This space physics research project
concerns studies of the interaction between radio waves (or, as
we say, electromagnetic radiation) and the outer,
tenuous part of the Earth's atmosphere at hundreds of
kilometres above the surface of the Earth. Due to the strong,
natural ultra-violet (UV) and X-ray radiation from the Sun, a
few of the atoms and molecules in this gas are broken up into
electrons, which are elementary particles with negative
electric charge, and ions of positive electric charge.
Since the behaviour of electric and magnetic fields and waves
is strongly affected by this tenuous ionised gas, which
constitutes what we call a plasma, this region of the
outer planetary atmospheres is called the ionosphere.
Study of the Earth's ionospheric plasma - a space plasma
which has existed in our own "space backyard" for millions, if
not billions of years - is very important for a complete
understanding of the interplay between Earth and its space
environment (also known as Earthspace) since it constitutes an
important link in the
biosphere-atmosphere-ionosphere-magnetosphere-heliosphere chain
that influences life on Earth.
Also, since over 99% of all known matter in universe is in
the plasma state and information from it comes in the form of
electromagnetic radiation (radio, infrared, optical,
ultraviolet, X-ray, and gamma radiation) a good knowledge of
the intricate physics which governs the interaction between
electromagnetic radiation and plasmas anywhere, is essential
for the understanding of Universe as a whole. In view of this,
we now use the near-Earth space plasma (ionosphere, lower
magnetosphere) as a giant natural laboratory where we perform
model experiments, mimicking conditions in other space plasma
environments. This allows us to use a powerful
stimulus-response methodology for investigating, in a
systematic manner, phenomena which would otherwise be
impossible to study experimentally.
Open questions which we address in
this research project include:
- How do the large variations in the Sun's activity,
mediated to the Earth via the natural solar radiation and the
solar wind, affect the state of the ionosphere and/or the
upper atmosphere?
- How can we understand the mechanisms responsible for
the generation of the copious amounts of natural
electromagnetic radiation in the Earth's magnetosphere that
continuously "bombard" the ionosphere and have done so for
eons?
- How can we understand and predict the detailed
mechanism behind the huge short-time and long-time natural
variations in the plasma content of the ionosphere, causing the
depletion of this plasma over vast volumes (often referred to
as ionospheric irregularities, "holes", "cavities", or
"bubbles") and observed ever since the early days of
ionospheric research?
- Can we learn anything new about our own space habitat
from the electromagnetic radiation observed? Can we apply such
knowledge to help interpret the physical processes that
generate the electromagnetic radiation received from remote
sources such as radio astronomical objects? If so, does this
radiation contain any signatures which can help us understand
the creation and the development of Universe and our own
planet?
- Do the natural physical processes that take place in the
Earth's magnetosphere and ionosphere, located at hundreds to
thousands of km altitude, have any measurable influence on the
atmosphere or the ozone layer at much lower altitudes, or
perhaps even on the Earth's weather system and climate?
- Does the electromagnetic radiation from the tens of
thousands of broadcast, TV, utility, radar and research
stations deployed on the ground by man over the past century,
or from the many satellites put into orbit over the past half
century, have any effect on the ionosphere? If so, is this an
adverse or a positive effect? Or, if measurable at all, is it
harmless?
The best way of finding answers to these, and similar,
important questions is to use the method of probing the
atmosphere, ionosphere, and the magnetosphere with radio waves
from the ground. While, in principle, any of the thousands of
existing powerful broadcasting or TV stations could be used for
scientific radio probing of the near-Earth space environment,
such an approach would be impractical, bordering on the
impossible. Hence, scientists have, in international
collaboration, built their own handful of radio stations, to be
used exclusively for scientific purposes, at various places on
Earth. Well-known examples are the Arecibo Observatory, Puerto
Rico; Jicamarca Radio Observatory, Peru; EISCAT, Northern
Scandinavia; Nançay, France; MU Radar, Japan; Sura, Russia;
HIPAS and HAARP, Alaska, and others of the same type.
