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Does the solar oxygen abundance change over the solar cycle?: An investigation into activity-induced variations in the O I infrared triplet

2026-01-24

The determination of the solar oxygen abundance remains a central problem in astrophysics, as its accuracy is limited not only by models but also by systematics. While many of these factors have been thoroughly characterized, the effect of the solar activity cycle has so far remained unexplored. Due to its relative strength and accessibility, the O I infrared triplet is typically the primary choice for abundance studies. However, previous investigations have shown that abundances inferred from this triplet tend to be higher than expected on active stars, whereas such an overabundance effect is not observed for the much weaker forbidden O I 6300 Å line. This raises the question of whether a similar trend can be found for the Sun. To address this question, we analyze two decades’ worth of synoptic disk-integrated Sun-as-a-star datasets from the FEROS, HARPS-N, PEPSI, and NEID spectrographs, focusing on the infrared triplet (7772, 7774, 7775 Å) and the forbidden O I 6300 Å line. The excellent signal-to-noise ratio of the PEPSI observations allows us to detect a weak but significant variation in the equivalent widths of the infrared triplet, corresponding to about 0.01 dex difference in abundance between activity minimum and maximum. This value is significantly smaller than the typical uncertainties on the solar oxygen abundance. Due to higher scatter, no comparable trend is found in the other data sets. Based on these results, we conclude that within the typical uncertainties presented in other works, we can assume the inferred solar oxygen abundance to be stable across the solar cycle, but that this effect may be significant for other, more active stars.

Measured EW of the O I 7772 Å line with FEROS (blue), PEPSI (orange), and NEID (green), including corresponding uncertainties. The gray curve shows the sunspot number as an activity reference, while the black horizontal line at 50 distinguishes active from quiet times.

Read more: Pietrow et al. 2026, A&A, 706, L11


Surface image and activity-corrected orbit of the RSCVn binary HR7275: Disentangling activity tracers

2026-01-07

Quantifying stellar parameters and magnetic activity for cool stars in double-lined spectroscopic binaries (SB2) is not straightforward, as both stars contribute to the observed composite spectra and are likely variable. Disentangled component spectra allow a detailed analysis of a component’s magnetic activity. We aim at separating the spectra of the two stellar components of the HR7275 SB2 system. Our further aim is a more accurate orbital solution by cleaning the observed radial velocities (RV) from activity perturbations of the spotted primary (“RV jitter”) and obtain a surface image of this component. We provide time-series high- and ultra-high resolution optical spectra and apply two different disentangling methods. RV residuals are modeled with three-sine function fits. The primary’s spectral-line profiles are modeled with the Doppler imaging code iMAP. Magnetic fields are measured for the primary based on least-square deconvolved Stokes-V line profiles. Chromospheric emission is determined from the line-cores of Ca II H&K, Ca II IRT 8542 Å, and Balmer Hα. Before applying those analyses, we provide a disentangling technique to determine the system properties more accurately. The Doppler image of the primary shows two large cool spots of size ≈20% of the visible hemisphere plus three smaller spots, each still ≈13% in size. In total, HR7275a exhibited an impressive spottedness of ≈40% of its entire surface in May-June 2022. The RV is modulated by the rotation of the primary with maximum amplitudes of 320 ms−1 and 650 ms−1 for two different modulation behaviors during the 250 d of our observations. This jitter is primarily caused by the varying asymmetries of the apparent disk brightness due to the cool spots. Its removal resulted in roughly ten times higher precision of the orbital elements. Our snapshot magnetic-field measurements reveal phase dependent (large-scale) surface fields between +0.6±2.0G at phase 0.1 and −15.2±2.7G at phase 0.6, indicating a complex magnetic morphology related to the location of the photospheric spots. We also obtain a logarithmic lithium abundance of 0.58±0.1 for HR7275a, indicating considerable mixing, and 0.16 for HR7275b, which is an extremely low value.

Spectral disentangling by median subtraction. Panel a: The mean spectrum of the secondary star is plotted as a black line (top). The composite spectrum (blue) and a spectrum of the primary star (red) are plotted with a vertical shift of 0.15 at orbital phase 0.82. Panel b: Time series composite spectra phase folded with the orbital period.

