In 1946, Dennis Gabor suggested that a signal can be represented in two dimensions, with time and frequency coordinates. And the signal can be expanded into a discrete set of Gaussian elementary signals.

Definition edit

The Gabor expansion of signal s(t) is defined by this formula:

${\displaystyle s(t)=\sum _{m=-\infty }^{\infty }\sum _{n=-\infty }^{\infty }C_{m,n}h(t-mT)e^{jnt\Omega }}$ 

where h(t) is the Gaussian elementary function:

${\displaystyle h(t)=\left({\frac {\alpha }{\pi }}\right)^{\frac {1}{4}}e^{\left(-{\frac {\alpha }{2}}t^{2}\right)}}$ 

Once the Gabor elementary function is determined, the Gabor coefficients ${\displaystyle C_{m,n}}$ can be obtained by the inner product of s(t) and a dual function ${\displaystyle \gamma (t)}$ 

${\displaystyle C_{m,n}=\int s(t)\gamma ^{*}(t-mT)e^{-jnt\Omega }\,dt.}$ 

${\displaystyle T}$  and ${\displaystyle \Omega }$  denote the sampling steps of time and frequency and satisfy the criteria

${\displaystyle T\Omega \leqq 2\pi \,}$ 

Relationship between Gabor representation and Gabor transform edit

Gabor transform simply computes the Gabor coefficients ${\displaystyle C_{m,n}}$  for the signal s(t).

Adaptive signal expansion is defined as

${\displaystyle s\left(t\right)=\sum _{p}B_{p}h_{p}(t)}$ 

where the coefficients ${\displaystyle B_{p}}$  are obtained by the inner product of the signal s(t) and the elementary function ${\displaystyle h_{p}}$ 

${\displaystyle B_{p}=\left\langle s,h_{p}\right\rangle \,}$ 

Coeffients ${\displaystyle B_{p}}$  represent the similarity between the signal and elementary function.
Adaptive signal decomposition is an iterative operation, aim to find a set of elementary function ${\displaystyle \left\{h_{p}(t)\right\}}$ , which is most similar to the signal's time-frequency structure.
First, start with w=0 and ${\displaystyle s_{0}\left(t\right)=s\left(t\right)}$ . Then find ${\displaystyle h_{0}\left(t\right)}$  which has the maximum inner product with signal ${\displaystyle s_{0}\left(t\right)}$  and

${\displaystyle \left|B_{p}\right|^{2}=\max _{h}\left|\left\langle s_{p}(t),h_{p}(t)\right\rangle \right|^{2}}$ 

Second, compute the residual:

${\displaystyle s_{1}\left(t\right)=s_{0}\left(t\right)-B_{0}h_{0}\left(t\right),}$ 

and so on. It will comes out a set of residual (${\displaystyle s_{p}\left(t\right)}$ ), projection (${\displaystyle B_{p}=\left\langle s_{p}(t),h_{p}(t)\right\rangle }$ ), and elementary function (${\displaystyle h_{p}\left(t\right)}$ ) for each different p. The energy of the residual will vanish if we keep doing the decomposition.

Energy conservation equation edit

If the elementary equation (${\displaystyle h_{p}\left(t\right)}$ ) is designed to have a unit energy. Then the energy contain in the residual at the pth stage can be determined by the residual at p+1th stage plus (${\displaystyle B_{p}}$ ). That is,

${\displaystyle \left\|s_{p}(t)\right\|^{2}=\left\|s_{p+1}(t)\right\|^{2}+\left|B_{p}\right|^{2},}$ 

${\displaystyle \left\|s(t)\right\|^{2}=\sum _{p=o}^{\infty }\left|B_{p}\right|^{2},}$ 

similar to the Parseval's theorem in Fourier analysis.

The selection of elementary function is the main task in adaptive signal decomposition. It is natural to choose a Gaussian-type function to achieve the lower bound for the inequality:

${\displaystyle h_{p}(t)=\left({\frac {\alpha }{\pi }}\right)^{\frac {1}{4}}e^{-{\frac {\alpha }{2}}(t-T_{p})^{2}}e^{jt\Omega _{p}},}$ 

where ${\displaystyle \left(T_{p},\Omega _{p}\right)}$  is th mean and ${\displaystyle \alpha _{p}^{-1}}$  is the variance of Gaussian at ${\displaystyle \left(T_{p},\Omega _{p}\right)}$ . And

${\displaystyle s\left(t\right)=\sum _{p}B_{p}h_{p}(t)=\sum _{p}B_{p}\left({\frac {\alpha }{\pi }}\right)^{\frac {1}{4}}e^{-{\frac {\alpha }{2}}(t-T_{p})^{2}}e^{jt\Omega _{p}}}$ 

is called the adaptive Gabor representation.

Changing the variance value will change the duration of the elementary function (window size), and the center of the elementary function is no longer fixed. By adjusting the center point and variance of the elementary function, we are able to match the signal's local time-frequency feature. The better performance of the adaptation is achieved at the cost of matching process. The trade-off between different window length now become the trade-off between computation time and performance.

• Gabor transform
• Short-time Fourier transform

• M.J. Bastiaans, "Gabor's expansion of a signal into Gaussian elementary signals", Proceedings of the IEEE, vol. 68, Issue:4, pp. 538–539, April 1980
• Shie Qian and Dapang Chen, "Signal Representation using adaptive normalized Gaussian functions," Signal Processing, vol. 42, no.3, pp. 687–694, March 1994
• Qinye Yin, Shie Qian, and Aigang Feng, "A Fast Refinement for Adaptive Gaussian Chirplet Decomposition," IEEE Transactions on Signal Processing, vol. 50, no.6, pp. 1298–1306, June 2002
• Shie Qian, Introduction to Time-Frequency and Wavelet Transforms, Prentice Hall, 2002