论文标题
太阳径向p-Modes的速度强度不对称逆转
Velocity-intensity asymmetry reversal of solar radial p-modes
论文作者
论文摘要
太空传教任务的发展显着提高了类似太阳能样振荡器光谱的质量。现在可以解决他们的$ p $ mode线配置文件,并且除了太阳以外的各种恒星所推断出的不对称。然而,很长一段时间以来,太阳能$ p $模型的不对称性在速度和强度光谱之间逆转。为了使用不对称性作为地震诊断的工具,必须了解这种逆转的起源。对于太阳以外的其他恒星,只有强度功率谱就足够解决了,以估算不对称的模式。我们最近开发了一种方法,旨在在太阳的速度功率谱中建模和预测这些不对称性,并成功地将它们与观察得出的对应物进行比较。在本文中,我们扩展了模型,并预测强度功率谱中特征的不对称性。我们发现,强度的模式线轮廓的形状在很大程度上取决于如何处理辐射通量的振荡诱导的变化,并且对其进行现实建模对于理解不对称反转至关重要。扰动太阳能校准的灰色大气模型,并采用准绝热框架作为第一步,我们重现了在太阳强度光谱中观察到的低频模式中观察到的不对称性。我们得出的结论是,与以前的思想不同,没有必要引起额外的机制(例如非绝热效应,连贯的非谐波背景信号)来解释不对称逆转。但是,需要这种附加机制来解释高阶模式的不对称逆转。
The development of space-borne missions has significantly improved the quality of the measured spectra of solar-like oscillators. Their $p$-mode line profiles can now be resolved, and the asymmetries inferred for a variety of stars other than the Sun. However, it has been known for a long time that the asymmetries of solar $p$-modes are reversed between the velocity and the intensity spectra. Understanding the origin of this reversal is necessary in order to use asymmetries as a tool for seismic diagnosis. For stars other than the Sun, only the intensity power spectrum is sufficiently resolved to allow for an estimation of mode asymmetries. We recently developed an approach designed to model and predict these asymmetries in the velocity power spectrum of the Sun and to successfully compare them to their observationally derived counterparts. In this paper we expand our model and predict the asymmetries featured in the intensity power spectrum. We find that the shape of the mode line profiles in intensity is largely dependent on how the oscillation-induced variations of the radiative flux are treated, and that modelling it realistically is crucial to understanding asymmetry reversal. Perturbing a solar-calibrated grey atmosphere model, and adopting the quasi-adiabatic framework as a first step, we reproduce the asymmetries observed in the solar intensity spectrum for low-frequency modes. We conclude that, unlike previously thought, it is not necessary to invoke an additional mechanism (e.g. non-adiabatic effects, coherent non-resonant background signal) to explain asymmetry reversal. This additional mechanism is necessary, however, to explain asymmetry reversal for higher-order modes.