Spectral Anisotropy of Els\"asser Variables in Two Dimensional Wave-vector Space as Observed in the Fast Solar Wind Turbulence

TL;DR

This study investigates the spectral anisotropy of Els"asser variables in 2D wave-vector space within the fast solar wind, revealing distinct distribution patterns and energy dominance characteristics linked to Alfvénic fluctuations.

Contribution

It verifies the transformation between PSD and correlation functions and applies it to analyze Els"asser variables' anisotropy in solar wind turbulence, uncovering new distribution patterns and energy dynamics.

Findings

PSD$_{2D}$ spectra are mainly distributed along an inclined ridge toward $k_ot$

Residual energy is larger at small $k_ot$, indicating magnetic energy dominance

Els"asser ratio and residual energy distributions support Alfvén wave interaction simulations

Abstract

Intensive studies have been conducted to understand the anisotropy of solar wind turbulence. However, the anisotropy of Els\"asser variables ($\textbf{Z}^\pm$) in 2D wave-vector space has yet to be investigated. Here we first verify the transformation based on the projection-slice theorem between the power spectral density PSD$_{2D}(k_\parallel,k_\perp )$ and the spatial correlation function CF$_{2D} (r_\parallel,r_\perp )$. Based on the application of the transformation to the magnetic field and the particle measurements from the WIND spacecraft, we investigate the spectral anisotropy of Els\"asser variables ($\textbf{Z}^\pm$), and the distribution of residual energy E$_{R}$, Alfv\'en ratio R$_{A}$ and Els\"asser ratio R$_{E}$ in the $(k_\parallel,k_\perp)$ space. The spectra PSD$_{2D}(k_\parallel,k_\perp )$ of $\textbf{B}$, $\textbf{V}$, and $\textbf{Z}_{major}$ (the larger of $\textbf{Z}^\pm$) show a similar pattern that PSD$_{2D}(k_\parallel,k_\perp )$ is mainly distributed along a ridge inclined toward the $k_\perp$ axis. This is probably the signature of the oblique Alfv\'enic fluctuations propagating outwardly. Unlike those of $\textbf{B}$, $\textbf{V}$, and $\textbf{Z}_{major}$, the spectrum PSD$_{2D}(k_\parallel,k_\perp )$ of $\textbf{Z}_{minor}$ is distributed mainly along the $k_\perp$ axis. Close to the $k_\perp$ axis, $\left| {E}_{R}\right|$ becomes larger while R$_{A}$ becomes smaller, suggesting that the dominance of magnetic energy over kinetic energy becomes more significant at small $k_\parallel$. R$_{E}$ is larger at small $k_\parallel$, implying that PSD$_{2D}(k_\parallel,k_\perp )$ of $\textbf{Z}_{minor}$ is more concentrated along the $k_\perp$ direction as compared to that of $\textbf{Z}_{major}$. The residual energy condensate at small $k_\parallel$ is consistent with simulation results in which E$_{R}$ is spontaneously generated by Alfv\'en wave interaction.