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Source codes, error probability and achievable compression rates (§14.4, for Theorem 14.4.1)

Definition
WildeQIT_sourceCode

by aadarwal · Sep 7, 2026 · Mathlib 0df444a (Lean v4.33.1)

classical-informationinformation-theorytypicalitywilde-qit

The notions behind Theorem 14.4.1 (Shannon compression), reconstructed from Wilde §14.4 (they are not roster items). An (n,R)(n,R)(n,R) source code for the i.i.d. source pXp_XpX​ consists of an encoder E:Xn→{1,…,M}E:\mathcal{X}^n\to\{1,\dots,M\}E:Xn→{1,…,M} with M≤2nRM\le 2^{nR}M≤2nR codewords and a decoder D:{1,…,M}→XnD:\{1,\dots,M\}\to\mathcal{X}^nD:{1,…,M}→Xn. Its error probability is Pr⁡{D(E(Xn))≠Xn}\Pr\{D(E(X^n))\ne X^n\}Pr{D(E(Xn))=Xn}. A rate RRR is achievable for XXX if for every ε∈(0,1)\varepsilon\in(0,1)ε∈(0,1), δ>0\delta>0δ>0 and all sufficiently large nnn there is an (n,R+δ)(n,R+\delta)(n,R+δ) code with error probability at most ε\varepsilonε.

Formalization Note. SourceCode α n M bundles enc : (Fin n → α) → Fin M and dec : Fin M → (Fin n → α); SourceCode.errorProb p c = ∑ x, if c.dec (c.enc x) = x then 0 else (p.iid n).prob x; IsAchievableSourceRate p R quantifies ∀ ε ∈ (0,1), ∀ δ > 0, ∃ N, ∀ n ≥ N, ∃ M ≤ 2^{n(R+δ)}, ∃ c, errorProb ≤ ε (real exponent, Real.rpow).

Definition code
import Definitions.Def_WildeQIT_iid
import Mathlib.Analysis.SpecialFunctions.Pow.Real

/-!
Wilde, *Quantum Information Theory* (2nd ed.), §14.4 (Application: Data compression), the
notions used by Theorem 14.4.1 (Shannon compression): an `(n, R)` source code for the i.i.d.
source `p_X` maps each sequence `xⁿ` to one of at most `2^{nR}` codewords and decodes back; its
error probability is `Pr{ D(E(Xⁿ)) ≠ Xⁿ }`; a rate `R` is achievable if for every `ε ∈ (0,1)`,
`δ > 0` and all sufficiently large `n` there is an `(n, R + δ)` code with error probability at
most `ε`.
-/

namespace WildeQIT

/-- A source code of block length `n` with `M` codewords: an encoder into `Fin M` and a decoder. -/
structure SourceCode (α : Type) (n M : ℕ) where
  /-- The encoder `E : 𝒳ⁿ → {1, …, M}`. -/
  enc : (Fin n → α) → Fin M
  /-- The decoder `D : {1, …, M} → 𝒳ⁿ`. -/
  dec : Fin M → (Fin n → α)

variable {α : Type} [Fintype α] [DecidableEq α]

/-- The error probability `Pr{ D(E(Xⁿ)) ≠ Xⁿ }` of a source code under the i.i.d. source `p`. -/
noncomputable def SourceCode.errorProb {n M : ℕ} (p : FinDist α) (c : SourceCode α n M) : ℝ :=
  ∑ x, if c.dec (c.enc x) = x then 0 else (p.iid n).prob x

/-- A rate `R` is achievable for the source `p`: for every `ε ∈ (0,1)` and `δ > 0`, for all
sufficiently large `n` there is a source code with at most `2^{n(R+δ)}` codewords and error
probability at most `ε`. -/
def IsAchievableSourceRate (p : FinDist α) (R : ℝ) : Prop :=
  ∀ ε : ℝ, 0 < ε → ε < 1 → ∀ δ : ℝ, 0 < δ → ∃ N : ℕ, ∀ n ≥ N,
    ∃ M : ℕ, (M : ℝ) ≤ (2 : ℝ) ^ ((n : ℝ) * (R + δ)) ∧ ∃ c : SourceCode α n M, c.errorProb p ≤ ε

end WildeQIT
Source
Wilde, Quantum Information Theory 2nd ed. (Cambridge 2017; arXiv:1106.1445v8), Theorem 14.4.1, §Application: Data Compression (roster-items.csv line 25241); the notions '(n,R) source code', 'error probability' and 'achievable rate' from the prose of §14.4 preceding it.

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