Delayed Development of Cool Plasmas in X-ray Flares from kappa1 Ceti
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Date
2023-01-03
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This work was written as part of one of the author's official duties as an Employee of the United States Government and is therefore a work of the United States Government. In accordance with 17 U.S.C. 105, no copyright protection is available for such works under U.S. Law.
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Abstract
he Neutron star Interior Composition ExploreR (NICER) X-ray observatory observed two powerful
X-ray flares equivalent to superflares from the nearby young solar-like star, κ
1 Ceti, in 2019. NICER
follows each flare from the onset through the early decay, collecting over 30 cnts s−1 near the peak,
enabling a detailed spectral variation study of the flare rise. The flare in September varies quickly in
∼800 sec, while the flare in December has a few times longer timescale. In both flares, the hard band
(2−4 keV) light curves show typical stellar X-ray flare variations with a rapid rise and slow decay,
while the soft X-ray light curves, especially of the September flare, have prolonged flat peaks. The
time-resolved spectra require two temperature plasma components at kT ∼0.3−1 keV and ∼2−4 keV.
Both components vary similarly, but the cool component lags by ∼200 sec with a 4−6 times smaller
emission measure (EM) compared to the hot component. A comparison with hydrodynamic flare loop
simulations indicates that the cool component originates from X-ray plasma near the magnetic loop
footpoints, which mainly cools via thermal conduction. The time lag represents the travel time of the
evaporated gas through the entire flare loop. The cool component has several times smaller EM than
its simulated counterpart, suggesting a suppression of conductive cooling possibly by the expansion of
the loop cross-sectional area or turbulent fluctuations. The cool component’s time lag and small EM
ratio provide important constraints on the flare loop geometry.