Abstract
Magnetic reconnection is a fundamental process within highly conductive plasmas. Oppositely oriented field lines are reconfigured, releasing stored magnetic energy. It plays a vital role in shaping the dynamics of the solar corona and provides one of the main mechanisms for releasing the stored energy that powers solar eruptions. Reconnection at the Sun has been studied using remote-sensing observations, but the Parker Solar Probe (PSP) now permits in situ sampling of reconnection-related plasma in the corona. Here we report on a PSP fly-through of a reconnecting current sheet in the corona during a major solar eruption on 5–6 September 2022. We find that even 24 h after the flare peak, PSP detected the reconnection exhaust, indicating continuing fast reconnection, which we confirmed using remote-sensing observations made by the Solar Orbiter. This reconnection persisted much longer than typical timescales of a few minutes to hours. Plasma parameters measured by PSP within the reconnection region match numerical simulations. These new observations provide a key bridge between theory and measurements of plasmas in the solar atmosphere, laboratory experiments and astrophysical systems, generating new constraints required for the refinement of models and for the strengthening of their links to observations at many scales.
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Data availability
The PSP mission data used in this study are openly available at the CDAWeb of the NASA Space Physics Data Facility (https://cdaweb.gsfc.nasa.gov/). The SolO mission data are openly available in the ESA Solar Orbiter Archive (https://soar.esac.esa.int/soar/). The simulation data will be shared upon request to author X.X. (xiaoyan.xie@cfa.harvard.edu).
Code availability
The codes used for reducing and analysing the data are available as part of the SolarSoft library (https://www.lmsal.com/solarsoft/sswdb_description.html). The public version of the NIRVANA code is available on the GitLab repository (https://gitlab.aip.de/ziegler/NIRVANA). Python packages Astropy (v.5.1, https://github.com/astropy/astropy), Astrospice (v.0.2, now archived, https://github.com/astrospice/astrospice/tree/main/astrospice), Pyspedas (v.4.1.0, https://github.com/spedas/pyspedas), Matplotlib (v3.5.2, https://github.com/matplotlib/matplotlib) and Sunpy (v.5.0, https://github.com/sunpy/sunpy) were used in creating some of the figures.
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Acknowledgements
We thank T. G. Forbes, N. E. Raouafi and Z. Mei for helpful discussions while we carried out the analysis for this paper. This work originally developed during the team meetings of the Connect programme of NASA’s Heliophysics System Observatory: Energetics of solar eruptions from the chromosphere to the inner heliosphere project, supported by Grant No. 80NSSC20K1283. The WISPR, FIELDS and SWEAP suites were designed, developed and are operated under NASA contract NNN06AA01C. We acknowledge the extraordinary contributions of the PSP mission operations and spacecraft engineering team at the Johns Hopkins University Applied Physics Laboratory. The PSP was designed, built and is now operated by the Johns Hopkins University Applied Physics Laboratory as part of NASA’s Living with a Star programme (Contract No. NNN06AA01C). The EUI instrument was built by CSL, IAS, MPS, MSSL/UCL, PMOD/WRC, ROB, LCF/IO with funding from the Belgian Federal Science Policy Office (Grant Nos. BELSPO/PRODEX PEA 4000134088, 4000112292, 4000117262 and 4000134474); the Centre National d’Etudes Spatiales (CNES); the UK Space Agency; the Bundesministerium für Wirtschaft und Energie (BMWi) through the Deutsches Zentrum für Luft- und Raumfahrt (DLR); and the Swiss Space Office. The space mission SolO is the result of an international collaboration between ESA and NASA, and it is operated by ESA. The NIRVANA code was developed by U. Ziegler at the Leibniz Institute for Astrophysics Potsdam. We are grateful to the ESA SOC and MOC teams for their support. The German contribution to SO/PHI is funded by the BMWi through DLR and by MPG central funds. The Spanish contribution is funded by AEI/MCIN/10.13039/501100011033/ and the European Union Next Generation EU/PRTR (Grant Nos. RTI2018-096886-C5, PID2021-125325OB-C5, PCI2022-135009-2 and PCI2022-135029-2) and ERDF – A way of making Europe; Center of Excellence Severo Ochoa awards to IAA-CSIC (SEV-2017-0709, CEX2021-001131-S); and a Ramón y Cajal fellowship awarded to D.O.S. The French contribution is funded by CNES. R.P., D.B.S., M.J.W., K.K.R., S.R., X.X. and T.N. were supported by the Connect programme of NASA’s Heliophysics System Observatory (Grant No. 80NSSC20K1283). S.T.B. and Y.J.R. were supported by the PSP project through the SAO/SWEAP (Subcontract No. 975569). G.S. was supported by WISPR Phase-E funds. P.H. is funded by the Office of Naval Research. This project has received funding from the European Research Council under the European Union’s Horizon 2020 research and innovation programme (Grant Agreement No. 101097844 for project WINSUN).