Radio waves are a combination of
oscillating electric and magnetic fields which, in the
short-wave range, have an oscillation rate, or as we prefer to
say, a frequency, which is in the order of a few million
times per second (Megahertz, MHz). We call these
short-wave radio frequencies, from 3 to 30 MHz, the High
Frequency (HF) range. This is the short-wave radio band
used by international short-wave/HF broadcasters such as the
BBC World Service, Voice of America, and Radio Sweden. The
frequency range in which our FM radio stations operate is
tenfold higher and is called the Very High Frequency
(VHF) range. Still a tenfold higher is the Ultra High
Frequency (UHF) band where we find, for instance, TV and
radar transmitters. Satellite TV and mobile radio
communication systems operate in the Super High Frequency
(SHF) range a thousand times higher than HF. So despite
its name, given in the early days of radio communication to
discriminate it from the long-wave (Low Frequency/LF) and
medium-wave (Medium Frequency/MF) bands used by many
broadcasters at the time, the short-wave (High Frequency/HF)
band of frequencies are nowadays considered to be low-frequency
(long wavelength) in nature.
The ionospheric plasma has, at each given altitude, its own
natural resonance frequency called the plasma frequency.
The exact value of this plasma frequency depends on how many
electrons per cubic metre there happen to be at the altitude in
question, and this, in turn, is determined by the solar
activity and the local density of the atmosphere. At about 100
km altitude where the atmosphere is relatively dense but the
solar radiation is weak the ionospheric plasma frequency lies
typically in the long-wave/LF or medium-wave/MF range. At
altitudes of 200-400 km it lies in the short-wave/HF range. At
still higher altitudes of 500-1000 km the solar radiation is
quite strong, but the atmosphere so very dilute that the plasma
frequency is again lower. At the particular altitude where the
frequency of a vertically propagating radio wave coincides with
the local ionospheric plasma frequency, the radio wave will
interact with the ionosphere in such a way that the wave will
be reflected. It is this reflecting property of the
ionosphere, discovered already about a hundred years ago, which
makes the everyday high-frequency radio communication over
large distances possible.
Recently we have demonstrated experimentally that radio
waves from modern radio stations are strong enough that the
interaction in the reflecting region of the ionosphere is such
that the plasma no longer can be thought of as a passive,
reflecting mirror. A more accurate description of the
ionospheric plasma is that it self-modifies weakly its
reflecting properties more or less in synchronism with the
radio waves that propagate through and reflect from it. The
fact that the "mirror" so to speak takes an active part in the
reflection process is due to weak, complicated, but important
non-linear (non-proportional) properties which can lead
to turbulence and perhaps even chaos in the plasma. We call
this phenomenon ionospheric modification and its
manifestation shows that the old, simplistic picture, based on
linear models of the physical processes in plasma, is no longer
adequate. Like all plasmas in nature, the ionosphere is a
complex physical system and not just a passive mirror of radio
signals. We have only just begun to understand this complexity
and much more basic research is needed before we have an
adequate knowledge of the true behaviour of the ionosphere and
other space plasma.
For hundreds of millions of years
the Earth's ionosphere and upper atmosphere have been subjected
to perturbations from above in the form of enormous radiation
and particle streams of solar and other cosmic origin. This is
manifested in many ways, for instance by the Aurora Borealis
("northern lights") and the Aurora Australis ("southern
lights") which occur almost daily in the upper parts of the
polar zone atmospheres. Other examples are the large and small
"ionospheric holes" or "cavities" which appear regularly when
the Earth rotates away from the Sun so that the ionosphere
receives less solar UV and X-ray radiation. The same thing
happens also during solar eclipses and during magnetospheric
storms. Hence, "ionospheric holes" have been an integral and
most natural part of our space environment for as long as life
has existed on Earth, and are entirely different from and
totally independent of the holes which have appeared over the
last decades in the ozone layer at much lower altitudes.
"Ionospheric holes" are created mainly due to the absence of
electromagnetic radiation and can therefore not be created by
radio waves, for instance. And in contrast to ozone holes,
"ionospheric holes" provide (a slightly) increased protection
from cosmic radiation.
Other perturbations of the ionosphere are caused by the
extremely powerful radio emissions which occur naturally in
space. One example is the Auroral Kilometric Radiation (AKR)
which can release up to hundreds of billions of watts of
electromagnetic radiation in the ELF-MF range. This powerful
radiation impinges upon the ionosphere from above. Other
examples are the radio emissions from the plasma around the
Sun, called Soloar Corona Radio Emissions which were observed
on the Earth for the first time in the 1940s. They are caused
by giant eruptions on the Sun and are accompanied by an intense
particle radiation which can easily destroy communication
satellites and electric power grids on the ground.
