2019
DOI: 10.3847/1538-4357/ab48ec
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Coronae of Zero/Low-metal, Low-mass Stars

Abstract: Recent theoretical studies suggest the existence of low-mass zero-metal stars in the current universe. In order to study the basic properties of the atmosphere of low-mass first stars, we perform one dimensional magnetohydrodynamical simulations for the heating of coronal loops on low-mass stars with various metallicities. While the simulated loops are heated up to ≥ 10 6 K by the dissipation of Alfvénic waves originating from the convective motion irrespectively of the metallicity, the coronal properties sens… Show more

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Cited by 12 publications
(23 citation statements)
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“…We note that the dependence of 𝜏 cool on 𝑇 is different for different temperature ranges; for 𝑇 > 10 6 K, Λ ∝ 𝑇 1/2 so that 𝜏 cool ∝ 𝑇 1/2 𝜌 −1 . On the other hand, for 𝑇 < 10 6 K, Λ ∝ 𝑇 −1 in the case of zero metallicity (Sutherland & Dopita 1993;Washinoue & Suzuki 2019) and thus 𝜏 cool ∝ 𝑇 2 𝜌 −1 . For both temperature ranges, 𝜏 cool increases with temperature so that the gas should be thermally unstable (Balbus 1995).…”
Section: Time Evolution Of the Loop Profilesmentioning
confidence: 99%
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“…We note that the dependence of 𝜏 cool on 𝑇 is different for different temperature ranges; for 𝑇 > 10 6 K, Λ ∝ 𝑇 1/2 so that 𝜏 cool ∝ 𝑇 1/2 𝜌 −1 . On the other hand, for 𝑇 < 10 6 K, Λ ∝ 𝑇 −1 in the case of zero metallicity (Sutherland & Dopita 1993;Washinoue & Suzuki 2019) and thus 𝜏 cool ∝ 𝑇 2 𝜌 −1 . For both temperature ranges, 𝜏 cool increases with temperature so that the gas should be thermally unstable (Balbus 1995).…”
Section: Time Evolution Of the Loop Profilesmentioning
confidence: 99%
“…The loop model and simulations are basically similar to those in Washinoue & Suzuki (2019); we consider a single magnetic flux tube that is anchored at the photosphere and take the coordinate 𝑠 along the loop. We inject velocity perturbations 𝛿𝑣 in three directions from the footpoints to excite MHD waves.…”
Section: Settingsmentioning
confidence: 99%
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“…As noted in Table 1, the coordinate along the axis of the flux tube is denoted by s. Spatial variation only along the loop is assumed to be nonzero, that is, ∂/∂s 0. Similar one-dimensional flux tube models are used in the models of solar spicules (Hollweg et al 1982;Kudoh & Shibata 1999;Matsumoto & Shibata 2010), solar and stellar coronal heating (Moriyasu et al 2004;Washinoue & Suzuki 2019), and solar wind acceleration (Suzuki & Inutsuka 2005;Shoda et al 2018).…”
Section: Model Of the Closed Flux Tubementioning
confidence: 99%
“…Whether our theoretical predictions apply to lowermass stars (M dwarfs in particular) needs to be investigated in future. In light of lower metallicity found in old M-type stars, the metallicity dependence of the XUV emission needs to be studied as well (Washinoue & Suzuki 2019). According to the Figure 14 of Johnstone et al (2021), a single power law between L X and L EUV is applicable to low-mass stars with various spectral types, and thus, it is possible that Eq.…”
Section: Extension To Other Types Of Starsmentioning
confidence: 99%