We expand on the comprehensive study of hyperfine structure (HFS) in Mn II conducted by Holt et al. (1999) by verifying hyperfine magnetic dipole constants (A) for 20 levels previously measured by Holt et al. (1999) and deriving A constants for 47 previously unstudied levels. The HFS patterns were measured in archival spectra from Fourier transform (FT) spectrometers at Imperial College London and the National Institute of Standards and Technology. Analysis of the FT spectra was carried out in XGREMLIN. Our A constant for the ground level has a lower uncertainty by a factor of 6 than that of Blackwell-Whitehead et al.Key words: atomic data -line: profiles -methods: laboratory: atomic -techniques: spectroscopic.
I N T RO D U C T I O NThe cosmic abundance of manganese is 5.42 ± 0.04 1 (Scott et al. 2015), and is the fourth highest of the iron-group elements. However, much higher abundances of manganese are found in some chemically peculiar stars of late B spectral types. An example is given by the HgMn star HD 175640, in which the Mn abundance of 7.8 exceeds that of any element heavier than oxygen (Castelli & Hubrig 2004). The high abundance of manganese in this star gives rise to many lines of Mn II that are not seen in laboratory spectra (Castelli, Kurucz & Cowley 2015).Manganese has one stable isotope with a mass number of 55. The ground configuration of Mn II is 3d 5 ( 6 S)4s (Sansonetti & Martin 2005). Since manganese has a nuclear spin of 5/2 and a nuclear magnetic moment of 3.4687, spectral lines of Mn II show hyperfine structure (HFS). HFS is of importance in astronomy because it broadens the lines observed in stellar spectra, giving incorrect abundances if it is not taken into account and potentially confusing the line identification. Jomaron, Dworetsky & Allen (1999) showed that the chemical abundance of Mn II in HgMn stars can be overestimated by up to 3 orders of magnitude if HFS is neglected. Even if a rough estimate is made of the HFS pattern, the abundance can be overestimated by up to a factor of 4 in stars. other lines that exhibit broader HFS where the HFS constants for one or both levels are not known. For three notable lines in Castelli & Hubrig (2004) at 9407.0 Å, 9408.7 Å, and 9446.8 Å, the A constants for the upper levels, 3d 5 ( 6 S)4p z 5 P o 2,3,4 , were known but the lower levels, 3d 5 ( 4 P)4s b 5 D 2, 3 were not. The resulting synthetic spectra are a poor fit to the observed stellar spectrum. Hyperfine structure constants are also needed to obtain a more accurate value for the wavelength of a transition, particularly for close-lying levels where it may be difficult to distinguish between HFS and fine-structure components in the observed spectral lines, and second-order hyperfine mixing may be of importance.Previous work on the HFS of Mn II began with Villemoes et al. (1991) who used laser spectroscopy to measure HFS constants for the three levels of the 3d 5 ( 6 S)4p z 5 P o J term and 3d 5 ( 6 S)4s a 5 S 2 . Holt, Scholl & Rosner (1999) later expanded on this study by indepen...