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Ultra-Wideband, Multi-epoch Radio Study of the First Discovered `Main sequence Radio Pulse emitter' CU Vir

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arxiv 2107.00849 v1 pith:Z4YSMC37 submitted 2021-07-02 astro-ph.SR

classification astro-ph.SR
keywords ecmeradiostarfirstmagneticcircularlydiscovereddiscovery
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abstract

Presence of large-scale surface magnetic field in early-type stars leads to several unique electromagnetic phenomena producing radiation over X-ray to radio bands. Among them, the rarest type of emission is electron cyclotron maser emission (ECME) observed as periodic, circularly polarized radio pulses. The phenomenon was first discovered in the hot magnetic star CU Vir. Past observations of this star led to the consensus that the star produces only right circularly polarized ECME, suggesting that only one magnetic hemisphere takes part in the phenomenon. Here we present the first ultra-wideband (0.4$-$4 GHz) study of this star using the upgraded Giant Metrewave Radio telescope and the Karl G. Jansky Very Large Array, which led to the surprising discovery of ECME of both circular polarizations up to around 1.5 GHz. The GHz observations also allowed us to infer that the upper ECME cut-off frequency is at $\gtrsim 5\,\mathrm{GHz}$. The sub-GHz observation led to the unexpected observation of more than two pairs of ECME pulses per rotation cycle. In addition, we report the discovery of a `giant pulse', and transient enhancements, which are potentially the first observational evidence of `centrifugal breakout' of plasma from the innermost part of the stellar magnetosphere. The stark contrast between the star's behavior at GHz and sub-GHz frequencies could either be due to propagation effects, a manifestation of varying magnetic field topology as a function of height, or a signature of an additional `ECME engine'.

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  1. First monitoring campaign of a Main-sequence Radio Pulse emitter: the case of CU Vir

    astro-ph.SR 2026-08 conditional novelty 7.0 of 10

    A six-month, 36-epoch radio campaign on CU Vir shows the leading pulse fluctuates more than the trailing pulse, reveals arrival-phase jitter, and refines the rotation period to 0.5206882 days.

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