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Contributions
R.P. led the work, carried out the analysis of the remote-sensing data and led the preparation of the paper. T.N. carried out the analysis of PSP in situ data. X.X. carried out the numerical simulation and provided its results. D.B.S. contributed towards the interpretation of the data, models and results and worked on improving the figures. S.T.B. performed the ballistic projection of the magnetogram data. S.R. interpreted the flare energetics. Y.J.R. helped interpretation of in situ signatures and results. K.K.R. interpreted the data, models and results. G.S. processed the WISPR data and provided its outputs. P.H. and M.J.W. helped in interpreting the WISPR and EUI data, respectively. A.F., J.H., D.O.S., S.K.S., H.S. and G.V. processed and provided SO/PHI data. All authors participated in discussing the results and writing the draft.
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Extended data
Extended Data Fig. 1 Additional plasma parameters based on PSP measurements.
(a) PSP in situ measurement of BR on 6 September 2022 from 17:25 to 17:45 UT, the time period used for generating PSP data plots in Fig. 4, right panel, shown in red for consistency with Figs. 3 and 4. Derived parameters in panels (b - e) are Alfvén speed (VA), total pressure (PTOTAL), proton plasma beta (ß) and Alfvén Mach number (MA) respectively during this period. The vertical dashed line at 17:35 UT is the same reference time as in Fig. 3.
Extended Data Fig. 2 Schematic of the September 5, 2022 CME.
The dimensions are not to scale and have been exaggerated to visualize the extent of the CME, current sheet and PSP orbit plane in the context of the CME source region. Even though the source region (shown with the red-blue pair of filled circles) is in the southern hemisphere, the CME is wide enough that PSP crosses its associated current sheet. The light blue triangle shows the part of the current sheet lying above the plane along the vector radial to the source region, whereas the magenta region is below that plane. The black arrow at the top of the sphere and the solid black curve near the center represent the solar north pole and equator, respectively. The gray shaded region bound by a dashed line shows PSP’s orbit plane. Note that in the real scenario, the active region is more complex (Fig. 3b), and the flare loops arcade shows inclined orientation as shown in Fig. 2. For simplicity, here we only show a portion of the complicated arcade system, which should not be confused with the loops orientation seen in EUI images. Further, the flux rope structure has traveled well out into interplanetary space.
Extended Data Fig. 3 Spatial distributions and parameter profiles from the 2.5D magnetohydrodynamic models.
The left panel shows a snapshot of the distributions of density (color shading) and magnetic field (solid curves) at 1641 s. Reference coordinates in R and T direction with respect to PSP are shown in the top left corner of this panel. Magnetic field, speed, density, temperature and current density as a function of distance are plotted from left to right panels along inclined cuts marked with black arrows at different heights for comparison. Note that the distance in these panels from 0 to 20 Mm in the horizontal axis corresponds to x = 10 Mm to x = -10 Mm in the left panel, that is from right to left along the black arrow. The same is applicable to the right panel based on PSP measurements, where the time axis is converted to distance.
Supplementary information
Supplementary Video 1
Imaging observation from 12:00 ut on 5 September 2022 to 23:14 ut on 6 September 2022 by the WISPR-I telescope of PSP. Snapshots of this video at various timestamps are shown in Fig. 1.
Supplementary Video 2
The evolution of the active region of interest. The left panel shows SO/PHI observations that are related to Fig. 3b. The middle and right panels show FSI observations of the same region at 174 and 304 Å, respectively. Stills from these two panels are shown in Fig. 2b,c and 2e,f, respectively.
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Patel, R., Niembro, T., Xie, X. et al. Direct in situ observations of eruption-associated magnetic reconnection in the solar corona. Nat Astron 9, 1444–1454 (2025). https://doi.org/10.1038/s41550-025-02623-6
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DOI: https://doi.org/10.1038/s41550-025-02623-6


