Parker Solar Probe Observations of Magnetic Reconnection Exhausts in Quiescent Plasmas near the Sun

S. Eriksson, M. Swisdak, Alfred Mallet, O. Krupařová, R. Livi, Orlando Romeo, S. Bale, J. Kasper, D. Larson, M. Pulupa
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Abstract

Parker Solar Probe observations are analyzed for the presence of reconnection exhausts across current sheets (CSs) within R < 0.26 au during encounters 4–11. Exhausts are observed with nearly equal probability at all radial distances with a preference for quiescent Tp < 0.80 MK plasmas typical of a slow-wind regime. High Tp > 0.80 MK plasmas of a fast wind characterized by significant transverse fluctuations rarely support exhausts irrespective of the CS width. Exhaust observations demonstrate the presence of local temperature gradients across several CSs with a higher-Tp plasma on locally closed fields and a lower-Tp plasma on locally open field lines for an interchange-type reconnection. A CS geometry analysis directly supports the property that X-lines bisect the magnetic field rotation θ-angle, whether the fields and plasmas are asymmetric or not, to maximize reconnection rates and available magnetic energy. The CS normal width d cs distributions suggest that a multiscale reconnection process through nested layers of bifurcated CSs may be responsible for observed power-law distributions beyond the median d cs ∼ 1000 km with an exponential d cs distribution present for ion kinetic dissipation scales below this median. Magnetic field shear θ-angles are essentially identical at R < 0.26 and 1 au with medians at θ ∼ 55° near the Sun and θ ∼ 65° at 1 au. In contrast, the tangential flow shear distributions are different near and far from the Sun. A bimodal flow shear angle distribution is present near the Sun with strong shear flow magnitudes. This distribution is modified with radial distance toward a relatively flat distribution of weaker flow shear magnitudes.
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帕克太阳探测器对太阳附近静态等离子体中磁性再连接排气的观测
帕克太阳探测器(Parker Solar Probe)的观测结果分析了在遭遇 4-11 期间 R < 0.26 au 范围内电流片(CS)上是否存在重连接排气。在所有径向距离上观测到排气的概率几乎相等,但更倾向于 Tp < 0.80 MK 的静态等离子体,这是慢风机制的典型特征。快速风的高 Tp > 0.80 MK 等离子体具有显著的横向波动特征,无论 CS 宽度如何,都很少出现排气现象。排气观测结果表明,在几个CS上存在局部温度梯度,局部封闭场上的等离子体Tp较高,而局部开放场线上的等离子体Tp较低,这就是交换型再连接。CS 几何分析直接支持这样一个特性,即无论磁场和等离子体是否不对称,X 线都将磁场旋转 θ 角一分为二,以最大限度地提高再连接率和可用磁能。CS 法向宽度 d cs 分布表明,通过嵌套的分叉 CS 层的多尺度再连接过程可能是观测到的 d cs ∼ 1000 公里中位数以外的幂律分布的原因,而低于该中位数的离子动能耗散尺度则存在指数 d cs 分布。磁场剪切θ角在 R < 0.26 和 1 au 时基本相同,太阳附近的中值为θ ∼ 55°,1 au 时为θ ∼ 65°。相反,切向流切变分布在太阳附近和远处有所不同。太阳附近存在双峰流切变角分布,切变流幅度很大。这种分布随着径向距离的增加而改变,变成相对平坦的较弱流切变分布。
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Parker Solar Probe Observations of Magnetic Reconnection Exhausts in Quiescent Plasmas near the Sun Erratum: “Inferences from Surface Brightness Fluctuations of Zwicky 3146 via the Sunyaev–Zel’dovich Effect and X-Ray Observations” (2023, ApJ, 951, 41) Erratum: “On Stellar Evolution in a Neutrino Hertzsprung–Russell Diagram” (2020, ApJ, 893, 133) Three-dimensional Magnetohydrodynamic Simulations of Periodic Variations of Ganymede’s Footprint Observability of Substructures in the Planet-forming Disk in the (Sub)centimeter Wavelength with SKA and ngVLA
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