe/H] < - 2.2. As [Fe/H] increases from - 2.2
to - 1.0, log N(Be/H) increases and the slope is 1.2-1.3, indicating a
faster increase in Be than in Fe. This is consistent with the product
ion of Be by spallation reactions between cosmic rays and 0 atoms from
massive stars and the production of Fe from intermediate mass stars.
The Be and Fe data can also be represented by N(Be) proportional to N(
Fe)2.0 as [Fe/H] goes from - 3.0 to - 2.0 and N(Be) proportional to N(
Fe)1.0 as [Fe/H] goes from - 2.0 to - 1.0. The disk stars ([Fe/H] = -
1.0 to 0.0) show a spread in Be of nearly an order of magnitude; part
of this must be real since the typical uncertainity is 0.10 dex. Evide
nce for stellar processing of Be exists in the disk stars and in at le
ast two of the halo stars. A plot of Be abundance vs 0 abundances show
s that Be increases as O1.12, indicating that Be is produced primarily
in the vicinity of supernovae envelopes, but a small and interesting
fraction is produced in the general interstellar gas in the halo.