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M06 — Frozen-input differentiation

Proved
VathekProof.M06_frozen_input_gradient

by ajax · Sep 22, 2026 · Mathlib 0df444a (Lean v4.33.1)

formal-verificationgradient-descentmachine-learning

Two facts about frozen components.

(i) The chain derivative through a frozen component's input survives. Take the concrete graft of the source: a trainable bridge w↦3ww \mapsto 3ww↦3w grafted into a frozen donor u↦2uu \mapsto 2uu↦2u, with loss 12∥u−1∥2\tfrac{1}{2}\|u - 1\|^221​∥u−1∥2 evaluated at w0=2w_0 = 2w0​=2. The composite w↦12∥2⋅(3w)−1∥2=12(6w−1)2w \mapsto \tfrac{1}{2}\|2 \cdot (3w) - 1\|^2 = \tfrac{1}{2}(6w - 1)^2w↦21​∥2⋅(3w)−1∥2=21​(6w−1)2 has gradient 6(6⋅2−1)=66≠06(6 \cdot 2 - 1) = 66 \neq 06(6⋅2−1)=66=0 at w0w_0w0​: freezing the donor's parameters does not remove the derivative through its input (detaching that input would falsely give 000).

(ii) The declared masked update preserves frozen coordinates. For the masked AdamW instance with 0≤β1,β2<10 \le \beta_1, \beta_2 < 10≤β1​,β2​<1, ε>0\varepsilon > 0ε>0, and nonnegative incoming second moments: every frozen coordinate (j∉Tj \notin Tj∈/T) of www is unchanged by the update, second moments stay nonnegative, and the update denominator v^j+ε\sqrt{\hat v_j} + \varepsilonv^j​​+ε is strictly positive — properties of this declared masked update, not of an arbitrary update function.

Preamble
import Definitions.Def_VathekFrame
import Definitions.Def_VathekState
import Definitions.Def_VathekAdamW
import Definitions.Def_VathekWitness
Formal statement
namespace VathekProof

/-- **M06 — Frozen-input differentiation.**  (i) The §5.3 chain instance: a trainable
bridge `w ↦ 3w` grafted into a *frozen* donor `u ↦ 2u`, with loss `½‖u - 1‖²` at
`w₀ = 2`, has the nonzero gradient `66` — freezing the donor's parameters does not
remove the chain derivative through its input (detaching that input would instead
falsely give `0`).  (ii) For the declared masked AdamW update: frozen coordinates are
preserved untouched, nonnegative second moments stay nonnegative, and the update
denominator `√v̂ + ε` is strictly positive — properties of this declared masked
update, not of an arbitrary update function. -/
theorem M06_frozen_input_gradient :
    HasGradientAt
      (fun (w : EuclideanSpace ℝ (Fin 1)) =>
        (1 / 2) * ‖(2 : ℝ) • ((3 : ℝ) • w) - WithLp.toLp 2 (fun _ => (1 : ℝ))‖ ^ 2)
      (WithLp.toLp 2 (fun _ => (66 : ℝ)))
      (WithLp.toLp 2 (fun _ => (2 : ℝ)))
    ∧ (WithLp.toLp 2 (fun _ => (66 : ℝ)) : EuclideanSpace ℝ (Fin 1)) ≠ 0
    ∧ ∀ (d : ℕ) (β₁ β₂ η lam ε : ℝ) (T : Finset (Fin d)) (S : TrainState d)
        (g : EuclideanSpace ℝ (Fin d)),
        0 ≤ β₁ → β₁ < 1 → 0 ≤ β₂ → β₂ < 1 → 0 < ε → (∀ j, 0 ≤ S.mom2 j) →
        (∀ j ∉ T, (adamWStep β₁ β₂ η lam ε T S g).w j = S.w j)
        ∧ (∀ j, 0 ≤ (adamWStep β₁ β₂ η lam ε T S g).mom2 j)
        ∧ ∀ j, 0 < Real.sqrt (adamM2 β₂ S g j / (1 - β₂ ^ (S.t + 1))) + ε := by sorry

end VathekProof
Source
Vathek Graft: A Proof and Evidence Programme, mission-source white paper v1.0, 22 September 2026 (Thomas Davis). Section 5.3 (witness), Section 6 milestone M06, and Appendix A.
Read-back

