1986
DOI: 10.1038/321290a0
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Observations of waves and plasma in the environment of comet Halley

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Cited by 82 publications
(32 citation statements)
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“…This assures the access to the crossing point with simple experimental techniques, such as Langmuir probes [34,35]. The situation may be slightly different for Tokamak (n 0 ∼ 10 14 cm −3 ) and solid-state (n 0 ∼ 10 18 cm −3 ) plasmas, for which we respectively estimate λ Ã ∼ 0.1 mm and λ Ã ∼ 1 μm, implying the use of more sophisticated spectroscopic techniques [36][37][38].…”
Section: Physical Review Lettersmentioning
confidence: 99%
“…This assures the access to the crossing point with simple experimental techniques, such as Langmuir probes [34,35]. The situation may be slightly different for Tokamak (n 0 ∼ 10 14 cm −3 ) and solid-state (n 0 ∼ 10 18 cm −3 ) plasmas, for which we respectively estimate λ Ã ∼ 0.1 mm and λ Ã ∼ 1 μm, implying the use of more sophisticated spectroscopic techniques [36][37][38].…”
Section: Physical Review Lettersmentioning
confidence: 99%
“…It may be stressed here that the present investigation may be useful for understanding the low-frequency electrostatic noise enhancement observed by the Vega and Giotto space probes [23] in the dust regions of Haley's comet and spoke-like structures revealed by the Voyager space mission [21] in Saturn's rings.…”
mentioning
confidence: 82%
“…Angelis et al [14] investigated the propagation of ion-acoustic waves in a dusty plasma, in which a spatial inhomogeneity is created by a distribution of immobile dust particles [22]. They [14] applied their results in interpreting the low frequency noise enhancement observed by the Vega and Giotto space probes in the dusty regions of Haley's comet [23].…”
mentioning
confidence: 99%
“…Section 4 summarizes the major findings of this paper. Figure 1 shows the locations of the APV-V sensors (Grard et al, 1989) and the IKS IR-camera (Arduine et al, 1983) on the Vega spacecraft. The quasistatic (dc) and wave (ac) electric fields are measured with a double probe antenna, made of two solid spheres (sensors P1 and P2), 10 cm in diameter, located at the tips of two 2-meter long booms and separated by a distance L = 11 m. The potential differences between the probes, V 12 = V 1 − V 2 , and between probe P2 and the spacecraft structure, V 2s = V 2 − V s , are sampled at intervals of 1 s and 4 s, respectively.…”
Section: Introductionmentioning
confidence: 99%
“…Probe L2 is biased at a fixed potential of +5V with respect to the spacecraft structure in order to detect fast fluctuations of the electron flux. The current response of probe L1 is measured while its potential is swept with a period of 32 s between −6V and +6V on Vega 1 and between −4V and +2V on Vega 2 (Grard et al, 1989).…”
Section: Introductionmentioning
confidence: 99%