2015
DOI: 10.1051/0004-6361/201425139
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Composition of inner-source heavy pickup ions at 1 AU: SOHO/CELIAS/CTOF observations

Abstract: Context. Pickup ions in the inner heliosphere mainly originate in two sources, one interstellar and one in the inner solar system. In contrast to the interstellar source that is comparatively well understood, the nature of the inner source has not been clearly identified. Former results obtained with the Solar Wind Ion Composition Spectrometer on-board the Ulysses spacecraft revealed that the composition of inner-source pickup ions is similar, but not equal, to the elemental solar-wind composition. These obser… Show more

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Cited by 16 publications
(15 citation statements)
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“…However, we know from observations of inner-source pickup ions heavier than helium that the inner source of pickup ions is dominant at relative velocities w sw < 0.5 . Because the composition of the inner source resembles the composition of the solar wind (Allegrini et al 2005;Gloeckler et al 2000;Taut et al 2015) and the inner-source pickup ion flux is correlated to the flux of the corresponding element in the solar wind , the seed population of inner-source pickup ions is likely the solar wind.…”
Section: The Asymmetry Of the He + Ring Beammentioning
confidence: 99%
“…However, we know from observations of inner-source pickup ions heavier than helium that the inner source of pickup ions is dominant at relative velocities w sw < 0.5 . Because the composition of the inner source resembles the composition of the solar wind (Allegrini et al 2005;Gloeckler et al 2000;Taut et al 2015) and the inner-source pickup ion flux is correlated to the flux of the corresponding element in the solar wind , the seed population of inner-source pickup ions is likely the solar wind.…”
Section: The Asymmetry Of the He + Ring Beammentioning
confidence: 99%
“…The model, I(m/q), was adapted from Taut et al (2015), where it was used to derive the composition of inner-source pickup ions with the charge and timeof-flight (CTOF) instrument on board the SOlar Heliospheric Observatory (SOHO; Hovestadt et al 1995). Because of the very similar measurement principle of CTOF and PLASTIC, choosing the mass-per-charge model from Taut et al (2015), which considers the asymmetry of the mass-per-charge model for an individual species, over a more simple, symmetric model (Drews et al 2010) or a simple mass-per-charge filter (Drews et al 2012), is most likely the best approach to deconvolve the contributions of individual species from the heavy pickup ion m/qspectra. The model I(m/q) of an individual species, which is a combined Gaussian-κ-function, is given by…”
Section: Discussionmentioning
confidence: 99%
“…Of course, the aforementioned parameters for the m/qmodel depend on the ion species, which further complicates a precise determination of I(m/q). Contrary to the analysis by Taut et al (2015), who derived these parameters via a simulation of the time-of-flight characteristic of CTOF, we use a more direct approach via an in-flight observation, in which the m/q-spectra were significantly dominated by either C + , O + , or Ne + . First of all, a time period between day of year (DoY) since 2007 between 127.3 < DoY < 127.5 was chosen to obtain a m/q-spectrum in which, almost exclusively, O + from the Earth's magnetosphere was observed with PLASTIC on STEREO A (Fig.…”
Section: Discussionmentioning
confidence: 99%
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“…Surprisingly, the data, with one exception of Venus tail ray O + observations (Grünwaldt et al 1997), has never been used to study inner source PUIs, although CTOFs active phase coincides with the discovery of the inner source. In this work and a companion paper (Taut et al 2015) we investigate inner source PUIs using CTOF data. Here, we address the short-term variability of inner source O + and C + while the companion paper adresses the composition of the inner source.…”
Section: Introductionmentioning
confidence: 99%