What the Lean code literally says, in plain math · glm-5.3 (independent auditor subagent)

{"text": "{\n "readback": "The theorem M06_frozen_input_gradient asserts a conjunction of three statements.\n\nFirst conjunct \u2014 the concrete gradient claim. Let W=mathrmEuclideanSpacemathbbR(mathrmFin1)W = \\\\mathrm{EuclideanSpace}\\\\ \\\\mathbb{R}\\\\ (\\\\mathrm{Fin}\\\\ 1)W=mathrmEuclideanSpacemathbbR(mathrmFin1), the one-coordinate Euclidean space (vectors are written via the identification mathrmWithLp.toLp2\\\\mathrm{WithLp.toLp}\\\\ 2mathrmWithLp.toLp2, which packages a coordinate function as an L2L^2L2-typed vector; e.g. \\\\mathrm{WithLp.toLp}\\\\ 2\\\\ (\\\\lambda \\\\_ \\\\mapsto 2) is the constant vector w0=(2)w_0 = (2)w0​=(2)). The claim is that the function\n\n

F(w)=tfrac12,bigl∣,2cdot(3w)−mathbf1,bigr∣2,F(w) = \\\\tfrac{1}{2}\\\\,\\\\bigl\\\\|\\\\, 2 \\\\cdot (3w) - \\\\mathbf{1} \\\\,\\\\bigr\\\\|^2,F(w)=tfrac12,bigl∣,2cdot(3w)−mathbf1,bigr∣2,

\n\nwhere ∣cdot∣\\\\|\\\\cdot\\\\|∣cdot∣ is the Euclidean norm on the one-coordinate space and mathbf1=(1)\\\\mathbf{1} = (1)mathbf1=(1) is the constant vector 111, has gradient at the point w0=(2)w_0 = (2)w0​=(2) equal to the constant vector (66)(66)(66). Here HasGradientAt is the standard Fr\u00e9chet-gradient notion: F(w)=F(w0)+langle(66),,w−w0rangle+o(∣w−w0∣)F(w) = F(w_0) + \\\\langle (66),\\\\, w - w_0\\\\rangle + o(\\\\|w - w_0\\\\|)F(w)=F(w0​)+langle(66),,w−w0​rangle+o(∣w−w0​∣) as wtow0w \\\\to w_0wtow0​. Concretely F(w)=tfrac12(6w−1)2F(w) = \\\\tfrac12(6w - 1)^2F(w)=tfrac12(6w−1)2 on the single coordinate, so the assertion is the literal numerical statement nablaF(2)=66\\\\nabla F(2) = 66nablaF(2)=66. Note that 2cdot(3w)2\\\\cdot(3w)2cdot(3w) is the composition of scaling by 333 with scaling by 222 (i.e. 6w6w6w); the norm and squaring are the Euclidean ones.\n\nSecond conjunct \u2014 nonzeroness. The constant vector (66)inmathrmEuclideanSpacemathbbR(mathrmFin1)(66) \\\\in \\\\mathrm{EuclideanSpace}\\\\ \\\\mathbb{R}\\\\ (\\\\mathrm{Fin}\\\\ 1)(66)inmathrmEuclideanSpacemathbbR(mathrmFin1) is not the zero vector. This is a bare inequality; combined with the first conjunct it says the gradient in question is nonzero, but the conjunct itself asserts only (66)neq0(66) \\\\neq 0(66)neq0.\n\nThird conjunct \u2014 the universally quantified AdamW clause. For every natural number ddd, real numbers beta1,beta2,eta,lambda,varepsilon\\\\beta_1, \\\\beta_2, \\\\eta, \\\\lambda, \\\\varepsilonbeta1​,beta2​,eta,lambda,varepsilon, finite set TsubseteqmathrmFindT \\\\subseteq \\\\mathrm{Fin}\\\\ dTsubseteqmathrmFind of trainable coordinates, training state SSS, and gradient vector ginmathrmEuclideanSpacemathbbR(mathrmFind)g \\\\in \\\\mathrm{EuclideanSpace}\\\\ \\\\mathbb{R}\\\\ (\\\\mathrm{Fin}\\\\ d)ginmathrmEuclideanSpacemathbbR(mathrmFind), assuming:\n\n- 0lebeta10 \\\\le \\\\beta_10lebeta1​ and beta1<1\\\\beta_1 < 1beta1​<1;\n- 0lebeta20 \\\\le \\\\beta_20lebeta2​ and beta2<1\\\\beta_2 < 1beta2​<1;\n- 0<varepsilon0 < \\\\varepsilon0<varepsilon;\n- every second-moment slot of SSS is nonnegative: 0leSmathrmmom2(j)0 \\\\le S_{\\\\mathrm{mom2}}(j)0leSmathrmmom2​(j) for all coordinates jjj;\n\nit concludes all three of the following about the state S′=mathrmadamWStepbeta1beta2etalambdavarepsilonTSgS' = \\\\mathrm{adamWStep}\\\\ \\\\beta_1\\\\ \\\\beta_2\\\\ \\\\eta\\\\ \\\\lambda\\\\ \\\\varepsilon\\\\ T\\\\ S\\\\ gS′=mathrmadamWStepbeta1​beta2​etalambdavarepsilonTSg, where the masked AdamW transition is defined coordinatewise by\n\n

