Radio Waves Diagnostics of Ionospheric Plasma
1Space Research Center, Polish Academy of Sciences, Warsaw, Poland
2 Swedish Institute of Space Physics, Uppsala, Sweden3 Institute of Experimental Physics, Slovak Academy of Sciences, Slovak
Republic
Corsica, Corte 21-27 June 2008
H. Rothkaehl1, J. Bergman2, J. Błęcki1, J. Juchniewicz1, K. Kudela3
M. Morawski1, B. Thide2
Wave in situ diagnostics ULF and LF ion plasma diagnostics, E B field fluctuations.
VLF low density plasma diagnostics
HF electron plasma diagnostics, Solar radio burst.
Local plasma frequency =local electron density tens kHz up to few MHz
Local gyro-frequency proportional to the intensity of magnetic field
tens kHz up to MHz
The ionosphere represents less than 0.1% of the total mass of the Earth's atmosphere. Even so, it is extremely important!
1. Electromagnetic pollution at top-side
ionosphere, H. Rothkaehl et al. 2003,2005
2. Broad band emissions inside the ionospheric
trough H. Rothkaehl et al.1997 ,Grigoryan
2003, Rotkhkaehl et al. 2007.
3. Whistler- gamma rays interaction related to
the Earthquake, Rothkaehl et al. 2006. Kudela,
Bucik 2005.
4. Emissions triggered by lightning, Bucik 2005
The map of gamma rays fluxes in the energy range 0.12-0.32 MeV detected by SONG on CORONAS-I satellite during the period from March 1994 through June 1994., K. Kudela, R. Bucik 2002
Magnetosphere-ionosphere coupling,interation of HF waves and energetic electrons
Radio waves diagnostic past experiments
IK-19 1978-1981
500-980 Km inc. 74 deg
0.1-6. MHz HF
IK-24 Activny 1989-1990
500-2500 Km inc. 82.5 deg
0.1- 10. MHz HF
IK-25 Apex Magion-3 1991-1992
430-3100 Km inc. 82.5 deg
0.1-10. MHz HF
Coronas-I 1994
500 Km inc. 82.5 deg
0.1-30. MHz HF
COMPASS 2
weighting 85 kg, circular orbit with height 400 km and inclination 79 degrees for development of the methods of monitoring and forecasting of natural disasters on the base of coordinated monitoring at the Earth and from space the pre-earthquake phenomena.
25 May 2006
Human activity can perturb Earth's
environment.
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6.04.1992
0-14 MHz
4-14 MHz
0-2 MHz
CORONAS
0
0.5
1
1.5
2
2.5
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1 2 3 4 5 6 7
'STOS''STOSW''STOS.2'
'STOSW.2'
Jk, Lang k=0.25Ion-akust k=0.25Lang k=0.1Ion-akust k=0.1
pe
The ratio of emissionscoefficients S ,for scattering of subthermal
electron on Langmuir and ion-acoustic turbulence for different ratio of Te to Ti
for ionospheric plasma of ωfpe=1.3MHz.
The emissions coefficients for scattering of subthermal electron on the Langmuir jl
k, and ion-acoustic jsk, turbulence for
different k vector for Te=8000 °K, Ti=1200 °K , fpe=1.3MHz neo=0.1ne.
0
1
2
3
4
5
0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 k
'STOS''stos1''stos2'
Te/Ti=10Te/Ti=7Te/Ti=2.5
Langmir turbulence
Ion-acustic turbulence
Earthquake 31. 03.1994
DB
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max 171 E, 17 S0-2 MHz
455
normal grid mall45500
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Earthquake
22 40 52 UT
-180 long, -22 lat
Earthquake
HF diagnostics
171-170 long, -17 lat
Ionospheric response to seismic activity
HF increasing of wave activity (whistler mode) Enhancement of gamma rays in 0.12-0.35 Mev Increase of local electron density over epicentre Wave-like change of electron density at F2 layers,
enhancements of Es More pronouns effect during quit geomagnetic
condition
Parallel to the well-known effects related to the seismic activity in the top side ionosphere such as small-scale irregularities generated due to acoustic waves (Hegai et.al. 1997), and large-scale irregularities generated by anomalous electric field (Pulinets at al 2000), the modification of magnetic flux tube are also common features (Kim and Hegai 1997, Pulinets at al. 2002). So it seems that changes of the magnetic flux tube topology correlated with seismic activity can lead to the increase in the precipitation of energetic electron fluxes and, as a consequence, can yield excitation of the HF whistler mode. , H.Rothkaehl 2005
IONOSPHERIC TROUGH
W
KKf
mppt
2**
))(10/1(exp)8.033.1(
Rothkaehl et al.1997
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1 6 4 0 1 6 6 0 1 6 8 0 1 7 0 0 1 7 2 0 1 7 4 0 1 7 6 0
L
R E V
L p pL t r o u g h
L F - A K R , V L F , H F .
