On the probable interpretation of anticorrelation between the proton temperature and density in the solar wind

Dumin Yu.V., Lukashenko A.T., Svirskaya L.M.
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Abstract

The anticorrelated distributions of temperature and density of protons are a well-known property of the solar wind. Nevertheless, it is unclear till now if they are formed by some kind of the universal physical mechanism? Unfortunately, a straightforward comparison of the characteristic relaxation times for the temperature and density, on the one hand, and pressure, on the other hand, encounters the problem of inapplicability of the hydrodynamical approach in the situation when the free-path length of the protons is considerably greater than the spatial scale of the structures under consideration. To resolve this problem, some kinds of the MHD turbulence—reducing the effective free paths—are usually assumed. In the present paper, we use an alternative approach based on the electrostatic (Langmuir) turbulence, described by the mathematical formalism of the spin-type Hamiltonians, which was actively discussed in the recent time in the literature on statistical physics. As follows from the corresponding calculations, formation of the anticorrelated distributions of temperature and density is a universal property of the strongly nonequilibrium plasmas governed by the spintype Hamiltonians when they gradually approach the thermodynamic equilibrium. So, just this phenomenon could be responsible for the anticorrelations observed in the solar wind.
太阳风中质子温度与密度反相关关系的可能解释
温度和质子密度的反相关分布是太阳风的一个众所周知的特性。然而,到目前为止,我们还不清楚它们是否由某种普遍的物理机制形成。不幸的是,当质子的自由路径长度远远大于所考虑的结构的空间尺度时,直接比较温度和密度与压力的特征弛豫时间会遇到水动力方法不适用的问题。为了解决这一问题,通常假设几种MHD湍流减少了有效自由路径。在本文中,我们使用了一种基于静电(Langmuir)湍流的替代方法,该方法由自旋型哈密顿量的数学形式描述,这在最近的统计物理文献中得到了积极的讨论。由相应的计算可知,温度和密度反相关分布的形成是由自旋型哈密顿量控制的强非平衡等离子体在逐渐接近热力学平衡时的普遍特性。所以,这种现象可能是太阳风中观察到的反相关关系的原因。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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