25 research outputs found
The EISCAT meteor code
The EISCAT UHF system has the unique capability to determine meteor vector velocities from the head echo Doppler shifts measured at the three sites. Since even meteors spending a very short time in the common volume produce analysable events, the technique lends itself ideally to mapping the orbits of meteors arriving from arbitrary directions over most of the upper hemisphere. <br><br> A radar mode optimised for this application was developed in 2001/2002. A specially selected low-sidelobe 32-bit pseudo-random binary sequence is used to binary phase shift key (BPSK) the transmitted carrier. The baud-length is 2.4 μs and the receiver bandwidth is 1.6 MHz to accommodate both the resulting modulation bandwidth and the target Doppler shift. Sampling is at 0.6 μs, corresponding to 90-m range resolution. Target range and Doppler velocity are extracted from the raw data in a multi-step matched-filter procedure. For strong (SNR&gt;5) events the Doppler velocity standard deviation is 100–150 m/s. The effective range resolution is about 30 m, allowing very accurate time-of-flight velocity estimates. On average, Doppler and time-of-flight (TOF) velocities agree to within about one part in 10<sup>3</sup>. Two or more targets simultaneously present in the beam can be resolved down to a range separation &lt;300 m as long as their Doppler shifts differ by more than a few km/s
Meteor head echo altitude distributions and the height cutoff effect studied with the EISCAT HPLA UHF and VHF radars
Meteor fluxes and visual magnitudes from EISCAT radar event rates: a comparison with cross-section based magnitude estimates and optical data
The EISCAT meteor-head method ? a review and recent observations
International audienceSince the very first meteor observations at EISCAT in December 1990, the experimental method has improved significantly. This is due to a better understanding of the phenomenon and a recent major upgrade of the EISCAT signal processing and data storage capabilities. Now the simultaneous spatial-time resolution is under 100 m-ms class. To illuminate the meteor target for as long as possible and simultaneously get as good altitude resolution as possible, various coding techniques have been used, such as Barker codes and random codes with extremely low side lobe effects. This paper presents some background and the current view of the meteor head echo process at EISCAT as well as the observations which support this view, such as altitude distributions, dual-frequency target sizes and vector velocities. It also presents some preliminary results from recent very high resolution tristatic observations
Meteor head echo polarization at 930 MHz studied with the EISCAT UHF HPLA radar
The polarization characteristics of 930-MHz meteor head echoes have been
studied for the first time, using data obtained in a series of radar
measurements carried out with the tristatic EISCAT UHF high power, large
aperture (HPLA) radar system in October 2009. An analysis of 44 tri-static
head echo events shows that the polarization of the echo signal recorded by
the Kiruna receiver often fluctuates strongly on time scales of tens of
microseconds, illustrating that the scattering process is essentially
stochastic. On longer timescales (> milliseconds), more than 90 % of
the recorded events show an average polarization signature that is
independent of meteor direction of arrival and echo strength and equal to
that of an incoherent-scatter return from underdense plasma filling the
tristatic observation volume. This shows that the head echo plasma targets
scatter isotropically, which in turn implies that they are much smaller than
the 33-cm wavelength and close to spherically symmetric, in very good
agreement with results from a previous EISCAT UHF study of the head echo RCS/meteor angle-of-incidence relationship.
Significant polarization is present in only three events with unique target
trajectories. These all show a larger effective target cross section
transverse to the trajectory than parallel to it. We propose that the
observed polarization may be a signature of a transverse charge separation
plasma resonance in the region immediately behind the meteor head, similar
to the resonance effects previously discussed in connection with meteor
trail echoes by Herlofson, Billam and Browne, Jones and Jones and others
Meteor head echoes - observations and models
Meteor head echoes - instantaneous echoes moving with the velocities of the
meteors - have been recorded since 1947. Despite many attempts, this
phenomenon did not receive a comprehensive theory for over 4 decades. The High
Power and Large Aperture (HPLA) features, combined with present signal
processing and data storage capabilities of incoherent scatter radars, may
give an explanation for the old riddle. The meteoroid passage through the
radar beam can be followed with simultaneous spatial-time resolution of
about 100m-ms class. The current views of the meteor head echo process will
be presented and discussed. These will be related to various EISCAT
observations, such as dual-frequency target sizes, altitude distributions
and vector velocities