Abstract:Context. According to most stellar dynamo theories, differential rotation (DR) plays a crucial role in the generation of toroidal magnetic fields. Numerical models predict surface differential rotation to be anti-solar for rapidly rotating giant stars, i.e. their surface angular velocity could increase with stellar latitude. However, surface differential rotation has been derived only for a handful of individual giant stars to date. Aims. The spotted surface of the K-giant KU Pegasi is investigated in order to… Show more
“…Still, other mechanisms could also be con-sidered to spin up the surface of an evolved star on the red giant branch. A certain fraction of red giants have undergone such spin up phases (e.g., Carlberg et al 2011;Ceillier et al 2017), which may involve mixing processes (Simon & Drake e.g., 1989, but see also Kriskovics et al 2014;Kővári et al 2017b), planet engulfment (Siess & Livio 1999;Kővári et al 2016), binary mergers (Webbink 1976;Strassmeier et al 1998) or other, less known mechanisms. However, the lack of systematic radial velocity measurements does not enable to know whether KIC 2852961 is a member of a wide binary system or rather a close binary.…”
Section: On the Stellar Evolution Rotation And Differential Rotationmentioning
Context. The most powerful superflares reaching 1039 erg bolometric energy are from giant stars. The mechanism behind flaring is thought to be the magnetic reconnection, which is closely related to magnetic activity (including starspots). However, it is poorly understood how the underlying magnetic dynamo works and how the flare activity is related to the stellar properties that eventually control the dynamo action.
Aims. We analyze the flaring activity of KIC 2852961, a late-type giant star, in order to understand how its flare statistics are related to those of other stars with flares and superflares, and to understand the role of the observed stellar properties in generating flares.
Methods. We searched for flares in the full Kepler dataset of KIC 2852961 using an automated technique together with visual inspection. We cross-matched the flare-like events detected by the two different approaches and set a final list of 59 verified flares during the observing term. We calculated flare energies for the sample and performed a statistical analysis.
Results. The stellar properties of KIC 2852961 are revised and a more consistent set of parameters are proposed. The cumulative flare energy distribution can be characterized by a broken power law; that is to say, on the log-log representation the distribution function is fitted by two linear functions with different slopes, depending on the energy range fitted. We find that the total flare energy integrated over a few rotation periods correlates with the average amplitude of the rotational modulation due to starspots.
Conclusions. Flares and superflares seem to be the result of the same physical mechanism at different energy levels, also implying that late-type stars in the main sequence and flaring giant stars have the same underlying physical process for emitting flares. There might be a scaling effect behind the generation of flares and superflares in the sense that the higher the magnetic activity, the higher the overall magnetic energy released by flares and/or superflares.
“…Still, other mechanisms could also be con-sidered to spin up the surface of an evolved star on the red giant branch. A certain fraction of red giants have undergone such spin up phases (e.g., Carlberg et al 2011;Ceillier et al 2017), which may involve mixing processes (Simon & Drake e.g., 1989, but see also Kriskovics et al 2014;Kővári et al 2017b), planet engulfment (Siess & Livio 1999;Kővári et al 2016), binary mergers (Webbink 1976;Strassmeier et al 1998) or other, less known mechanisms. However, the lack of systematic radial velocity measurements does not enable to know whether KIC 2852961 is a member of a wide binary system or rather a close binary.…”
Section: On the Stellar Evolution Rotation And Differential Rotationmentioning
Context. The most powerful superflares reaching 1039 erg bolometric energy are from giant stars. The mechanism behind flaring is thought to be the magnetic reconnection, which is closely related to magnetic activity (including starspots). However, it is poorly understood how the underlying magnetic dynamo works and how the flare activity is related to the stellar properties that eventually control the dynamo action.
Aims. We analyze the flaring activity of KIC 2852961, a late-type giant star, in order to understand how its flare statistics are related to those of other stars with flares and superflares, and to understand the role of the observed stellar properties in generating flares.
