Abstract:One Titanian year spans over two complete solar cycles, and the solar irradiance has a significant effect on ionospheric densities. Solar cycle 24 has been one of the quietest cycles on record. In this paper we show data from the Cassini ion and neutral mass spectrometer (INMS) and the radio and plasma wave science Langmuir probe spanning the time period from early 2005, at the declining phase of solar cycle 23, to late 2015 at the declining phase of solar cycle 24. Densities of different ion species measured … Show more
“…Hence, we conclude that the plasma environment was significantly compressed during the impact, due to the increased solar wind dynamic pressure. This is in agreement with the background magnetic field strength increasing by a factor of about 2-3, which would then explain the increased suprathermal electron fluxes as an effect of adiabatic compression (Madanian et al 2016).…”
We present Rosetta observations from comet 67P/Churyumov-Gerasimenko during the impact of a coronal mass ejection (CME). The CME impacted on 5-6 Oct 2015, when Rosetta was about 800 km from the comet nucleus, and 1.4 AU from the Sun. Upon impact, the plasma environment is compressed to the level that solar wind ions, not seen a few days earlier when at 1500 km, now reach Rosetta. In response to the compression, the flux of suprathermal electrons increases by a factor of 5-10 and the background magnetic field strength increases by a factor of ∼2.5. The plasma density increases by a factor of 10 and reaches 600 cm −3 , due to increased particle impact ionisation, charge exchange and the adiabatic compression of the plasma environment. We also observe unprecedentedly large magnetic field spikes at 800 km, reaching above 200 nT, which are interpreted as magnetic flux ropes. We suggest that these could possibly be formed by magnetic reconnection processes in the coma as the magnetic field across the CME changes polarity, or as a consequence of strong shears causing Kelvin-Helmholtz instabilities in the plasma flow. Due to the limited orbit of Rosetta, we are not able to observe if a tail disconnection occurs during the CME impact, which could be expected based on previous remote observations of other CME-comet interactions.
“…Hence, we conclude that the plasma environment was significantly compressed during the impact, due to the increased solar wind dynamic pressure. This is in agreement with the background magnetic field strength increasing by a factor of about 2-3, which would then explain the increased suprathermal electron fluxes as an effect of adiabatic compression (Madanian et al 2016).…”
We present Rosetta observations from comet 67P/Churyumov-Gerasimenko during the impact of a coronal mass ejection (CME). The CME impacted on 5-6 Oct 2015, when Rosetta was about 800 km from the comet nucleus, and 1.4 AU from the Sun. Upon impact, the plasma environment is compressed to the level that solar wind ions, not seen a few days earlier when at 1500 km, now reach Rosetta. In response to the compression, the flux of suprathermal electrons increases by a factor of 5-10 and the background magnetic field strength increases by a factor of ∼2.5. The plasma density increases by a factor of 10 and reaches 600 cm −3 , due to increased particle impact ionisation, charge exchange and the adiabatic compression of the plasma environment. We also observe unprecedentedly large magnetic field spikes at 800 km, reaching above 200 nT, which are interpreted as magnetic flux ropes. We suggest that these could possibly be formed by magnetic reconnection processes in the coma as the magnetic field across the CME changes polarity, or as a consequence of strong shears causing Kelvin-Helmholtz instabilities in the plasma flow. Due to the limited orbit of Rosetta, we are not able to observe if a tail disconnection occurs during the CME impact, which could be expected based on previous remote observations of other CME-comet interactions.