\\nm'_j &= \\\\beta_1\\\\, S_{\\\\mathrm{mom1}}(j) + (1 - \\\\beta_1)\\\\, g_j &&\\\\text{(first moment, } \\\\mathrm{adamM1}\\\\text{)},\\\\\\\\\\nv'_j &= \\\\beta_2\\\\, S_{\\\\mathrm{mom2}}(j) + (1 - \\\\beta_2)\\\\, g_j^2 &&\\\\text{(second moment, } \\\\mathrm{adamM2}\\\\text{)},\\\\\\\\\\nS'_w(j) &= \\\\begin{cases}\\n(1 - \\\\eta\\\\lambda)\\\\, S_w(j) \\\\;-\\\\; \\\\eta\\\\,\\\\dfrac{m'_j / (1 - \\\\beta_1^{\\\\,S_t + 1})}{\\\\sqrt{v'_j / (1 - \\\\beta_2^{\\\\,S_t + 1})} + \\\\varepsilon}, & j \\\\in T,\\\\\\\\[2ex]\\nS_w(j), & j \\\\notin T,\\n\\\\end{cases}\\\\\\\\\\nS'_t &= S_t + 1,\\n

\n\nwith Sw,Smathrmmom1,Smathrmmom2S_w, S_{\\\\mathrm{mom1}}, S_{\\\\mathrm{mom2}}Sw​,Smathrmmom1​,Smathrmmom2​ the parameter, first-moment, and second-moment vectors of SSS and StinmathbbNS_t \\\\in \\\\mathbb{N}St​inmathbbN its step counter:\n\n1. Frozen coordinates preserved: for every coordinate jnotinTj \\\\notin TjnotinT, the updated parameter equals the old one, Sw′(j)=Sw(j)S'_w(j) = S_w(j)Sw′​(j)=Sw​(j);\n2. Second moments stay nonnegative: 0leSmathrmmom2′(j)=vj′0 \\\\le S'_{\\\\mathrm{mom2}}(j) = v'_j0leSmathrmmom2′​(j)=vj′​ for every jjj;\n3. Denominator positivity: for every jjj, 0<sqrt,vj′/(1−beta2,St+1)+varepsilon0 < \\\\sqrt{\\\\,v'_j / (1 - \\\\beta_2^{\\\\,S_t + 1})} + \\\\varepsilon0<sqrt,vj′​/(1−beta2,St​+1​)+varepsilon, where the square root is the real square root.\n\nEdge cases and fine print. The hypotheses 0lebeta1<10 \\\\le \\\\beta_1 < 10lebeta1​<1 and 0lebeta2<10 \\\\le \\\\beta_2 < 10lebeta2​<1 make the bias-correction denominators 1−beta1St+11 - \\\\beta_1^{S_t+1}1−beta1St​+1​ and 1−beta2St+11 - \\\\beta_2^{S_t+1}1−beta2St​+1​ positive (so no division by zero there), and together with 0leSmathrmmom2(j)0 \\\\le S_{\\\\mathrm{mom2}}(j)0leSmathrmmom2​(j) they make vj′ge0v'_j \\\\ge 0vj′​ge0; the third conclusion's strict positivity then rests on varepsilon>0\\\\varepsilon > 0varepsilon>0 (it forces the denominator strictly positive