1971
DOI: 10.1007/bf00154290
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Measurements on the Lyman alpha corona

Abstract: As a result of a collaborative rocket experiment carried out during the solar eclipse on 7 March, 1970, measurements have been made of the brightness of Lyman a from the corona, at heights between 5 x 104 and 5 x 105 km above the limb. The emission is shown to occur primarily through the resonance scattering of chromospheric Lyman ~ from the residual neutral hydrogen in the corona. Both the absolute value and radial fall-off of the brightness agree well with calculations based on solar density models. The Lyma… Show more

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Cited by 99 publications
(52 citation statements)
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“…The emission of the coronal H I Lyα line is mainly due to two mechanisms: 1) collisional excitation by free electrons impact and 2) resonant scattering of chromospheric photons by neutral hydrogen atoms, with the first one accounting for only a small fraction of the total intensity of the radiative process (Gabriel 1971;Raymond et al 1997). Resonant scattering of the solar chromospheric light by neutral hydrogen atoms thus becomes the primary tool for studying the corona at 121.6 nm.…”
Section: Coronal H I Lyα Intensitymentioning
confidence: 99%
“…The emission of the coronal H I Lyα line is mainly due to two mechanisms: 1) collisional excitation by free electrons impact and 2) resonant scattering of chromospheric photons by neutral hydrogen atoms, with the first one accounting for only a small fraction of the total intensity of the radiative process (Gabriel 1971;Raymond et al 1997). Resonant scattering of the solar chromospheric light by neutral hydrogen atoms thus becomes the primary tool for studying the corona at 121.6 nm.…”
Section: Coronal H I Lyα Intensitymentioning
confidence: 99%
“…Comparing the predictions of (2) to the temperatures observed for explosive events, ≈(0.2-5) × 10 5 K (Dere 1994), consistency is obtained if pickup ions typically represent only a fraction ≈10 −2 -0.4 of the total plasma density. This seems reasonable based on equilibrium ionisation balance calculations for the chromosphere (Gabriel 1971;Fontenla et al 1990Fontenla et al , 1991Fontenla et al , 1993, which yield n w /n e ≈ 10 −2 -1 (Section 3.1). For EUV blinkers (Harrison 1997;Harrison et al 1999), with v flow 25 km s −1 , the predictions (2) and (8) yield T ⊥i ≈ 8 × 10 4 K and T e ≈ (3-10) × 10 4 K. These temperatures are very characteristic of the chromosphere and transition region, although as for explosive events, reweighting via (9) will reduce the predicted heating.…”
Section: Chromospheric and Transition Region Eventsmentioning
confidence: 75%
“…The recent development of a coronagraph capable of observing intensities and line profiles of ultraviolet resonance lines [9] represents an important step in our ability to interpret certain physical variables of the coronal medium. Indeed, : initial considerations and measurements [10,11,12] indicate that combined measurement of profiles and intensities in the ultraviolet and the intensity of Thorn son-scattered radiation in visible light can provide an important new tool for determining temperatures, densities, and flow velocities in solar coronal structures. The early instruments, however, are inevitably limited in their capabilities because of their small scale; this is the result of the small-scale occulting geometries available on ordinary space platforms.…”
Section: Coronagraphic Observationsmentioning
confidence: 99%