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Eq. (47), p. 554 — the tilted density maximises the Lagrangian; closed form of θ(λ₀, λ)

Proved
WorstCaseVaR.Entropy.dual_function_closed_form

by mikedeng1 · Sep 27, 2026 · Mathlib 0df444a (Lean v4.33.1)

lagrangian-dualityp2o-batch-p100bp2o-gran-per-chapterp2o-plan-paperp2o-v1relative-entropyvalue-at-risk

Let P0=N(x^,Γ)P_0 = \mathcal N(\hat x, \Gamma)P0​=N(x^,Γ) with Γ≻0\Gamma \succ 0Γ≻0, let w∈Rnw \in \mathbb R^nw∈Rn, γ,d,λ0∈R\gamma, d, \lambda_0 \in \mathbb Rγ,d,λ0​∈R and λ>0\lambda > 0λ>0, and write S={x:γ≤−x⊤w}\mathcal S = \{x : \gamma \le -x^\top w\}S={x:γ≤−x⊤w} with indicator χS\chi_{\mathcal S}χS​. Call a measure QQQ on Rn\mathbb R^nRn admissible if it is finite, Q≪P0Q \ll P_0Q≪P0​, and log⁡dQdP0\log\frac{dQ}{dP_0}logdP0​dQ​ is QQQ-integrable (a density of finite relative entropy). For admissible QQQ define the Lagrangian

L(Q)=Q(S)+λ0(1−Q(Rn))+λ(d−∫log⁡dQdP0 dQ).L(Q) = Q(\mathcal S) + \lambda_0\big(1 - Q(\mathbb R^n)\big) + \lambda\Big(d - \int \log\frac{dQ}{dP_0}\,dQ\Big).L(Q)=Q(S)+λ0​(1−Q(Rn))+λ(d−∫logdP0​dQ​dQ).

Let Q⋆Q^\starQ⋆ be the measure with density dQ⋆dP0(x)=exp⁡ ⁣(χS(x)−λ0λ−1)\dfrac{dQ^\star}{dP_0}(x) = \exp\!\Big(\dfrac{\chi_{\mathcal S}(x) - \lambda_0}{\lambda} - 1\Big)dP0​dQ⋆​(x)=exp(λχS​(x)−λ0​​−1) (Eq. 47), and

θ(λ0,λ)=λ0+λd+λe−λ0/λ−1((e1/λ−1)P0(S)+1).\theta(\lambda_0,\lambda) = \lambda_0 + \lambda d + \lambda e^{-\lambda_0/\lambda - 1}\big((e^{1/\lambda} - 1)P_0(\mathcal S) + 1\big).θ(λ0​,λ)=λ0​+λd+λe−λ0​/λ−1((e1/λ−1)P0​(S)+1).

Then:

  1. Q⋆Q^\starQ⋆ is admissible and L(Q⋆)=θ(λ0,λ)L(Q^\star) = \theta(\lambda_0,\lambda)L(Q⋆)=θ(λ0​,λ);
  2. L(Q)≤θ(λ0,λ)L(Q) \le \theta(\lambda_0,\lambda)L(Q)≤θ(λ0​,λ) for every admissible QQQ;
  3. λ0+λd+λ∫exp⁡ ⁣(χS(x)−λ0λ−1) dP0(x)=θ(λ0,λ)\lambda_0 + \lambda d + \lambda \displaystyle\int \exp\!\Big(\frac{\chi_{\mathcal S}(x) - \lambda_0}{\lambda} - 1\Big)\,dP_0(x) = \theta(\lambda_0,\lambda)λ0​+λd+λ∫exp(λχS​(x)−λ0​​−1)dP0​(x)=θ(λ0​,λ).

So the dual function θ(λ0,λ)=sup⁡QL(Q)\theta(\lambda_0,\lambda) = \sup_Q L(Q)θ(λ0​,λ)=supQ​L(Q) of the worst-case probability problem (46) is attained at the exponentially tilted density (47) and has the stated closed form.