even when vj′=0v'_j = 0vj′​=0). No sign or size restrictions are placed on eta\\\\etaeta or lambda\\\\lambdalambda (the learning rate and weight-decay coefficient appear only in the trainable-branch formula and are otherwise unconstrained), nor on ggg or Smathrmmom1S_{\\\\mathrm{mom1}}Smathrmmom1​. The quantification includes the degenerate cases d=0d = 0d=0 (empty coordinate set, all three conclusions vacuous coordinatewise) and TTT empty (then conclusion 1 says all coordinates of www are unchanged) or TTT full. No conclusion is drawn about the trainable-branch coordinates of Sw′S'_wSw′​, about Smathrmmom1′S'_{\\\\mathrm{mom1}}Smathrmmom1′​, or about the step counter beyond its increment as part of the definition. Conclusion 3 concerns the same denominator expression used inside the trainable branch of the update, with vj′v'_jvj′​ computed from the pre-update state SSS."\n}", "details": {"resolvedPath": "/home/ajax/.omp/agent/sessions/-math/2026-09-22T19-31-08-510Z_01a0ca99-be5e-7000-93c6-dac7c74cc004/RB-M06.md", "contentType": "text/markdown", "totalLines": 3, "displayContent": {"text": "{\n "readback": "The theorem M06_frozen_input_gradient asserts a conjunction of three statements.\n\nFirst conjunct \u2014 the concrete gradient claim. Let W=mathrmEuclideanSpacemathbbR(mathrmFin1)W = \\\\mathrm{EuclideanSpace}\\\\ \\\\mathbb{R}\\\\ (\\\\mathrm{Fin}\\\\ 1)W=mathrmEuclideanSpacemathbbR(mathrmFin1), the one-coordinate Euclidean space (vectors are written via the identification mathrmWithLp.toLp2\\\\mathrm{WithLp.toLp}\\\\ 2mathrmWithLp.toLp2, which packages a coordinate function as an L2L^2L2-typed vector; e.g. \\\\mathrm{WithLp.toLp}\\\\ 2\\\\ (\\\\lambda \\\\_ \\\\mapsto 2) is the constant vector w0=(2)w_0 = (2)w0​=(2)). The claim is that the function\n\n

F(w)=tfrac12,bigl∣,2cdot(3w)−mathbf1,bigr∣2,F(w) = \\\\tfrac{1}{2}\\\\,\\\\bigl\\\\|\\\\, 2 \\\\cdot (3w) - \\\\mathbf{1} \\\\,\\\\bigr\\\\|^2,F(w)=tfrac12,bigl∣,2cdot(3w)−mathbf1,bigr∣2,

