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arXiv 1912.03608physics.space-phastro-ph.SR
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Clustering of Intermittent Magnetic and Flow Structures near Parker Solar Probe's First Perihelion -- A Partial-Variance-of-Increments Analysis

Rohit Chhiber, M. Goldstein, B. Maruca, A. Chasapis, W. Matthaeus, D. Ruffolo, R. Bandyopadhyay, T. Parashar, R. Qudsi, T. Dudok de Wit, S. Bale, J. Bonnell, K.… 展开作者

Rohit Chhiber, M. Goldstein, B. Maruca, A. Chasapis, W. Matthaeus, D. Ruffolo, R. Bandyopadhyay, T. Parashar, R. Qudsi, T. Dudok de Wit, S. Bale, J. Bonnell, K. Goetz, P. Harvey, R. MacDowall, D. Malaspina, M. Pulupa, J. Kasper, K. Korreck, A. Case, M. Stevens, P. Whittlesey, D. Larson, R. Livi, M. Velli, N. Raouafi

英文摘要:

During the Parker Solar Probe's (PSP) first perihelion pass, the spacecraft reached within a heliocentric distance of \(\sim 37~R_\odot\) and observed numerous magnetic and flow structures characterized by sharp gradients. To better understand these intermittent structures in the young solar wind, an important property to examine is their degree of correlation in time and space. To this end, we use the well-tested Partial Variance of Increments (PVI) technique to identify intermittent events in FIELDS and SWEAP observations of magnetic and proton-velocity fields (respectively) during PSP's first solar encounter, when the spacecraft was within 0.25 au from the Sun. We then examine distributions of waiting times between events with varying separation and PVI thresholds. We find power-law distributions for waiting times shorter than a characteristic scale comparable to the correlation time, suggesting a high degree of correlation that may originate in a clustering process. Waiting times longer than this characteristic time are better described by an exponential, suggesting a random memory-less Poisson process at play. These findings are consistent with near-Earth observations of solar wind turbulence. The present study complements the one by Dudok de Wit et al. (2020, present volume), which focuses on waiting times between observed "switchbacks" in the radial magnetic field.

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