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Hann-Poisson Window
Definition:
![$\displaystyle w(n) = \frac{1}{2}\left[1 + \cos\left(\pi\frac{n}{\frac{M-1}{2}}\right)\right] e^{-\alpha\frac{\vert n\vert}{\frac{M-1}{2}}}$](img452.png) |
(4.35) |
Figure 3.21:
Hann-Poisson window (upper plot, circles)
and Fourier transform (lower plot). The upper plot also shows (using
solid lines) the Hann and Poisson windows that are multiplied
pointwise to produce the Hann-Poisson window.
![\includegraphics[width=\twidth]{eps/hannPoissonWindow}](img453.png) |
The Hann-Poisson window is, naturally enough, a Hann window times a
Poisson window (exponential times raised cosine). It is plotted along
with its DTFT in Fig.3.21.
The Hann-Poisson window has the very unusual feature among windows of
having ``no side lobes'' in the sense that, for
, the
window-transform magnitude has negative slope for all positive
frequencies [58], as shown in
Fig.3.22. As a result, this window is valuable for
``hill climbing'' optimization methods such as Newton's method or any
convex optimization methods. In other terms, of all windows we have
seen so far, only the Hann-Poisson window has a
convex transform magnitude to the left or right of the peak
(Fig.3.21b).
Figure 3.22:
Hann-Poisson Slope and Curvature
![\includegraphics[width=\twidth]{eps/hannPoissonSlope}](img455.png) |
Figure 3.23 also shows the slope and curvature of the Hann-Poisson
window transform, but this time with
increased to 3. We see
that higher
further smooths the side lobes, and even the
curvature becomes uniformly positive over a broad center range.
Figure 3.23:
Hann-Poisson magnitude,
slope, and curvature, in the frequency domain, for larger
.
![\includegraphics[width=\twidth]{eps/hannPoissonSlope2}](img456.png) |
Subsections
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