\n\nwhere ∣cdot∣\\\\|\\\\cdot\\\\|∣cdot∣ is the Euclidean norm on the one-coordinate space and mathbf1=(1)\\\\mathbf{1} = (1)mathbf1=(1) is the constant vector 111, has gradient at the point w0=(2)w_0 = (2)w0​=(2) equal to the constant vector (66)(66)(66). Here HasGradientAt is the standard Fr\u00e9chet-gradient notion: F(w)=F(w0)+langle(66),,w−w0rangle+o(∣w−w0∣)F(w) = F(w_0) + \\\\langle (66),\\\\, w - w_0\\\\rangle + o(\\\\|w - w_0\\\\|)F(w)=F(w0​)+langle(66),,w−w0​rangle+o(∣w−w0​∣) as wtow0w \\\\to w_0wtow0​. Concretely F(w)=tfrac12(6w−1)2F(w) = \\\\tfrac12(6w - 1)^2F(w)=tfrac12(6w−1)2 on the single coordinate, so the assertion is the literal numerical statement nablaF(2)=66\\\\nabla F(2) = 66nablaF(2)=66. Note that 2cdot(3w)2\\\\cdot(3w)2cdot(3w) is the composition of scaling by 333 with scaling by 222 (i.e. 6w6w6w); the norm and squaring are the Euclidean ones.\n\nSecond conjunct \u2014 nonzeroness. The constant vector (66)inmathrmEuclideanSpacemathbbR(mathrmFin1)(66) \\\\in \\\\mathrm{EuclideanSpace}\\\\ \\\\mathbb{R}\\\\ (\\\\mathrm{Fin}\\\\ 1)(66)inmathrmEuclideanSpacemathbbR(mathrmFin1) is not the zero vector. This is a bare inequality; combined with the first conjunct it says the gradient in question is nonzero, but the conjunct itself asserts only (66)neq0(66) \\\\neq 0(66)neq0.\n\nThird conjunct \u2014 the universally quantified AdamW clause. For every natural number ddd, real numbers beta1,beta2,eta,lambda,varepsilon\\\\beta_1, \\\\beta_2, \\\\eta, \\\\lambda, \\\\varepsilonbeta1​,beta2​,eta,lambda,varepsilon, finite set TsubseteqmathrmFindT \\\\subseteq \\\\mathrm{Fin}\\\\ dTsubseteqmathrmFind of trainable coordinates, training state SSS, and gradient vector ginmathrmEuclideanSpacemathbbR(mathrmFind)g \\\\in \\\\mathrm{EuclideanSpace}\\\\ \\\\mathbb{R}\\\\ (\\\\mathrm{Fin}\\\\ d)ginmathrmEuclideanSpacemathbbR(mathrmFind), assuming:\n\n- 0lebeta10 \\\\le \\\\beta_10lebeta1​ and beta1<1\\\\beta_1 < 1beta1​<1;\n- 0lebeta20 \\\\le \\\\beta_20lebeta2​ and beta2<1\\\\beta_2 < 1beta2​<1;\n- 0<varepsilon0 < \\\\varepsilon0<varepsilon;\n- every second-moment slot of SSS is nonnegative: 0leSmathrmmom2(j)0 \\\\le S_{\\\\mathrm{mom2}}(j)0leSmathrmmom2​(j) for all coordinates jjj;\n\nit concludes all three of the following about the state S′=mathrmadamWStepbeta1beta2etalambdavarepsilonTSgS' = \\\\mathrm{adamWStep}\\\\ \\\\beta_1\\\\ \\\\beta_2\\\\ \\\\eta\\\\ \\\\lambda\\\\ \\\\varepsilon\\\\ T\\\\ S\\\\ gS′=mathrmadamWStepbeta1​beta2​etalambdavarepsilonTSg, where the masked AdamW transition is defined coordinatewise by\n\n