Formalization Note The paper writes densities p,p0p, p_0p,p0​; here QQQ is a finite measure and log⁡dQdP0\log\frac{dQ}{dP_0}logdP0​dQ​ is Mathlib's log-likelihood ratio llr Q P₀. The paper's second line splits the integral over {γ≤−x⊤w}\{\gamma \le -x^\top w\}{γ≤−x⊤w} and {γ≥−x⊤w}\{\gamma \ge -x^\top w\}{γ≥−x⊤w}, which overlap on a hyperplane; the Lean statement uses P0(S)P_0(\mathcal S)P0​(S) and its complement directly, so no null-set argument is needed.

Preamble
import Mathlib
import Definitions.Def_WorstCaseVaR_Entropy_Basic

open MeasureTheory
Formal statement
namespace WorstCaseVaR.Entropy

/-- Eq. (47) and the closed form of the dual function, p. 554. Fix `λ > 0` and `λ₀ ∈ ℝ`, and
let `𝒮 = {x | γ ≤ -xᵀw}`. Over finite measures `Q ≪ P₀` with `P₀`-log-likelihood ratio
integrable against `Q` (densities `p` of finite relative entropy), the Lagrangian
`L(Q) = Q(𝒮) + λ₀(1 - Q(ℝⁿ)) + λ(d - ∫ log(dQ/dP₀) dQ)` is maximised by the tilted measure
`dQ*/dP₀ = exp((χ_𝒮 - λ₀)/λ - 1)`, and its maximum is
`λ₀ + λd + λ∫ exp((χ_𝒮 - λ₀)/λ - 1) dP₀ = λ₀ + λd + λe^{-λ₀/λ-1}((e^{1/λ} - 1)P₀(𝒮) + 1)`. -/
theorem dual_function_closed_form {n : ℕ} (xhat w : Returns n) (Γ : Matrix (Fin n) (Fin n) ℝ)
    (hΓ : Γ.PosDef) (d γ lam0 lam : ℝ) (hlam : 0 < lam) :
    let P₀ := refGaussian xhat Γ
    let S := lossSet w γ
    let L : Measure (Returns n) → ℝ := fun Q =>
      Q.real S + lam0 * (1 - Q.real Set.univ) + lam * (d - ∫ x, llr Q P₀ x ∂Q)
    let Admissible : Measure (Returns n) → Prop := fun Q =>
      IsFiniteMeasure Q ∧ Q ≪ P₀ ∧ Integrable (llr Q P₀) Q
    let Qstar : Measure (Returns n) :=
      P₀.withDensity fun x => ENNReal.ofReal (Real.exp ((S.indicator 1 x - lam0) / lam - 1))
    let θ : ℝ := lam0 + lam * d +
      lam * Real.exp (-(lam0 / lam) - 1) * ((Real.exp (1 / lam) - 1) * P₀.real S + 1)
    Admissible Qstar ∧ L Qstar = θ ∧ (∀ Q, Admissible Q → L Q ≤ θ) ∧
      lam0 + lam * d + lam * ∫ x, Real.exp ((S.indicator 1 x - lam0) / lam - 1) ∂P₀ = θ := by sorry

end WorstCaseVaR.Entropy
Source
El Ghaoui, Oks and Oustry, Worst-Case Value-at-Risk and Robust Portfolio Optimization: A Conic Programming Approach, Oper. Res. 51 (2003), p. 554, proof of Theorem 9, Eq. (47) and the display following it
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What the Lean code literally says, in plain math · claude-opus-5-5

Setting. Let n∈Nn\in\mathbb Nn∈N and let x^,w∈Rn\hat x,w\in\mathbb R^nx^,w∈Rn. Let Γ\GammaΓ be a positive definite real n×nn\times nn×n matrix. Let d,γ,λ0,λd,\gamma,\lambda_0,\lambdad,γ,λ0​,λ be real numbers with λ>0\lambda>0λ>0. No condition is placed on www, ddd, γ\gammaγ or λ0\lambda_0λ0​. Set:

  • P0P_0P0​: the library's multivariate Gaussian with mean x^\hat xx^ and covariance Γ\GammaΓ;
  • S={x:γ≤−⟨x,w⟩}\mathcal S=\{x:\gamma\le-\langle x,w\rangle\}S={x:γ≤−⟨x,w⟩};
  • ℓQ(x)=log⁡(dQdP0(x))\ell_Q(x)=\log\big(\tfrac{dQ}{dP_0}(x)\big)ℓQ​(x)=log(dP0​dQ​(x)): the log-likelihood ratio. The Radon–Nikodym derivative is converted to a real number, with ∞↦0\infty\mapsto0∞↦0, and log⁡0=0\log 0=0log0=0.

For a measure QQQ on Rn\mathbb R^nRn define

L(Q)=Q(S)+λ0(1−Q(Rn))+λ(d−∫ℓQ dQ).L(Q)=Q(\mathcal S)+\lambda_0\big(1-Q(\mathbb R^n)\big)+\lambda\Big(d-\int\ell_Q\,dQ\Big).L(Q)=Q(S)+λ0​(1−Q(Rn))+λ(d−∫ℓQ​dQ).

The measures are taken as real numbers. The integral is the Lebesgue/Bochner integral, which is 000 for non-integrable integrands.

Call QQQ admissible if all three of these hold:

  1. QQQ is a finite measure;
  2. Q≪P0Q\ll P_0Q≪P0​;
  3. ℓQ\ell_QℓQ​ is QQQ-integrable.

Let Q∗Q^*Q∗ be the measure with density x↦exp⁡ ⁣((1S(x)−λ0)/λ−1)x\mapsto\exp\!\big((\mathbf 1_{\mathcal S}(x)-\lambda_0)/\lambda-1\big)x↦exp((1S​(x)−λ0​)/λ−1) with respect to P0P_0P0​, and let

θ=λ0+λd+λ e−λ0/λ−1((e1/λ−1) P0(S)+1).\theta=\lambda_0+\lambda d+\lambda\,e^{-\lambda_0/\lambda-1}\big((e^{1/\lambda}-1)\,P_0(\mathcal S)+1\big).θ=λ0​+λd+λe−λ0​/λ−1((e1/λ−1)P0​(S)+1).

Conclusion. All four of the following hold:

  1. Q∗Q^*Q∗ is admissible.
  2. L(Q∗)=θL(Q^*)=\thetaL(Q∗)=θ.
  3. Every admissible QQQ satisfies L(Q)≤θL(Q)\le\thetaL(Q)≤θ.
  4. The integral form agrees with θ\thetaθ:
λ0+λd+λ∫e(1S(x)−λ0)/λ−1 dP0(x)=θ.\lambda_0+\lambda d+\lambda\int e^{(\mathbf 1_{\mathcal S}(x)-\lambda_0)/\lambda-1}\,dP_0(x)=\theta.λ0​+λd+λ∫e(1S​(x)−λ0​)/λ−1dP0​(x)=θ.

Degenerate cases.

  • Zero measure. Q=0Q=0Q=0 is admissible and has L(0)=λ0+λdL(0)=\lambda_0+\lambda dL(0)=λ0​+λd, so claim 3 includes λ0+λd≤θ\lambda_0+\lambda d\le\thetaλ0​+λd≤θ.
  • w=0w=0w=0. This is allowed. S\mathcal SS is all of Rn\mathbb R^nRn if γ≤0\gamma\le0γ≤0 and empty if γ>0\gamma>0γ>0, and the same holds for any www when n=0n=0n=0.
  • n=0n=0n=0. R0\mathbb R^0R0 is one point, and Γ\GammaΓ is the empty matrix, which is positive definite.
  • Integral convention. The integral in claim 4 uses the convention that a non-integrable integrand has integral 000.
Human review
  • Endorsed by Shuze Chen · Sep 27, 2026

    Confirmed by the moderator at approval.

  • Endorsed by mikedeng1 · Sep 27, 2026

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

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