Journal
ASTROPHYSICAL JOURNAL
Volume 919, Issue 2, Pages -Publisher
IOP Publishing Ltd
DOI: 10.3847/1538-4357/ac1115
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Funding
- Gaia Multilateral Agreement
- National Development and Reform Commission
- Alfred P. Sloan Foundation
- National Aeronautics and Space Administration
- National Science Foundation
- U.S. Department of Energy
- Japanese Monbukagakusho
- Max Planck Society
- Astrophysical Research Consortium (ARC)
- University of Chicago
- Fermilab
- Institute for Advanced Study
- Japan Participation Group
- Johns Hopkins University, Los Alamos National Laboratory
- Max-Planck-Institute for Astronomy (MPIA)
- Max-PlanckInstitute for Astrophysics (MPA), New Mexico State University
- University of Pittsburgh
- Princeton University
- United States Naval Observatory
- University of Washington
- INAF (Istituto Nazionale di Astrofisica), Osservatorio Astronomico di Roma, ASI (Agenzia Spaziale Italiana) [INAF: ASI 2014-049-R.0]
- National Science Foundation [AST1714534]
- Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) [138713538 - SFB 881]
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The study of field RR Lyrae variables reveals a bimodal metallicity distribution, with RRab variables being more metal-rich than RRc variables. In the Bailey diagram, 80% of RRab variables are located along the short-period sequence, while 70% of RRc variables are along the long-period sequence. As metallicity increases, the pulsation period and visual amplitude of RR Lyrae variables steadily decrease.
We discuss the largest and most homogeneous spectroscopic data set of field RR Lyrae variables (RRLs) available to date. We estimated abundances using both high-resolution and low-resolution (Delta S method) spectra for fundamental (RRab) and first overtone (RRc) RRLs. The iron abundances for 7941 RRLs were supplemented with similar estimates that are available in the literature, ending up with 9015 RRLs (6150 RRab, 2865 RRc). The metallicity distribution shows a mean value of [Fe/H] = -1.51 +/- 0.01, and sigma(standard deviation) = 0.41 dex with a long metal-poor tail approaching [Fe/H] similar or equal to - 3 and a sharp metal-rich tail approaching solar iron abundance. The RRab variables are more metal-rich ([Fe/H](ab) = -1.48 +/- 0.01, sigma = 0.41 dex) than RRc variables ([Fe/H](c) = -1.58 +/- 0.01, sigma = 0.40 dex). The relative fraction of RRab variables in the Bailey diagram (visual amplitude versus period) located along the short-period (more metal-rich) and the long-period (more metal-poor) sequences are 80% and 20%, while RRc variables display an opposite trend, namely 30% and 70%, respectively. We found that the pulsation period of both RRab and RRc variables steadily decreases when moving from the metal-poor to the metal-rich regime. The visual amplitude shows the same trend, but RRc amplitudes are almost two times more sensitive than RRab amplitudes to metallicity. We also investigated the dependence of the population ratio (N- c /N-tot) of field RRLs on the metallicity and we found that the distribution is more complex than in globular clusters. The population ratio steadily increases from similar to 0.25 to similar to 0.36 in the metal-poor regime, it decreases from similar to 0.36 to similar to 0.18 for -1.8 <= [Fe/H] <= -0.9 and it increases to a value of similar to 0.3 approaching solar iron abundance.
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