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Fast magnetohydrodynamic oscillation of longitudinally inhomogeneous prominence threads: an analogue with quantum harmonic oscillator

机译:纵向非均匀的快速磁流体动力学振荡   突出线程:具有量子谐振子的模拟

摘要

Previous works indicate that the frequency ratio of second and firstharmonics of kink oscillations has tendency towards 3 in the case of prominencethreads. We aim to study the magnetohydrodynamic oscillations of longitudinallyinhomogeneous prominence threads and to shed light on the problem of frequencyratio. Classical Sturm--Liouville problem is used for the threads withlongitudinally inhomogeneous plasma density. We show that the spatial variationof total pressure perturbations along the thread is governed by the stationarySchr\"{o}dinger equation, where the longitudinal inhomogeneity of plasmadensity stands for the potential energy. Consequently, the equation has boundedsolutions in terms of Hermite polynomials. Boundary conditions at the threadsurface lead to transcendental dispersion equation with Bessel functions. Thinflux tube approximation of the dispersion equation shows that the frequency ofkink waves is proportional to the expression \alpha(2n+1), where \alpha is thedensity inhomogeneity parameter and n is the longitudinal mode number.Consequently, the ratio of the frequencies of second and first harmonics tendsto 3 in prominence threads. Numerical solution of the dispersion equation showsthat the ratio only slightly decreases for thicker tubes in the case of smallerlongitudinal inhomogeneity of external density, therefore the thin flux tubelimit is a good approximation for prominence oscillations. However, strongerlongitudinal inhomogeneity of external density may lead to the significantshift of frequency ratio for wider tubes and therefore the thin tubeapproximation may fail. The tendency of frequency ratio of second and firstharmonics towards 3 in prominence threads is explained by the analogy of theoscillations with quantum harmonic oscillator, where the density inhomogeneityof the threads plays a role of potential energy.
机译:先前的工作表明,在突出螺纹的情况下,扭结振荡的第二和第一谐波的频率比趋于3。我们旨在研究纵向不均匀突出线的磁流体动力学振荡,并阐明频率比的问题。经典Sturm-Liouville问题用于等离子密度纵向不均匀的螺纹。我们表明,沿螺纹的总压力扰动的空间变化由平稳的Schr \“ dinger方程控制,等离子体密度的纵向不均匀性代表势能。因此,该方程根据Hermite多项式具有有界解。螺纹表面处的条件导致具有Bessel函数的先验色散方程。色散方程的Thinflux管近似表明,扭结波的频率与表达式\ alpha(2n + 1)成比例,其中\ alpha是密度不均匀性参数,n是因此,突出螺纹中二次谐波和一次谐波的频率之比趋于3,色散方程的数值解表明,在外部密度纵向不均匀性较小的情况下,对于较厚的管子,该比率仅略有减小,因此较薄通量管极限是突出的良好近似振荡。但是,外部密度的纵向不均匀性越强,可能导致较宽的管的频率比发生明显偏移,因此细管的逼近可能会失败。通过与量子谐波振荡器的振荡类比,可以解释突出螺纹中第二和第一谐波的频率比趋于3的趋势,其中螺纹的密度不均匀性发挥势能的作用。

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