论文标题
从太阳能到Mira恒星:在存在随机噪声的情况下对恒星脉动器的统一描述
From Solar-like to Mira stars: a unifying description of stellar pulsators in the presence of stochastic noise
论文作者
论文摘要
我们讨论并表征了旨在描述从渐近巨型分支的主要序列中描述恒星脉动的模型的功率谱密度。我们表明,在存在随机噪声的情况下,脉冲模式的功率谱密度的预测极限总是通过洛伦兹功能很好地近似。虽然在恒星中主要是随机驱动的洛伦兹的宽度是由模式寿命定义的,而在恒星中,驱动驱动器主要是相干的,但宽度是由随机扰动的幅度定义的。在两个驱动器都是可比的恒星中,宽度都是由这两个参数定义的,并且比纯随机驾驶所期望的宽度要小。我们通过数值模拟说明了我们的模型,并提出了将恒星定义明确的分类,主要是随机(太阳样)和主要相干(经典)脉动器。我们将模型应用于MIRA变量U的研究,以及半剖变量L2 PUP,并在我们的分类之后得出结论,它们都是经典的脉动脉络膜。我们的模型为脉动振幅周期关系的行为变化提供了自然的解释,在几项早期作品中指出。此外,我们对L2 PUP的研究使我们能够测试模式线宽度和有效温度之间的缩放关系,证实指数级别的缩放量从主序列到渐近巨型分支一直很好地重现了数据,直到先前研究中已测试的内容约为1000 K的温度。
We discuss and characterise the power spectral density properties of a model aimed at describing pulsations in stars from the main-sequence to the asymptotic giant branch. We show that the predicted limit of the power spectral density for a pulsation mode in the presence of stochastic noise is always well approximated by a Lorentzian function. While in stars predominantly stochastically driven the width of the Lorentzian is defined by the mode lifetime, in stars where the driving is predominately coherent the width is defined by the amplitude of the stochastic perturbations. In stars where both drivings are comparable, the width is defined by both these parameters and is smaller than that expected from pure stochastic driving. We illustrate our model through numerical simulations and propose a well defined classification of stars into predominantly stochastic (solar-like) and predominately coherent (classic) pulsators. We apply the model to the study of the Mira variable U Per, and the semiregular variable L2 Pup and, following our classification, conclude that they are both classical pulsators. Our model provides a natural explanation for the change in behaviour of the pulsation amplitude-period relation noted in several earlier works. Moreover, our study of L2 Pup enables us to test the scaling relation between the mode line width and effective temperature, confirming that an exponential scaling reproduces well the data all the way from the main sequence to the asymptotic giant branch, down to temperatures about 1000 K below what has been tested in previous studies.