Methods. We searched for flares in the full Kepler dataset of KIC 2852961 using an automated technique together with visual inspection. We cross-matched the flare-like events detected by the two different approaches and set a final list of 59 verified flares during the observing term. We calculated flare energies for the sample and performed a statistical analysis.
Results. The stellar properties of KIC 2852961 are revised and a more consistent set of parameters are proposed. The cumulative flare energy distribution can be characterized by a broken power law; that is to say, on the log-log representation the distribution function is fitted by two linear functions with different slopes, depending on the energy range fitted. We find that the total flare energy integrated over a few rotation periods correlates with the average amplitude of the rotational modulation due to starspots.
Conclusions. Flares and superflares seem to be the result of the same physical mechanism at different energy levels, also implying that late-type stars in the main sequence and flaring giant stars have the same underlying physical process for emitting flares. There might be a scaling effect behind the generation of flares and superflares in the sense that the higher the magnetic activity, the higher the overall magnetic energy released by flares and/or superflares.
“…B05: Barnes (), BCL05: Barnes et al (), BJC04: Barnes et al (), DC97: Donati & Collier Cameron (), MWC05: Marsden et al (), DCP03: Donati et al (), PDV04 Petit et al (), KSG04: Kővári et al (), KWF09: Kővári et al (), KBH00: Korhonen et al (), PDO04: Petit et al (), VKS07: Vida et al (), HSK16: Harutyunyan et al (), KW04: Kővári & Weber (), KKO14: Kővári et al (), KKS13: Kővári et al (), KBS07: Kővári et al (), KKK12: Kővári et al (), KKV14: Kriskovics et al (), KKK15: Kővári et al (), WSW05: Weber et al (), ÖCK16: Özdarcan et al (), KKS16: Kővári et al (), MBD07: Marsden et al (), SKW03: Strassmeier et al (), KSO17: Kővári et al (), BVW86: Balthasar et al (), BJM16: Boro Saikia et al ().…”
Section: The Collected Observational Sampleunclassified
From our sample of spotted late-type stars showing surface differential rotation we find that the relationship between the rotation period and the surface shear coefficient α = ∆Ω/Ω eq is significantly different for single stars compared to members in close binaries. Single stars follow a general trend that α increases with the rotation period. However, differential rotation of stars in close binary systems shows much weaker dependence on the rotation, if any, suggesting that in such systems tidal forces operate as a controlling mechanism of differential rotation.
“…More reliable way of detecting differential rotation with its magnitude and type is Doppler imaging, which is based on high resolution time series spectroscopy. Considering other stars whose k values were determined by Doppler imaging, we see mostly weak differential rotation with a k value of a few percent, either among solar type differential rotators (HD 208472 k = 0.015 ( Özdarcan et al 2016), XX Tri k = 0.016 (Künstler et al 2015), ζ And k = 0.055 (Kővári et al 2012), KU Peg k = 0.04 (Kővári et al 2016)) or anti-solar type differential rotators (UZ Lib k = −0.004 (Vida et al 2007), σ Gem k = −0.04 (Kővári et al 2015), HU Vir k = −0.029 (Harutyunyan et al 2016)). Due to the binary nature of KIC 9451096, considerable effect of tidal forces on redistribution of the angular momentum in the convective envelope of the components can be expected, which would alter the magnitude of differential rotation (Scharlemann 1982).…”
We present spectroscopic and photometric analysis of KIC 9451096, where the latter is based on very high precision long cadence photometry obtained by Kepler space craft. Combined spectroscopic and photometric modeling show that the system is a detached eclipsing binary in a circular orbit and composed of F5V + K2V components. Subtracting the best-fit light curve model from whole long cadence data reveals additional low (mmag) amplitude light variation in time and occasional flares, suggesting low, but still remarkable level of magnetic spot activity on the K2V component. Analyzing rotational modulation of light curve residuals enables us to estimate differential rotation coefficient of the K2V component as k = 0.069 ± 0.008, which is 3 times weaker compared with the solar value of k = 0.19, assuming a solar type differential rotation. We find stellar flare activity frequency for K2V component as 0.000368411 h −1 indicating low magnetic activity level.
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