Temel Kavramlar
Stellar megaflares emit far more energy in the near-ultraviolet (NUV) spectrum than previously thought, challenging existing models and suggesting a need for revised understanding of particle acceleration and heating mechanisms in stellar atmospheres.
İstatistikler
The energy in the TESS bandpass for Flare Event 1 is 7.5 × 10^33 erg.
The peak luminosity of Flare Event 1 is 6.1 × 10^30 erg s^-1.
Flare Event 2 has an energy of approximately 10^35 erg in the TESS bandpass.
The peak luminosity in NUVA for Flare Event 2 is over a factor of 10 larger than the most luminous flare spectra from IUE/SWP.
The NUVB stellar flux (≈1.24 × 10^-14 erg cm^-2 s^-1 ˚A^-1) increased by a factor of more than 200 during the rise phase of Flare Event 2.
The peak luminosity of Flare Event 2 reached 8.8 × 10^31 erg s^-1.
Flare Event 2 is about 25 times more impulsive than Flare Event 1 in the TESS band.
The impulsiveness index is 2-2.3 times larger, and peak fluxes are approximately 1.4-1.5 times higher in NUVA during the two major peaks in Flare Event 1.
By the end of the HST observations of Flare Event 2, the peak flux in NUVA is a factor of approximately 1.7 larger than NUVB.
The power-law index, α, calculated for the entire impulsive phase light curve of Flare Event 1 is approximately 1.5.
The power-law index, α, calculated for the rise phase of Flare Event 2 is approximately 1.3.
Blackbody temperatures of approximately 9000-10,000 K were fit to the NUVB continua.
Blackbody temperatures for NUVA ranged from approximately 16,000 K to nearly 18,000 K.
A single-temperature fit to the ratio of the wavelength-averaged flux densities in the spectrum of Flare Event 2 yielded a blackbody color temperature of 14,790 ± 430 K.
The continuum fits comprise 97-99% of the wavelength-integrated fluxes within NUVA and NUVB.
The observed fluxes within NUVA and NUVB during Flare Event 2 are 6.1 and 2.6 times larger, respectively, than the extrapolation of a T = 10^4 K blackbody.
The inferred flare areas are approximately 2 × 10^19 cm^2 for the high-energy component and approximately 6.5 × 10^19 cm^2 for the low-energy component.
The total flare area is approximately 0.01 of the visible stellar hemisphere.
Alıntılar
"The composite NUV spectra are not well represented by a single blackbody that is commonly assumed in the literature."
"Rather, continuum flux rises toward shorter wavelengths into the FUV, and we calculate that an optical T = 10^4 K blackbody underestimates the short wavelength NUV flux by a factor of ≈6."
"We show that rising NUV continuum spectra can be reproduced by collisionally heating the lower atmosphere with beams of E ≳10 MeV protons or E ≳500 keV electrons and flux densities of 10^13 erg cm−2 s−1. These are much larger than canonical values describing accelerated particles in solar flares."