Abstract
Turbulent magnetic reconnection is believed to occur in astrophysical plasmas, and it has been suggested to be a trigger of solar flares. It often occurs in long stretched and fragmented current sheets. Recent observations by the Parker Solar Probe, the Solar Dynamics Observatory and in situ satellite missions agree with signatures expected from turbulent reconnection. However, the underlying mechanisms, including how magnetic energy stored in the Sun’s magnetic field is dissipated, remain unclear. Here we demonstrate turbulent magnetic reconnection in laser-generated plasmas created when irradiating solid targets. Turbulence is generated by strongly driven magnetic reconnection, which fragments the current sheet, and we also observe the formation of multiple magnetic islands and flux-tubes. Our findings reproduce key features of solar flare observations. Supported by kinetic simulations, we reveal the mechanism underlying the electron acceleration in turbulent magnetic reconnection, which is dominated by the parallel electric field, whereas the betatron mechanism plays a cooling role and Fermi acceleration is negligible. As the conditions in our laboratory experiments are scalable to those of astrophysical plasmas, our results are applicable to the study of solar flares.
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Data availability
All data needed to evaluate the conclusions in the paper are present in the paper. Experimental data and simulations are available from the corresponding author upon reasonable request.
Code availability
The EPOCH code is used under UK EPSRC contracts (nos. EP/G055165/1 and EP/G056803/1).
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Acknowledgements
We acknowledge the Shenguang II staff for operating the laser facility, and the staff at CAEP for providing some diagnostics and target fabrication. We also thank H. Yan from Universitat Potsdam, J. Lin from YAOC and Q.M. Lu from the University of Science and Technology of China for valuable discussions. This work was supported by the National Key RD Program of China (grant nos. 2022YFA1603200 and 2022YFA1603203) and the National Natural Science Foundation of China (grant nos. 12175018, 12135001, U1930108, 12075030 and 11903006) and the Strategic Priority Research Program of the Chinese Academy of Sciences (grant no. XDA25030700).
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Contributions
J. Zhong proposed the experiment. The experiments were carried out by B.H., W.S., C.X., J.W. and Z.L. The data were analysed by Y.P., J. Zhong, X.W. and Z.Z. The interference data were measured and analysed by J. Zhong, Y.Z. and D.Y. Numerical simulations were performed by Y.P. and H.Z. Additional theoretical support was provided by Y.L. and B.Q. Y.P., J. Zhong, X.W. and Y.L. contributed to writing of the manuscript. J. Zhu is responsible for running the laser facility. J. Zhang and G.Z. are the proposers and principal investigators of the laboratory astrophysics project.
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Extended data
Extended Data Fig. 1 Interferometric image analysis.
a and b, the interferograms in Case I with ds = 200μm and Case II with ds = 400μm respectively, for 1ns after lasers irradiation on the targets, and the bright spots are the laser irradiation positions, where the localised fringe shifts are presented and some darker zones break the fringe which imply the chaotic plasma density. c and d, the electron number density ne normalized by 1018cm−3 from the interferograms (a,b) are performed Abel inversion algorithm. Here, because the fringe is discontinuous, the inversion error is relatively large, especially in the fringe fracture area.
Extended Data Fig. 2 Measurement of magnetic field.
a, the evolution of the magnetic field probed by B-dot located 45mm from the center of the target in Case III where only one side part of target is irradiated by two lases corresponding two spots of the separation distance 400μm.
Extended Data Fig. 3 2D PIC simulation in Case I of the separation 20di.
The up row, the evolution of the magnetic field along X-direction Bx. The middle row, the evolution of the magnetic field along Y-direction By. The Unit of magnetic field is Tesla. The down row, the evolution of the electron number density ne which is normalized by 1024m−3. Here, ωci = eB0/mi is the ion gyro-frequency, and di is the ion inertial scale di = c/ωpi where \({\omega }_{pi}=\sqrt{4\pi {n}_{i}{e}^{2}/{m}_{i}}\), e is the element charge and mi is the ion mass with mi = 100me.
Extended Data Fig. 4 3D PIC simulations.
a and b, magnetic field along Y-direction By and electron number density in Case II where the magnetic and density tube are presented in the current sheet during MR. Here, the Bmax is about 189T and the unit of the electron number density is m−3. c, electron energy spectra in the current sheet which show non-thermal distributions and more energetic electrons in Case II than Case I. d, ion energy spectra in the current sheet and they are Maxwell distributions. dN/dE is the electron/ion energy distribution function.
Supplementary information
Supplementary Video 1
The electron number density evolution from 2D PIC simulation of Case I. Four density bubbles are generated as the lasers turned on, then expanded to form two dense sheaths, and eventually fragmented in the current sheet region.
Supplementary Video 2
The x-component evolution of the magnetic field, Bx versus t, by 2D PIC simulation of Case I. Four bubbles of Bx are created as the lasers turned on, and then expanded to form anti-parallel magnetic field regions. Eventually magnetic islands are generated due to reconnection.
Supplementary Video 3
The y-component evolution of the magnetic field, By versus t, by 2D PIC simulation of Case I. Four bubbles with By in opposite directions are created as the lasers turned on, and expanded. Then the adjacent By on the same side annihilates to form fine magnetic structures where By reconnects to generate islands in the current sheet region.
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Ping, Y., Zhong, J., Wang, X. et al. Turbulent magnetic reconnection generated by intense lasers. Nat. Phys. 19, 263–270 (2023). https://doi.org/10.1038/s41567-022-01855-x
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DOI: https://doi.org/10.1038/s41567-022-01855-x
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