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v2009.01.01 - Convex Optimization

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4.5. CONSTRAINING CARDINALITY 299<br />

a television transmission over cable or the airwaves, or a typically ravaged<br />

cell phone communication, etcetera.<br />

Here we consider signal dropout in a discrete-time signal corrupted by<br />

additive white noise assumed uncorrelated to the signal. The linear channel<br />

is assumed to introduce no filtering. We create a discretized windowed<br />

signal for this example by positively combining k randomly chosen vectors<br />

from a discrete cosine transform (DCT) basis denoted Ψ∈ R n×n . Frequency<br />

increases, in the Fourier sense, from DC toward Nyquist as column index of<br />

basis Ψ increases. Otherwise, details of the basis are unimportant except<br />

for its orthogonality Ψ T = Ψ −1 . Transmitted signal is denoted<br />

s = Ψz ∈ R n (686)<br />

whose upper bound on DCT basis coefficient cardinality cardz ≤ k is<br />

assumed known; 4.31 hence a critical assumption that transmitted signal s is<br />

sparsely represented (k < n) with respect to the DCT basis. Nonzero signal<br />

coefficients in vector z are assumed to place each chosen basis vector above<br />

the noise floor.<br />

We also assume that the gap’s beginning and ending in time are precisely<br />

localized to within a sample; id est, index l locates the last sample prior to<br />

the gap’s onset, while index n−l+1 locates the first sample subsequent to<br />

the gap: for rectangularly windowed received signal g possessing a time-gap<br />

loss and additive noise η ∈ R n<br />

⎡<br />

⎤<br />

s 1:l + η 1:l<br />

g = ⎣ η l+1:n−l<br />

⎦∈ R n (687)<br />

+ η n−l+1:n<br />

s n−l+1:n<br />

The window is thereby centered on the gap and short enough so that the DCT<br />

spectrum of signal s can be assumed invariant over the window’s duration n .<br />

Signal to noise ratio within this window is defined<br />

[<br />

∥<br />

SNR = ∆ 20 log<br />

]∥<br />

s 1:l ∥∥∥<br />

s n−l+1:n<br />

‖η‖<br />

(688)<br />

In absence of noise, knowing the signal DCT basis and having a<br />

good estimate of basis coefficient cardinality makes perfectly reconstructing<br />

4.31 This simplifies exposition, although it may be an unrealistic assumption in many<br />

applications.

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