Several types of scatter radar techniques are used for upper atmosphere research. Coherent scatter radar is a volume scattering technique whereby the radar detects energy scattered from within a medium when there are regular spatial variations of the refractive index due to irregularities. This is the analogue of Bragg scattering of X-rays from crystals. The ionosphere contains irregularities of many different sizes and in general a small fraction of the incident energy is scattered at each boundary. Signals backscattered from plasma wave irregularities with a spacing of half the radar wavelength will reinforce by constructive interference in the direction back to the radar and can produce a signal strong enough to be detected by the receiver. Thus, a radar of wavelength will effectively select from the scattering medium the spatial component of wavelength along the radar beam (a more detailed derivation of this property follows). The term ``coherent'' applies to the constructive interference possible when there is a scattering structure with an organized spatial content at half the radar wavelength.

The *scatter theorem* describes the signals that can be measured
by a coherent scatter radar. Figure 3.1
(left) shows the geometry used in the derivation of the scatter theorem for
a bistatic radar system.

**Figure 3.1:** Geometry of scatter theorem analysis

The origin of the coordinate system lies within the scattering region under
observation, points to a position within this region,
and are the positions of the transmitter and the
receiver, respectively. They are fixed in space and can be considered
constant in this derivation. We introduce further the vectors
and
. Considered is a volume element
*dV* at the position . The electric field produced by the
transmitter is given by:

where is the electric field at the transmitter, is the
transmitter antenna voltage gain and is the angular frequency of the
wave.
The electric field at the receiver from the volume element *dV*
is then given by:

where is the amplitude scattering cross section of electrons for signals
incident along and scattered along and
is the electron density at
and time *t*. To simplify this equation it is assumed that for a narrow
beam, the voltage gain function for the transmitting and receiving antennas can be
set to constants and respectively.
A similar simplification is done with the
scattering cross section which is set to a constant, since all
spatial information is contained in the electron density term *D*.
The differential voltage produced at the receiver input by volume element
*dV* of the scatterer is then:

Assuming and , performing a Taylor expansion on and and neglecting quadratic terms, one obtains the following approximations for the transmitter (t) and receiver (r) distances:

This approximation can now be used to rewrite the amplitude term , but not the phase term. Using the unit vectors and , equation 3.3 becomes:

We express the electron density through its Fourier component . Thus if the transform is denoted by the definition of N is:

That is, by the inverse transform,

or

Substituting Equation 3.9 into Equation 3.6 yields

In these steps we also used the fact that . If we integrate over the volume where backscatter occurs, the -dependent exponential term can be approximated by a delta function , where

This means we select the component of *N* that corresponds
to . After the integration over , taking the
delta function into account, the final result can be written as follows

where *C* denotes some constant.

This shows that the radar is sensitive to the Fourier components of the electron density fluctuation with wave vector , corresponding to the wavelength

where is the angle between and . This important property can be derived by considering the following equation derived from the conservation of momentum and energy in two dimensions (see Figure 3.1, right):

and

Rewriting Equation 3.14 in terms of the wavelength for
the *x* and *y* components gives

Similary Equation 3.15 becomes (using 3.17)

Hence using Equation 3.16

and Equation 3.17 we get

Using some trigonometric identities this can be written as

and since is small, it follows that

But since we arrive at the property that

which means that the angle which makes with the negative x-axis is along the bisector of the transmitter and receiver directions. Using this fact we can write Equation 3.14 as

where is the unit vector pointing along the incident direction and is perpendicular to . This can be simplified using the following trigonometric identities

to yield

By comparing the left and right side of this equation it follows that the direction and wavelength is described by:

We can convert to the angle that was used earlier using

which yields Equation 3.13 again. For a monostatic backscatter radar, with transmitting and receiving antennas at the same location, and .

Wed Oct 9 10:05:17 CST 1996