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Partial trace TrB{XAB}\mathrm{Tr}_B\{X_{AB}\}TrB​{XAB​} and TrA{XAB}\mathrm{Tr}_A\{X_{AB}\}TrA​{XAB​}

Definition
WildeQIT_partialTrace

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

partial-tracequantum-informationwilde-qit

Definition 4.3.4 (Partial Trace). Let XABX_{AB}XAB​ be a square operator acting on a tensor product Hilbert space HA⊗HB\mathcal{H}_A \otimes \mathcal{H}_BHA​⊗HB​, and let {∣l⟩B}\{|l\rangle_B\}{∣l⟩B​} be an orthonormal basis for HB\mathcal{H}_BHB​. Then the partial trace over the Hilbert space HB\mathcal{H}_BHB​ is defined as

TrB{XAB}≡∑l(IA⊗⟨l∣B)XAB(IA⊗∣l⟩B).\mathrm{Tr}_B\{X_{AB}\} \equiv \sum_l \left(I_A \otimes \langle l|_B\right) X_{AB} \left(I_A \otimes |l\rangle_B\right) .TrB​{XAB​}≡l∑​(IA​⊗⟨l∣B​)XAB​(IA​⊗∣l⟩B​).

Symmetrically, TrA{XAB}≡∑i(⟨i∣A⊗IB)XAB(∣i⟩A⊗IB)\mathrm{Tr}_A\{X_{AB}\} \equiv \sum_i (\langle i|_A \otimes I_B) X_{AB} (|i\rangle_A \otimes I_B)TrA​{XAB​}≡∑i​(⟨i∣A​⊗IB​)XAB​(∣i⟩A​⊗IB​) for an orthonormal basis {∣i⟩A}\{|i\rangle_A\}{∣i⟩A​} of HA\mathcal{H}_AHA​. The partial trace produces the local (reduced) density operator ρA=TrB{ρAB}\rho_A = \mathrm{Tr}_B\{\rho_{AB}\}ρA​=TrB​{ρAB​} of a bipartite state, and is the operation under which the trace distance is monotone (Corollary 9.1.2).

Formalization Note. A bipartite operator is a matrix X : Matrix (a × b) (a × b) ℂ indexed by the product type (Mathlib's Kronecker convention ⊗ₖ), and the orthonormal basis {∣l⟩B}\{|l\rangle_B\}{∣l⟩B​} is the standard basis of b. Then WildeQIT.partialTraceRight X : Matrix a a ℂ is TrB{X}\mathrm{Tr}_B\{X\}TrB​{X} with entries (TrBX)i,j=∑kX(i,k),(j,k)(\mathrm{Tr}_B X)_{i,j} = \sum_{k} X_{(i,k),(j,k)}(TrB​X)i,j​=∑k​X(i,k),(j,k)​, and WildeQIT.partialTraceLeft X : Matrix b b ℂ is TrA{X}\mathrm{Tr}_A\{X\}TrA​{X} with entries (TrAX)k,l=∑iX(i,k),(i,l)(\mathrm{Tr}_A X)_{k,l} = \sum_{i} X_{(i,k),(i,l)}(TrA​X)k,l​=∑i​X(i,k),(i,l)​. Only the traced-out factor is required to be finite.

Definition code
import Mathlib.LinearAlgebra.Matrix.Trace
import Mathlib.LinearAlgebra.Matrix.Kronecker
import Mathlib.Data.Complex.Basic

/-!
Wilde, *Quantum Information Theory* (2nd ed.), §4.3.4, Definition 4.3.4 (Partial Trace).

"Let `X_{AB}` be a square operator acting on a tensor product Hilbert space `ℋ_A ⊗ ℋ_B`, and let
`{|l⟩_B}` be an orthonormal basis for `ℋ_B`. Then the partial trace over the Hilbert space `ℋ_B`
is defined as `Tr_B{X_{AB}} ≡ ∑_l (I_A ⊗ ⟨l|_B) X_{AB} (I_A ⊗ |l⟩_B)`."

A bipartite operator is a matrix indexed by the product type `a × b` (the Kronecker convention
of Mathlib's `⊗ₖ`), and the orthonormal basis `{|l⟩_B}` is the standard basis of `b`.
-/

namespace WildeQIT

/-- **Definition 4.3.4 (Partial Trace over the right factor `B`).** For
`X : Matrix (a × b) (a × b) ℂ`, `Tr_B{X}` is the `a × a` matrix with entries
`(Tr_B X)ᵢⱼ = ∑ₖ X₍ᵢ,ₖ₎,₍ⱼ,ₖ₎`. -/
def partialTraceRight {a b : Type} [Fintype b] (X : Matrix (a × b) (a × b) ℂ) : Matrix a a ℂ :=
  Matrix.of fun i j => ∑ k, X (i, k) (j, k)

/-- **Definition 4.3.4 (Partial Trace over the left factor `A`).** For
`X : Matrix (a × b) (a × b) ℂ`, `Tr_A{X}` is the `b × b` matrix with entries
`(Tr_A X)ₖₗ = ∑ᵢ X₍ᵢ,ₖ₎,₍ᵢ,ₗ₎`. -/
def partialTraceLeft {a b : Type} [Fintype a] (X : Matrix (a × b) (a × b) ℂ) : Matrix b b ℂ :=
  Matrix.of fun k l => ∑ i, X (i, k) (i, l)

end WildeQIT
Source
Wilde, *Quantum Information Theory*, 2nd ed. (Cambridge University Press, 2017; arXiv:1106.1445v8), §4.3.4 "Local Density Operators and Partial Trace", Definition 4.3.4 (Partial Trace).

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