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with respect to the restriction of the Weil representation to a maximal non-split
torus in SL 2 . The only difference appears to be the field of definition, which for
the harmonic oscillator is the reals and for the oscillator functions is the finite
field.
4
Applications
Two applications of the oscillator system will be described. The first application
is to the theory of discrete radar. The second application is to CDMA systems.
We will give a brief explanation of these problems, while emphasizing the relation
to the Heisenberg representation.
4.1
Discrete Radar
The theory of discrete radar is closely related [2] to the finite Heisenberg group
H. A radar sends a signal ϕ ( t )andobtainsanecho e ( t ). The goal [9] is to
reconstruct, in maximal accuracy, the target range and velocity. The signal ϕ ( t )
and the echo e ( t ) are, principally, related by the transformation
e ( t )= e 2 πiwt ϕ ( t + τ )= M w L τ ϕ ( t ) ,
where the time shift τ encodes the distance of the target from the radar and
the phase shift encodes the velocity of the target. Equivalently, the transmitted
signal ϕ and the received echo e are related by an action of an element h 0
H ,
i.e., e = π ( h 0 ) ϕ. The problem of discrete radar can be described as follows.
Given a signal ϕ and an echo e = π ( h 0 ) ϕ extract the value of h 0 .
It is easy to show that
and it obtains its maximum
at h 0 . This suggests that a desired signal ϕ for discrete radar should admit an
ambiguity function A ϕ which is highly concentrated around 0
|
m ϕ,e ( h )
|
=
|
A ϕ ( h
·
h 0 )
|
H ,whichisa
property satisfied by signals in the oscillator system (Property 2).
Remark 2. It should be noted that the system
S O is “large” consisting of order
of p 3 signals. This property becomes important in a jamming scenario.
4.2
Code Division Multiple Access (CDMA)
We are considering the following setting.
- There exists a collection of users i
I , each holding a bit of information
(usually b i is taken to be an N 'th root of unity).
- Each user transmits his bit of information, say, to a central antenna. In order
to do that, he multiplies his bit b i by a private signal ϕ i ∈H
b i C
and forms a
message u i = b i ϕ i .
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