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RFI (man-made, lightning spherics) Auroral Kilometric Radiation. Sky background ... Saturn/Titan interaction ( other satellites ?) SW influence, substorms ? ... – PowerPoint PPT presentation

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Title: Pr


1
Planets and Solar System Science at Low
Frequencies Philippe Zarka LESIA,
CNRS-Observatoire de Paris France philippe.zarka_at_o
bspm.fr Towards a European Infrastructure for
Lunar Observatories Bremen, 22-23/3/2005 - EADS /
ASTRON / Radionet
2
  • Limitations of ground-based LF radioastronomy 
  •  RFI (man-made, lightning spherics)
  • Ionospheric cutoff (10 MHz)
  • propagation effects (30 MHz)
  • Sky background (fluctuations)
  •  IP, IS scintillations
  • (Solar radio emissions)

3
  • Limitations of LF radioastronomy in Earth
    orbit 
  •  RFI (man-made, lightning spherics)
  • Auroral Kilometric Radiation
  • Sky background (fluctuations)
  •  IP, IS scintillations
  • (Solar radio emissions)

4
  • Solar emission/ burst/storm
  • Spherics
  • LF Earth environment
  • AKR day/night (at 60 RE)
  • Thermal noise (?flux)
  • Galactic background
  • Ionospheric LF cutoff
  • Solar wind LF cutoff

5
  • Galactic background for a short dipole antenna,
    i.e. with ?8?/3, A3?2/8?
  • Antenna effective area
  • A k?2 with k 3/8? 1/8 for a short dipole,
  • k N/8 for N dipoles
  • A ? ?2 ? ? 1/k 8/N
  • LOFAR 104 dipoles

6
  • Jovian radio emissions (near opposition)
  • Solar wind / magnetosphere interaction (auroral
    emissions)
  • Io/magnetosphere interaction
  • Io torus
  • Synchrotron from radiation belts (HF)

7
Radiosources in Jupiter's environment
8
(No Transcript)
9
Io-Jupiter plasma interaction
10
  • Saturn, Uranus, Neptune auroral emissions

Saturn Uranus Neptune
11
  • Saturn, Uranus atmospheric lightning

Saturn Uranus
12
(No Transcript)
13
  • Detectability from the ground (Earth)
  • In absence of solar bursts spherics
  • In absence of RFI / after successful mitigation
  •  10-20 MHz
  • ? Jovian DAM with C(?dipole/?)?(b?)1/2N(b?)1/2
    100
  • (ex  N1, 10 kHz ? 1 sec)
  • ? Saturns lightning with C 105 (N200, 10 MHz
    ? 25 msec),
  • without access to LF cutoff

C 102 104 106
14
  • Moon
  • Shielding of RFI, spherics, AKR, Solar emissions
  • Only limitation to sensitivity sky background
  • fluctuations
  • Ionospheric LF cutoff ltlt500 kHz

15
  • Detectability from the Moon
  • ? all Jovian emissions Saturn auroral
    emissions with C 100-1000
  • (N1-10, 10 kHz ? 1 sec)
  • ? Uranus Neptune auroral emissions
  • Saturn Uranus lightning (including LF
    cutoff) with C 104 (N10-100, 200 kHz ? 50-500
    msec)

C 102 104 106
16
  • Long-term magnetospheric radio observations
  • ( multi-? correlations)

17
  • Variabilities/periodicities
  • ? magnetospheric dynamics
  • (role of SW, planetary rotation, satellite
    interactions, Io volcanism, short-lived bursts,
    substorms ?)
  • ? planetary rotation period
  • ? B anomalies secular variations
  • ? Io torus probing (nKOMFaraday effect)
  • ? SW monitoring from 1 to 30 AU

18
  • Saturn/Titan interaction (other satellites ?)
  • SW influence, substorms ?
  • Uranus Neptune auroral emissions observed only
    once by Voyager 2 !
  • Lightning long-term monitoring, correlation
    with optical observations, planetary comparative
    meteorology

19
  • Extrasolar Jupiter-like radio emissions at 10 pc
    range
  • Flux up to ? 105 Jupiters strength for
    magnetized hot Jupiters with solar-like stellar
    wind input, or unmagnetized hot Jupiters in
    interaction with strongly magnetized star
  • possible stronger stellar wind, focussing
    events,

C 103 105 107 109
105 103 10 1
20
Magnetic Radio Bode's Law


21
  • Detectability from the ground (Earth)
  • No solar bursts /spherics , RFI mitigation
  • 10-20 MHz
  • ? requires C107
  • (N1000-10000, 1-10 MHz ? 1-10 sec)

C 103 105 107 109
22
  • Detectability from the Moon

C 103 105 107 109
  • 1 order of magnitude better
  • (C 105-6  N100, 1-10 MHz ? 1-10 sec)
  • access to less energetic sources
  • (C 106-7  Ngtgt100)
  • access to VLF (weakly magnetized bodies)

23
  • NB 
  • Angular resolution required 1-10
  • ? D 6-60 ?
  • (18-180 km _at_ 100 kHz  1.8-18 km _at_ 1 MHz)
  • if detectability of exo-planetary radio
    emissions ? same for solar-like stellar radio
    emissions
  • complementarity to ground-based LOFAR
  • difficult from space
  • weak scattering/broadening effects at sources
    distances lta few 10s pc

24
  • possible active sounding of Terrestrial
    magnetosphere (IMAGE)
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