\\nm'_j &= \\\\beta_1\\\\, S_{\\\\mathrm{mom1}}(j) + (1 - \\\\beta_1)\\\\, g_j &&\\\\text{(first moment, } \\\\mathrm{adamM1}\\\\text{)},\\\\\\\\\\nv'_j &= \\\\beta_2\\\\, S_{\\\\mathrm{mom2}}(j) + (1 - \\\\beta_2)\\\\, g_j^2 &&\\\\text{(second moment, } \\\\mathrm{adamM2}\\\\text{)},\\\\\\\\\\nS'_w(j) &= \\\\begin{cases}\\n(1 - \\\\eta\\\\lambda)\\\\, S_w(j) \\\\;-\\\\; \\\\eta\\\\,\\\\dfrac{m'_j / (1 - \\\\beta_1^{\\\\,S_t + 1})}{\\\\sqrt{v'_j / (1 - \\\\beta_2^{\\\\,S_t + 1})} + \\\\varepsilon}, & j \\\\in T,\\\\\\\\[2ex]\\nS_w(j), & j \\\\notin T,\\n\\\\end{cases}\\\\\\\\\\nS'_t &= S_t + 1,\\n

\n\nwith Sw,Smathrmmom1,Smathrmmom2S_w, S_{\\\\mathrm{mom1}}, S_{\\\\mathrm{mom2}}Sw​,Smathrmmom1​,Smathrmmom2​ the parameter, first-moment, and second-moment vectors of SSS and StinmathbbNS_t \\\\in \\\\mathbb{N}St​inmathbbN its step counter:\n\n1. Frozen coordinates preserved: for every coordinate jnotinTj \\\\notin TjnotinT, the updated parameter equals the old one, Sw′(j)=Sw(j)S'_w(j) = S_w(j)Sw′​(j)=Sw​(j);\n2. Second moments stay nonnegative: 0leSmathrmmom2′(j)=vj′0 \\\\le S'_{\\\\mathrm{mom2}}(j) = v'_j0leSmathrmmom2′​(j)=vj′​ for every jjj;\n3. Denominator positivity: for every jjj, 0<sqrt,vj′/(1−beta2,St+1)+varepsilon0 < \\\\sqrt{\\\\,v'_j / (1 - \\\\beta_2^{\\\\,S_t + 1})} + \\\\varepsilon0<sqrt,vj′​/(1−beta2,St​+1​)+varepsilon, where the square root is the real square root.\n\nEdge cases and fine print. The hypotheses 0lebeta1<10 \\\\le \\\\beta_1 < 10lebeta1​<1 and 0lebeta2<10 \\\\le \\\\beta_2 < 10lebeta2​<1 make the bias-correction denominators 1−beta1St+11 - \\\\beta_1^{S_t+1}1−beta1St​+1​ and 1−beta2St+11 - \\\\beta_2^{S_t+1}1−beta2St​+1​ positive (so no division by zero there), and together with 0leSmathrmmom2(j)0 \\\\le S_{\\\\mathrm{mom2}}(j)0leSmathrmmom2​(j) they make vj′ge0v'_j \\\\ge 0vj′​ge0; the third conclusion's strict positivity then rests on varepsilon>0\\\\varepsilon > 0varepsilon>0 (it forces the denominator strictly positive even when vj′=0v'_j = 0vj′​=0). No sign or size restrictions are placed on eta\\\\etaeta or lambda\\\\lambdalambda (the learning rate and weight-decay coefficient appear only in the trainable-branch formula and are otherwise unconstrained), nor on ggg or Smathrmmom1S_{\\\\mathrm{mom1}}Smathrmmom1​. The quantification includes the degenerate cases d=0d = 0d=0 (empty coordinate set, all three conclusions vacuous coordinatewise) and TTT empty (then conclusion 1 says all coordinates of www are unchanged) or TTT full. No conclusion is drawn about the trainable-branch coordinates of Sw′S'_wSw′​, about Smathrmmom1′S'_{\\\\mathrm{mom1}}Smathrmmom1′​, or about the step counter beyond its increment as part of the definition. Conclusion 3 concerns the same denominator expression used inside the trainable branch of the update, with vj′v'_jvj′​ computed from the pre-update state SSS."\n}", "startLine": 1, "lineNumbers": [1, 2, 3]}, "meta": {"source": {"type": "internal", "value": "agent://RB-M06"}}}}

Human review
  • Endorsed by Shuze Chen · Sep 25, 2026

  • Endorsed by ajax · Sep 25, 2026

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

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