1997
DOI: 10.1023/a:1001192915841
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Cited by 13 publications
(15 citation statements)
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“…The reddening of the continuum in the gradual phase was suggested to be the result of the presence of two (or more) competing emission mechanisms, including a contribution from Hydrogen (Paschen continuum) recombination radiation. Other studies have similarly concluded from colorimetry that flare radiation consists of a combination of the hot blackbody emission and optically thin Balmer continuum recombination radiation, while speculating that the blackbody is short-lived and the Balmer continuum becomes more dominant in the gradual phase (Abdul-Aziz et al, 1995, see also Abranin et al (1997); Zhilyaev et al (2007)). A two-component model was first proposed using simultaneous colorimetry and spectra of dMe flares by Kunkel (1970) -see also Moffett & Bopp (1976) -who concluded that a single, isothermal (T e = 3000 − 30 000 K) optically thin hydrogen emission (bf+ff) model was too blue to explain the observed flare colors, nor could it account for the spread of colors among a sample of flares.…”
Section: Acknowledgmentsmentioning
confidence: 92%
See 1 more Smart Citation
“…The reddening of the continuum in the gradual phase was suggested to be the result of the presence of two (or more) competing emission mechanisms, including a contribution from Hydrogen (Paschen continuum) recombination radiation. Other studies have similarly concluded from colorimetry that flare radiation consists of a combination of the hot blackbody emission and optically thin Balmer continuum recombination radiation, while speculating that the blackbody is short-lived and the Balmer continuum becomes more dominant in the gradual phase (Abdul-Aziz et al, 1995, see also Abranin et al (1997); Zhilyaev et al (2007)). A two-component model was first proposed using simultaneous colorimetry and spectra of dMe flares by Kunkel (1970) -see also Moffett & Bopp (1976) -who concluded that a single, isothermal (T e = 3000 − 30 000 K) optically thin hydrogen emission (bf+ff) model was too blue to explain the observed flare colors, nor could it account for the spread of colors among a sample of flares.…”
Section: Acknowledgmentsmentioning
confidence: 92%
“…Self-consistent models that use realistic flare heating mechanisms typically result in a white-light continuum that is dominated by a strong Hydrogen recombination component (Hawley & Fisher, 1992). The sophisticated one-dimensional RHD models of Abbett & Hawley (1999) and Allred et al (2005Allred et al ( , 2006 used the RADYN code (Carlsson & Stein, 1994, 1995, 1997 to simulate flares on an M dwarf and on the Sun using moderate (10 10 ergs s −1 cm −2 , F10) and large (10 11 ergs s −1 cm −2 , F11) fluxes of mildly relativistic electrons injected at the top of a semi-circular flare loop. The RADYN models employ the thick-target formulae of Emslie (1978), Canfield (1983), and that describe how the nonthermal electron beam deposits energy throughout the atmosphere.…”
Section: Acknowledgmentsmentioning
confidence: 99%
“…However, it does provide the correct overall shape of the continuum and allows us to investigate the possible evolution of the flare temperature and area coverage. Other mechanisms have been tried by several authors, with marginal results (see, e.g., Abranin et al 1997). A description of the exact nature of the blue continuum emission, as well as the underlying physical mechanism that produces it, remains elusive.…”
Section: Continuum Emissionmentioning
confidence: 99%
“…Besides the exploration of the radio emission from wellknown objects such as Jupiter, Sun, and pulsars, the receiver can also be used for detecting and analyzing other radio sources, previously unexplored with ground-based instruments. Those include, for example, Saturn's lightning (Griessmeier et al 2008), flaring stars (Abranin et al 1997;Konovalenko et al 2008), the elusive radio emission from exoplanets (Weber et al 2007;Ryabov et al 2004b).…”
Section: Resultsmentioning
confidence: 99%