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20 CHAPTER 2. SPARSITY IN IMAGE CODING<br />

exponent. We first introduce the definition of optimal exponent, then cite the result that<br />

states the connection between critical index and optimal exponent.<br />

Optimal Exponent<br />

We consider a functional space Θ made by infinite-length real-valued sequences. An ɛ-ball<br />

in Θ, which is centered at θ 0 , is (by definition) B ɛ (θ 0 )={θ : ‖θ − θ 0 ‖ 2 ≤ ɛ, θ ∈ Θ}, where<br />

‖·‖ 2 is the l 2 norm in Θ and θ 0 ∈ Θ. An ɛ-net of Θ is a subset of Θ {f i : i ∈ I,f i ∈ Θ} that<br />

satisfies Θ ⊂ ⋃ i∈I B ɛ(f i ), where I is a given set of indices. Let N(ɛ, Θ) denote the minimum<br />

possible cardinality of the ɛ-net {f i }. The (Kolmogorov-Tikhomirov) ɛ-entropy of Θ is (by<br />

definition)<br />

H ɛ (Θ) = log 2 N(ɛ, Θ).<br />

The ɛ-entropy of Θ, H ɛ (Θ), is to within one bit the minimum number of bits required<br />

to code in space Θ with distortion less than ɛ. If we apply the nearest-neighbor coding,<br />

the total number of possible cases needed to record is N(ɛ, Θ), which should take no more<br />

than ⌈log 2 N(ɛ, Θ)⌉ bits. (The value ⌈x⌉ is the smallest integer that is no smaller than x.)<br />

Obviously the ɛ-entropy of Θ, which is denoted by H ɛ (Θ), is within 1 bit of the total number<br />

of bits required to code in functional space Θ.<br />

It is not hard to observe that when ɛ → 0, H ɛ (Θ) → +∞. Now the question is how fast<br />

the ɛ-entropy H ɛ (Θ) increases when ɛ goes to zero. The optimal exponent defined in [47] is<br />

a measure of the speed of increment:<br />

α ∗ (Θ) = sup{α : H ɛ (Θ) = O(ɛ −1/α ),ɛ→ 0}.<br />

We refer readers to the original paper [47] for a more detailed discussion.<br />

Asymptotic Result<br />

The key idea is that there is a direct link between the critical index p ∗ and the optimal<br />

exponent α ∗ . The following is cited from [47], Theorem 2.<br />

Theorem 2.2 Let Θ be a bounded subset of l 2 that is solid, orthosymmetric, and minimally

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