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  • Tian, Y. S., Li, X., Lu, G. P., Wang, Z. Y., Jiang, R. B., Nambalirwa, A., Zhu, B. Y., Qie, X. S., and Zhang Y. J. (2026). Examining charge transfer in an unusual rocket-triggered lightning flash with branched upward positive leaders. Earth Planet. Phys., 10(2), 1–12. DOI: 10.26464/epp2026018
    Citation: Tian, Y. S., Li, X., Lu, G. P., Wang, Z. Y., Jiang, R. B., Nambalirwa, A., Zhu, B. Y., Qie, X. S., and Zhang Y. J. (2026). Examining charge transfer in an unusual rocket-triggered lightning flash with branched upward positive leaders. Earth Planet. Phys., 10(2), 1–12. DOI: 10.26464/epp2026018
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Examining charge transfer in an unusual rocket-triggered lightning flash with branched upward positive leaders

  • We have examined an unusual rocket-triggered lightning flash during the summer campaign of the SHAndong Triggered Lightning Experiment (SHATLE) in 2018. High-speed video camera observations and three-dimensional (3D) lightning mapping show that the upward positive leader split into two branched channels (referred to as branch A & branch B, respectively) at a height of about 370 m, and then progressed into different charge regions of the thundercloud. Branch A initially developed upward before turning northwest from the trigger point; ten pronounced intermittent negative leaders were observed propagating downward along this branch channel, causing strong current pulses. Branch B propagated obliquely upward towards the northeast before continuing northward to a region of weak radar echo at 3 km altitude, resulting in a large-scale charge transfer of approximately –250 C (C = Coulomb) and generating a sustained, strong current exceeding 2 kA. Furthermore, downward dart leaders propagating along branch A connected to the active channel of branch B at the bifurcation point. This connection generated a surge of large current pulses (M-components) superimposed on the continuing current. Evidence from 3D lightning mapping and concurrent channel-base current measurements suggests that the 10th negative dart leader split during its downward propagation, with one branch propagating to ground, while the other entered into a positive charge reservoir. This initiated a positive charge transfer to ground via the existing channel, ultimately triggering the final stroke which exhibited a bi-polarity current pulse.
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