In addition, meteors and other "space dust" which we can
observe as "shooting stars" deposit substantial amounts of
various chemical substances in the ionosphere and the upper
atmosphere.
From below, the ionosphere is continually being irradiated
with thousands of megawatts of radio waves generated by
lightning strokes associated with the thunderstorms which occur
in the Earth's lower atmosphere at a rate of about one hundred
per second. It is also irradiated by the electromagnetic waves
from the tens of thousands of broadcast, TV, utility and radar
stations that are in use on the surface on the Earth. The
radiated powers from the more powerful of these stations range
from a few hundred kilowatts to a few megawatts. The handful
of research radio facilities that use radio waves for studying
the environment use the same type of transmitters with the same
powers, but are so few that they contribute negligibly to the
total man-made radiation. However, they are absolutely
indispensible when it comes to monitoring the atmosphere and
space surroundings of our planet, and for developing better
tools for such investigations.
Our research has demonstrated that
not only natural perturbations but also radio waves from modern
high-power radio stations can have such a "modifying" effect.
As a consequence, the ionospheric plasma produces its own radio
emissions of a more or less noise-like character at frequencies
which are offset from that of the original radio wave.
However, this secondary radiation is extremely faint, only
about one billionth of the power of the primary radio
transmission, and is very difficult to detect. In a way, it is
the same as trying to detect, in the midst of a roaring gale,
the small ripples of about one tenth of a millimetre caused by
dropping a small grain of sand on the surface of an ocean,
while the natural ocean waves are tens of metres high. Such
precision measurements of extremely diminutive waves are
possible only by using modern signal analysers and powerful
signal processing methods, allowing us to "dig noise out of
noise" and they allow us to develop better radio methods for
studying the Earth's space environment. This is in line with
the long-standing tradition in space physics where space has
been investigated with radio methods for almost a century.
The basis for the development of a new diagnostic tool of
this type was laid in 1981 when during ionospheric radio
experiments using the EISCAT/Heating facility in Tromsø in
Norway, Bo Thidé from IRFU was the first to detect, on the
ground, weak secondary electromagnetic radiation from the
ionospheric plasma, a phenomenon now known as stimulated
electromagnetic emission (SEE). Since then we have learned
how to utilise this SEE radiation as a method for studying many
new physical properties of plasma both in the proximity of the
Earth and further out in the Universe. By using our
experiments to learn how to "read off" the properties of the
secondary radio emission, we obtain a "fingerprint" of the
local conditions in the region where this radiation appears.
Since such secondary radio emissions are excited in almost all
plasma and this emission can propagate over vast distances,
through even extreme environments before they reach us on
Earth, this "fingerprinting technique" has provided completely
new possibilities for exploring physical conditions in those
regions of our universe where we can never expect to make
direct measurements.
As is well known, there exists around
the Earth a magnetic field which does not vary very much with
time or space, and which we use when we navigate with the help
of a compass. This magnetic field penetrates the ionospheric
plasma to make it magnetised. A magnetised plasma is
birefringent ("double refracting") for radio waves in a
way similar to that in which certain crystals are birefringent
for light waves (a light ray is split up into two parts, or
polarisation modes, which propagate and refract
independently and differently in the crystal).
The birefringence of the magnetised ionospheric plasma is
due to the fact that the Earth's magnetic field strongly
affects the motion of the charged particles (electrons, ions)
of the ionosphere. Among other things, it means that the
electrons and ions can move fairly easily along the direction
of the Earth's magnetic field, while the motion across the
magnetic field is restricted to a circular motion perpendicular
to this direction.
This dependence of the motion of the plasma particles on
the direction of the external magnetic field causes what is
called symmetry breaking. As a consequence of this, a
magnetised plasma will, when being is subjected to external
perturbations such as powerful radio waves, structure itself
into long, "cigar shaped" structures orientated along the
Earth's magnetic field from which a few percent of the plasma
will be "snow-ploughed" away. It is of great interest to study
the properties of such self-organised irregularities, created
under controlled experimental conditions, since similar
structures appear spontaneously in nature but are often
difficult to analyse there. Our experiments therefore help us
understand better non-linear phenomena which exhibit
self-structuring and chaos, something which occurs in many
different physical systems both on Earth and of the Universe as
a whole.
The plasma structures elongated along the Earth's magnetic
field which are formed under the action of external radio wave
irradiation, also have the property that they contribute to the
transformation of the plasma turbulence into the secondary
radio emission mentioned above.