Strömberg wavelet explained

In mathematics, the Strömberg wavelet is a certain orthonormal wavelet discovered by Jan-Olov Strömberg and presented in a paper published in 1983.[1] Even though the Haar wavelet was earlier known to be an orthonormal wavelet, Strömberg wavelet was the first smooth orthonormal wavelet to be discovered. The term wavelet had not been coined at the time of publishing the discovery of Strömberg wavelet and Strömberg's motivation was to find an orthonormal basis for the Hardy spaces.[1]

Definition

Let m be any non-negative integer. Let V be any discrete subset of the set R of real numbers. Then V splits R into non-overlapping intervals. For any r in V, let Ir denote the interval determined by V with r as the left endpoint. Let P(m)(V) denote the set of all functions f(t) over R satisfying the following conditions:

If A0 = ∪ ∪ and A1 = A0 ∪ then the Strömberg wavelet of order m is a function Sm(t) satisfying the following conditions:[1]

Sm(t)\inP(m)(A1).

\VertSm(t)\Vert=1

, that is,

\intR\vertSm(t)\vert2dt=1.

Sm(t)

is orthogonal to

P(m)(A0)

, that is,

\intRSm(t)f(t)dt=0

for all

f(t)\inP(m)(A0).

Properties of the set P(m)(V)

The following are some of the properties of the set P(m)(V):

  1. Let the number of distinct elements in V be two. Then f(t) ∈ P(m)(V) if and only if f(t) = 0 for all t.
  2. If the number of elements in V is three or more than P(m)(V) contains nonzero functions.
  3. If V1 and V2 are discrete subsets of R such that V1V2 then P(m)(V1) ⊂ P(m)(V2). In particular, P(m)(A0) ⊂ P(m)(A1).
  4. If f(t) ∈ P(m)(A1) then f(t) = g(t) + α λ(t) where α is constant and g(t) ∈ P(m)(A0) is defined by g(r) = f(r) for rA0.

Strömberg wavelet as an orthonormal wavelet

The following result establishes the Strömberg wavelet as an orthonormal wavelet.[1]

Theorem

Let Sm be the Strömberg wavelet of order m. Then the following set

\left\{2j/2Sm(2jt-k):j,kintegers\right\}

is a complete orthonormal system in the space of square integrable functions over R.

Strömberg wavelets of order 0

In the special case of Strömberg wavelets of order 0, the following facts may be observed:

  1. If f(t) ∈ P0(V) then f(t) is defined uniquely by the discrete subset of R.
  2. To each sA0, a special function λs in A0 is associated: It is defined by λs(r) = 1 if r = s and λs(r) = 0 if srA0. These special elements in P(A0) are called simple tents. The special simple tent λ1/2(t) is denoted by λ(t)

Computation of the Strömberg wavelet of order 0

As already observed, the Strömberg wavelet S0(t) is completely determined by the set . Using the defining properties of the Strömbeg wavelet, exact expressions for elements of this set can be computed and they are given below.[2]

S0(k)=S0(1)(\sqrt{3}-2)k-1

for

k=1,2,3,\ldots

S0(\tfrac{1}{2})=-S0(1)\left(\sqrt{3}+\tfrac{1}{2}\right)

S0(0)=S0(1)(2\sqrt{3}-2)

S0(-\tfrac{k}{2})=S0(1)(2\sqrt{3}-2)(\sqrt{3}-2)k

for

k=1,2,3,\ldots

Here S0(1) is constant such that ||S0(t)|| = 1.

Some additional information about Strömberg wavelet of order 0

The Strömberg wavelet of order 0 has the following properties.[2]

S0(-k/2)=(10-6\sqrt{3})S0(k)

for

k=1,2,3,\ldots.

Notes and References

  1. Janos-Olov Strömberg, A modified Franklin system and higher order spline systems on Rn as unconditional bases for Hardy spaces, Conference on Harmonic Analysis in Honor of A. Zygmond, Vol. II, W. Beckner, et al (eds.) Wadsworth, 1983, pp.475-494
  2. Book: P. Wojtaszczyk. A Mathematical Introduction to Wavelets. registration. 1997. Cambridge University Press. 0521570204. 5–14.