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2.4 Bases Associated with Lines
Restricting the Heisenberg representation π to a subgroup L yields a decom-
position of the Hilbert space
H
into a direct sum of one-dimensional subspaces
= χ H χ , where χ runs in the set L of (complex valued) characters of the
group L . The subspace H χ consists of vectors ϕ ∈H such that π ( l ) ϕ = χ ( l ) ϕ .
In other words, the space H χ consists of common eigenvectors with respect to
the commutative system of unitary operators
H
{
π ( l )
} l∈L
such that the operator
π ( l ) has eigenvalue χ ( l ).
Choosing a unit vector ϕ χ
L
∈H χ for every χ
we obtain an orthonor-
.Inparticular, Δ and Δ are recovered as the
bases associated with the lines T =
L }
mal basis
B L =
{
ϕ χ : χ
{
( τ, 0) : τ
F p }
and W =
{
(0 ,w ): w
F p }
respectively. For a general L the signals in
B L are certain kinds of chirps. Con-
cluding, we associated with every line L
B L , and
overall we constructed a system of signals consisting of a union of orthonormal
bases
V
an orthonormal basis
S H =
{
ϕ
∈B L : L
V
}
.
For obvious reasons, the system
S H will be called the Heisenberg system .
2.5
Properties of the Heisenberg System
It will be convenient to introduce the following general notion. Given two sig-
nals φ, ϕ
∈H
, their matrix coecient is the function m φ,ϕ : H
C
given by
m φ,ϕ ( h )=
φ, π ( h ) ϕ
. In coordinates, if we write h =( τ, w, z )then m φ,ϕ ( h )=
ψ
2 τw + z
1
.When φ = ϕ the function m ϕ,ϕ is called the am-
biguity function of the vector ϕ and is denoted by A ϕ = m ϕ,ϕ .
The system
φ, M w
L τ ϕ
S H consists of p + 1 orthonormal bases 1 , altogether p ( p +1)
signals and it satisfies the following properties [2,5]
1. Auto-correlation . For every signal ϕ
∈B L the function
|
A ϕ |
is the charac-
teristic function of the line L , i.e.,
= 0 ,v/
L,
|
A ϕ ( v )
|
1 ,v
L.
2. Cross-correlation . For every φ
∈B L and ϕ
∈B M where L
= M we have
1
p ,
|
m ϕ,φ ( v )
|≤
for every v ∈ V .If L = M then |m ϕ,φ | is the characteristic function of some
translation of the line L .
3. Supremum . Asignal ϕ
1
p
S H is a unimodular function, i.e.,
|
ϕ ( t )
|
=
for
every t
F p ,inparticularwehave
1
p
max
{|
ϕ ( t )
|
: t
F p }
=
1.
1 Note that p + 1 is the number of lines in V .
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