Spatial variability in the ratio of interstellar atomic deuterium to hydrogen. I. Observations toward delta Orionis by the interstellar medium absorption profile spectrograph
Eb. Jenkins et al., Spatial variability in the ratio of interstellar atomic deuterium to hydrogen. I. Observations toward delta Orionis by the interstellar medium absorption profile spectrograph, ASTROPHYS J, 520(1), 1999, pp. 182-195
Studies of the abundances of deuterium in different astrophysical sites are
of fundamental importance to answering the question about how much deuteri
um was produced during big bang nucleosynthesis and what fraction of it was
destroyed later. With this in mind, we used the Interstellar Medium Absorp
tion Profile Spectrograph (IMAPS) on the ORFEUS-SPAS II mission to observe
at a wavelength resolution of 4 km s(-1) (FWHM) the Ly delta and Ly epsilon
absorption features produced by interstellar atomic deuterium in the spect
rum of delta Ori A. A chi(2) analysis indicated that 0.96 < N(D I) < 1.45 x
10(15) cm(-2) at a 90% level of confidence, and the gas is at a temperatur
e of about 6000 K. In deriving these results, we created a template for the
velocity profile defined by seven different N I transitions recorded at a
high signal-to-noise ratio. Extra free parameters in the analysis allowed f
or the additional uncertainties that could arise from various sources of sy
stematic error. To derive a value for D/H, we measured the Ly alpha absorpt
ion features in 57 spectra of delta Ori in the IUE archive, with the object
ive of arriving at an H I column density more accurate than those reported
by other investigators. From our measurement of N(H I) = 1.56 x 10(20) cm(-
2), we found that N(D I)/N(H I) = 7.4(-1.3)(+1.9) x 10(-6) (90% confidence)
. Systematic errors in the derivation of N(H I) probably dominate over the
very small formal error, but their relative value should be smaller than th
at for N(D I). Our result for D/H contrasts with the more general finding a
long other lines of sight that D/H approximate to 1.5 x 10(-5). The underab
undance of D toward delta Ori A is not accompanied by an overabundance of N
or O relative to H, as one might expect if the gas were subjected to more
stellar processing than usual.