Read more: Adebali et al. 2026, A&A, 706, A179


Untangling the Sources of Abundance Dispersion in Low-metallicity Stars. II. Neutron Capture Elements

2026-01-06

We present the abundances of 23 elements, including 11 heavy elements (Cu, Zn, Sr, Y, Zr, Ba, La, Ce, Nd, Sm, Eu) for up to 86 metal-poor (−2 ≲ [Fe/H] ≲ −1) subgiants. We use KORG, a state of the art spectral synthesis package, to derive 1D-LTE abundances from high-SNR and high-resolution spectra taken by the Large Binocular Telescope with the Potsdam Echelle Polarimetric and Spectroscopic Instrument. These precise spectra and abundance measurements minimize the impact of photon-noise (≲ 0.06 dex), allowing us to robustly measure the intrinsic abundance scatter in [X/Fe]. After removing two stars with exceptional s-process enhancement, we find that the intrinsic scatter among the s- and r-process elements tends to be larger than for the lighter elements, with heavy element scatter ranging from 0.11 (Zn) to 0.27 (Eu) dex. Intrinsic abundance scatter could have multiple origins, including starto-star variations in the ratios of nucleosynthetic sources as well as stochastic sampling of the progenitor supernovae properties, such as mass, rotation, and magnetic field strength. We explore the expected abundance scatter signature caused by stochastic sampling, finding that a fraction of both rapidly rotating CCSN and magnetorotationally driven SN are needed to reach the observed abundances and intrinsic scatter. This analysis is limited by the restrictive parameter spaces spanned by existing yield sets. A diverse, finely sampled grid of supernovae yields is needed to robustly model stochastic abundance scatter.

Heavy element line windows for three stars with [Fe/H] of −2.12 (green, 2MASS J04315411-0632100), −1.58 (blue, 2MASS J15581861+0203059), and −1.04 (purple, 2MASS J17140534+1407170). Spectra have been offset by 0.1 for clarity. We show one window for each heavy element, with line centers labeled, including blended lines for Zr and Eu.

Read more: Griffith et al. 2026, ApJ, 1001, 193


Elemental abundance pattern and temperature inversion on the dayside of HAT-P-70b observed with CARMENES and PEPSI

2026-01-05

We observed the dayside thermal emission spectrum of UHJ HAT-P-70b using the high-resolution spectrographs CARMENES and PEPSI. Through our cross-correlation analysis, we detected emission signals for Al I, AlH, Ca II, Cr I, Fe I, Fe II, Mg I, Mn I, and Ti I, marking the first detection of Al I and AlH in an exoplanetary atmosphere. Tentative signals of C I, Ca I, Na I, NaH, and Ni I were also identified. Based on those detections, we were able to perform atmospheric retrievals to constrain the thermal profile and elemental abundances of the planet’s dayside hemisphere. The retrieved temperature-pressure profile reveals a strong temperature inversion layer. The chemical free retrieval yielded a metallicity of [Fe/H] = 0.38, while the chemical equilibrium retrieval resulted in [Fe/H] = 0.23, with both values consistent with the solar metallicity. We also tentatively found an enriched abundance of Ni, which could result from the accretion of Ni-rich planetesimals during the planet’s formation.

Ca II triplet emission lines observed with PEPSI. They were combined over two nights and shifted to the planetary rest frame using the best-fit velocity from the Ca II CCF signal. The dashed blue lines indicate the expected positions of the Ca II triplet lines. Among them, only the lines near 8500.36 Å and 8664.52 Å (vacuum wavelengths) were detected, with their Gaussian fits in red.

Read more: Guo et al. 2026, A&A, 706, A126


Surface activity of a Rossby number sequence of cool Hyades stars

2025-11-27

We present quantitative surface-activity information for a sequence of 21 Hyades dwarf stars with effective temperatures all cooler than the red edge of the lithium dip and Rossby (Ro) numbers between 0.14 to 0.54 with respect to the Sun (Ro(Sun)=1). High-resolution high-S/N PEPSI Stokes-IV spectra and least-squares deconvolution of thousands of spectral lines per spectrum are employed for measuring surface magnetic fields, rotational velocities, lithium abundances, and chromospheric CaII IRT fluxes. Lithium abundances A(Li) range from 95 times solar on the warm end of the sample to 1/25 solar on the cool end. We confirm the tight relation with T(eff) and extent it to K-M stars. A formal relation with rotational period and velocity in the sense higher A(Li) for faster rotators is present. Targets rotating faster than vsini of 6 km/s appear Li saturated. CaII IRT fluxes also show a relation with T(eff), P(rot) and vsini, but opposite to A(Li), in an inverse sense with higher radiative losses for the slower=cooler rotators. Disk-integrated, unsigned, magnetic-field strengths of 15.4±3.6(rms)G are measured for targets warmer than 5000K and 91±61(rms)G for targets cooler than this. These field strengths relate to P(rot), vsini, and Ro, but in a bi-modal fashion. We conclude that the Rossby-number dependency of the surface activity tracers on our Hyades dwarf sequence primarily originates from convective motions, expressed by its turnover time, and only to a smaller and sometimes inverse extent from surface rotation and its related extra mixing.

Lithium-activity-rotation relation versus normalized Rossby number (Ro_n). From left to right: A(Li) logarithmic lithium abundance, R‘(IRT) logarithmic radiative loss in the three CaII infrared-triplet lines, <|B|> disk-integrated, unsigned magnetic field strength in Gauss.

Read more: Strassmeier et al. 2025, A&A, 704, A8