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'FOF2_B~1.TXT'
Magion-3
Alfven waves, LHR, UHR, EMIC
Double trough structure
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geographic long itude
C O R O N A S 3 0 0 3 1 9 9 4
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ge
og
rap
hic
la
titu
de
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D b
The global distribution over Europe of mean value of the electromagnetic emission in the ionosphere in the frequency range 0.1-15 MHz on 30.03.1994 during strong geomagnetic disturbances, recorded by SORS-1 instrument on board the Coronas_I satellite. The characteristic increase of emission over Euroasia is visible and the conjugate point in southward hemisphere . The area where maximum particle flux was registered is indicated by cross points. The resolution is 5x5 deg; the units are DB/μV
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g eo g rap h ic lo n g itu d e
C O R O N A S 3 0 . 0 3. 1 9 9 4
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0
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geo
gra
ph
ic l
atit
ud
e
3 0
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Africa
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Eh
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B x
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11 12 1 3 0 1 9 82 A R C A D -3
The global distribution of electric component Eh and magnetic component Bx registered during very quit condition from 11 till 13 January 1982 on the board AUREOL-3 satellite in the wide frequency band from
9 to 16 kHz. The intensity of detected emissions is in log(mV/m/√(Hz)) for electric component and log(nT/m//√(Hz)) for magnetic component.
ARCAD-3quite geom. conditions
LIGHTNING INDUCED HARD X-RAY FLUX ENHANCEMENTS: CORONAS-F
OBSERVATIONS,
Bucik 2005.X rays enhanced emissions 30 - 500 keV
Geographic locations of X ray counts (during two consecutive CORONAS-F orbits in each panel onNovember 9 (left), November 10-11 (middle), and November 12 (right). Colored scale matches the log of the counts.Lightning discharges detected by the LIS are shown as a red/blue The crosses on south indicate conjugate points of the northern lightning flashes. .
Trakhtengerts at al. 2003
LIGHTNING INDUCED HARD X-RAY FLUX ENHANCEMENTS: CORONAS-F OBSERVATIONS, Bucik 2005.
VLF emissions triggered by lightning
X rays enhanced emissions
UNIMAIsat-1• Mass < 10 kg
• Ionospheric orbit, 400-1000 km
• Define the main goals of the experiment
• Design the instruments
• Test the prototype• Design the mode of
operation
Memorybuffer
DSP
Glue Logic (FPGA)Internal data
bus
LPF
LPF
Glue Logic&
DSP
LPF
LPF
LPF
Internal databus
Wave Recorder conceptWave Recorder concept
Vector Digital Receiver conceptVector Digital Receiver concept
OBSTANOVKA on ISS
• General• Mass [kg] 5.4 (+10% / - 30 %)• Power [W] 12.0 (+30% / - 50 %)• Voltage [V] 28.0 ( +/- 20%)• Dimension [mm] 190.0x150.0x115.0
Radio waves are 3D EM vector waves!about 66% of the total information content
is lost if only single polarised antennas are used
Angular momentum
Angular momentum for EM field
= 0 planar waves, no components other than those along the axis of propagation
≠0, small non-zero components perpendicular to the axis of propagation
By providing a software configurable sensor and emitter infrastructure distributed in southern Sweden with Växjö,
LOIS will enhance the atmospheric and space physics capabilities of the huge, new-generation digital radio telescope LOFAR (Low Frequency Array), currently being built in the Netherlands. LOIS is a large radio telescope array that will operate in the 10-240 MHz frequency range. Its 13,000 dipole antennas will be clustered in roughly 100 stations spread over a region 400 km across.
Test station operated in Vaxjo
Twisted RF is the rotation of the plane of
polarisation within a transmitted or received
non planar waveform This concept has been
demonstrated at optical and sub-millimetre
wavelengths.
B. Thide at al. 2007
“Sura” operated by the Radiophysical Research Institute in Nizhniy Novgorod, Russia, will be used for systematic studies of the ionosphere;
A 1.2 MW HF ionospheric research radio transmitter, “Heating”,operated by the EISCAT (European Incoherent Scatter) scientific organisation in Tromso, northern Norway. This instrument is used for systematic studies of the ionosphere.
access to the following high-power radio sources in the 5-30 MHz frequency range:A 0.5 MW HF broadcast radio transmitter at Hörby, southern Sweden, operated by the Teracom company.,
Borowiec LOIS
POLFARPOLFAR
Future- MOON