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INVESTIGATION OF THE ZEEMAN EFFECT IN THE e ⁶Π −a ⁶∆ SYSTEM OF FeH: APPLICATION TO STELLAR SPECTROSCOPY
Ross, Amanda J.
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https://hdl.handle.net/2142/122395
Description
- Title
- INVESTIGATION OF THE ZEEMAN EFFECT IN THE e ⁶Π −a ⁶∆ SYSTEM OF FeH: APPLICATION TO STELLAR SPECTROSCOPY
- Author(s)
- Ross, Amanda J.
- Contributor(s)
- Tokaryk, Dennis W.
- Blackmore, Timothy E
- Adam, Allan G.
- Crozet, Patrick
- Issue Date
- 2023-06-20
- Keyword(s)
- Small molecules
- Abstract
- We investigate the Zeeman effect in the e ⁶Π − a ⁶∆ system of FeH. The molecule has been produced by reaction of Fe(CO)₅ with H atoms, and examined by laser excitation with selective detection and by Fourier transform resolved fluorescence. The field-free spectrum of the e ⁶Π − a ⁶∆ system was extensively studied by the J.M. Brown group and collaborators in the 1990’s ᵃ. Their analysis located the low-lying excited a ⁶∆ state 1890 cm−¹ above the X ⁴∆ electronic ground state. One of the infrared systems of FeH already recognisedᵇ in the spectra of cool stars around 1.6 µm, E ⁴Π − A ⁴Π, originates in an excited state lying only 920 cm−¹ lower in energy in energy than a ⁶∆, so it seemed not unreasonable to expect signatures from the known sextet systems e−a and g−a to appear in the spectra of cool stars as well. We found that the e − a system can indeed be used as a diagnostic for FeH. Cross-correlation functions between a mask of laboratory-measured e − a transitions and spectra from four M- dwarf stars taken on spectropolarimetric instruments ESPaDOnS (on Maunakea) and Narval (in the French Pyrenees), show that reliable radial-velocity information can be extracted for these objects. Our new Zeeman measurements are intended to improve reference data for cross-correlation calculations for M-type stars, whose magnetic fields are typically 0 − 5000 Gauss.
- Publisher
- International Symposium on Molecular Spectroscopy
- Type of Resource
- Text
- Language
- eng
- Handle URL
- https://hdl.handle.net/2142/122395
- DOI
- https://doi.org/10.15278/isms.2023.6950
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