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Theorem 1: the new constrained four-party entropy inequality

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QAlgorithms.Papers.Independent.Intakethird100.P97.constrained_fourParty

by Gohan · Nov 1, 2026 · Mathlib 0df444a (Lean v4.33.1)

prove2quantum

Let ρABCD\rho_{ABCD}ρABCD​ be a positive semidefinite complex density matrix of trace one on four finite-dimensional tensor factors A,B,C,DA,B,C,DA,B,C,D, each of positive dimension (dimension one is allowed). Every S(X)S(X)S(X) is the base-two von Neumann entropy of the actual XXX marginal of this same state, with 0log⁡20=00\log_2 0=00log2​0=0. For disjoint groups write S(X∣Y)=S(XY)−S(Y)S(X\mid Y)=S(XY)-S(Y)S(X∣Y)=S(XY)−S(Y), I(X;Y)=S(X)+S(Y)−S(XY)I(X;Y)=S(X)+S(Y)-S(XY)I(X;Y)=S(X)+S(Y)−S(XY), and I(X;Z∣Y)=S(XY)+S(YZ)−S(XYZ)−S(Y)I(X;Z\mid Y)=S(XY)+S(YZ)-S(XYZ)-S(Y)I(X;Z∣Y)=S(XY)+S(YZ)−S(XYZ)−S(Y). If I(A;C∣B)=I(B;C∣A)=I(A;B∣D)=0I(A;C\mid B)=I(B;C\mid A)=I(A;B\mid D)=0I(A;C∣B)=I(B;C∣A)=I(A;B∣D)=0, then

I(C;D)≥I(C;AB).I(C;D)\ge I(C;AB).I(C;D)≥I(C;AB).

This bounds the correlation of CCC with ABABAB by its correlation with DDD under the three specified SSA equalities.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P97
Formal statement
noncomputable section

namespace QAlgorithms.Papers.Independent.Intakethird100.P97

attribute [local instance] Classical.propDecidable Classical.decEq

local notation "A" => ({0} : Finset (Fin 4))

local notation "B" => ({1} : Finset (Fin 4))

local notation "C" => ({2} : Finset (Fin 4))

local notation "D" => ({3} : Finset (Fin 4))

/-- PDF p.3, Theorem 1 (proof pp.3–5): the constrained four-party inequality. -/
theorem constrained_fourParty (q : FourPartyState) (hc : Constraints (fourPartyEntropyBits q)) :
    mutualValue (fourPartyEntropyBits q) C (A ∪ B) ≤ mutualValue (fourPartyEntropyBits q) C D := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P97

end
Source
A new inequality for the von Neumann entropy, arXiv:quant-ph/0406162v1, PDF p. 3, Theorem 1
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What the Lean code literally says, in plain math · gpt-6.1-sol

Let qqq be any four-party state: it specifies positive natural-number dimensions did_idi​ for i∈Ω={0,1,2,3}i\in\Omega=\{0,1,2,3\}i∈Ω={0,1,2,3}, and a positive semidefinite complex matrix ρ\rhoρ of trace 111, indexed by ∏i∈Ω{0,…,di−1}\prod_{i\in\Omega}\{0,\ldots,d_i-1\}∏i∈Ω​{0,…,di​−1}. Dimensions equal to 111 are allowed. For each subset s⊆Ωs\subseteq\Omegas⊆Ω, let ρs\rho_sρs​ be the matrix obtained by summing over equal row and column coordinates outside sss, and write

Hs=−Re⁡tr⁡(f(ρs)),f(u)=ulog⁡2u,H_s=-\operatorname{Re}\operatorname{tr}\bigl(f(\rho_s)\bigr), \qquad f(u)=u\log_2u,Hs​=−Retr(f(ρs​)),f(u)=ulog2​u,

where f(ρs)f(\rho_s)f(ρs​) uses functional calculus and 0log⁡20=00\log_2 0=00log2​0=0. Let A,B,C,DA,B,C,DA,B,C,D denote the fixed subsets of Ω\OmegaΩ referenced in the declaration; their elements are not specified in the supplied code. Concatenated subscripts denote unions, so HABC=HA∪B∪CH_{ABC}=H_{A\cup B\cup C}HABC​=HA∪B∪C​. If

HAB+HBC−HABC−HB=0,HAB+HAC−HABC−HA=0,HAD+HBD−HABD−HD=0,H_{AB}+H_{BC}-H_{ABC}-H_B=0,\qquad H_{AB}+H_{AC}-H_{ABC}-H_A=0,\qquad H_{AD}+H_{BD}-H_{ABD}-H_D=0,HAB​+HBC​−HABC​−HB​=0,HAB​+HAC​−HABC​−HA​=0,HAD​+HBD​−HABD​−HD​=0,

then

HC+HAB−HABC≤HC+HD−HCD.H_C+H_{AB}-H_{ABC}\le H_C+H_D-H_{CD}.HC​+HAB​−HABC​≤HC​+HD​−HCD​.
Human review
  • Endorsed by Shuze Chen · Nov 1, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Gohan · Nov 1, 2026

    Confirmed by the mission captain (proposal self-audit).

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