“…It should also be noted that the nightside EUV trends are clear both with the median normalization and SLT detrending, although the error margins are much greater in the latter case. Interestingly, both peak and max n + and n À correlate with F EUV on the dayside, a factor ≈2 (≈4000 cm À3 ) increases between minimum and maximum solar activity (similar enhancements have also been observed by the Cassini INMS for positive ions <100 amu [Madanian et al, 2016]). At the same time, the charge densities strongly anticorrelate with F EUV on the nightside of Titan, a factor ≈3-4 (≈3000-4000 cm À3 ) Figure 6.…”
Section: Solar Cycle Dependenciessupporting
confidence: 61%
“…It should also be noted that the nightside EUV trends are clear both with the median normalization and SLT detrending, although the error margins are much greater in the latter case. Interestingly, both peak and max n + and n − correlate with F EUV on the dayside, a factor ≈2 (≈4000 cm −3 ) increases between minimum and maximum solar activity (similar enhancements have also been observed by the Cassini INMS for positive ions <100 amu [ Madanian et al , ]). At the same time, the charge densities strongly anticorrelate with F EUV on the nightside of Titan, a factor ≈3–4 (≈3000–4000 cm −3 ) decrease (Figures d and e; fit coefficients are summarized in Table ), and despite the fact that there are no measurements of nightside for high F EUV (≳ 40 μW m −2 , see Figures d and e) that cover the altitudes <1200 km, the trends of both n + and n − are consistent (as expected due to the coupled ion‐ion reactions [ Shebanits et al , ]).…”
Section: Resultsmentioning
confidence: 53%
“…The ionizing solar EUV flux evidently plays a key role in the complex organic chemistry of Titan's dayside ionosphere as the main source of energy. Recent research revealed the influence of the solar cycle on Titan's ionosphere, showing that electron [ Edberg et al , ] and positive ion number densities for lighter species (<100 amu) [ Madanian et al , ] are enhanced during the solar maximum, including the ions not directly produced by the ionizing EUV flux. Moreover, Sagnières et al [] showed that the ion number densities correlate with the local ionization rate, although the correlation is significantly stronger for the short‐lived ions than for the long‐lived ones.…”
Effects of solar EUV on positive ions and heavy negative charge carriers (molecular ions, aerosol, and/or dust) in Titan's ionosphere are studied over the course of almost 12 years, including 78 flybys below 1400 km altitude between TA (October 2004) and T120 (June 2016). The Radio and Plasma Wave Science/Langmuir Probe‐measured ion charge densities (normalized by the solar zenith angle) show statistically significant variations with respect to the solar EUV flux. Dayside charge densities increase by a factor of ≈2 from solar minimum to maximum, while nightside charge densities are found to anticorrelate with the EUV flux and decrease by a factor of ≈3–4. The overall EUV dependence of the ion charge densities suggest inapplicability of the idealized Chapman theory below 1200 km in Titan's ionosphere. Nightside charge densities are also found to vary along Titan's orbit, with higher values in the sunward magnetosphere of Saturn compared to the magnetotail.
“…The structure and variability of this ionosphere are sensitive to several factors. On the dayside of the moon, the ionosphere is created mainly through photoionization by extreme ultraviolet (EUV) radiation of the atmospheric N 2 and CH 4 (Ågren et al, ; Galand et al, ), which means that Titan's ionospheric properties will vary with the solar rotation and the phase of the solar cycle (Edberg et al, ; Madanian et al, ; Shebanits et al, ). Particle impact ionization also contributes and is the main ionization source on the nightside of the moon (Ågren et al, ; Cravens et al, , ; Vigren et al, ).…”
We report on unusual dynamics in Titan's ionosphere as a significant difference in ionospheric electron density is observed between the T118 and T119 Cassini nightside flybys. Two distinct nightside electron density peaks were present during T118, at 1,150 and 1,200 km, and the lowest density ever observed in Titan's ionosphere at altitudes 1,000–1,350 km was during T118. These flybys were quite similar in geometry, Saturn local time, neutral density, extreme ultraviolet flux, and ambient magnetic field conditions. Despite this, the Radio and Plasma Waves/Langmuir Probe measured a density difference up to a factor of 6 between the passes. The overall difference was present and similar during both inbound and outbound legs. By ruling out other factors, we suggest that an exceptionally low rate of particle impact ionization in combination with dynamics in the ionosphere is the explanation for the observations.
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