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The stepsizes (3.6) are positive and strictly decreasing

Proved
ThreeOpSplitting.Accel.stepsizes_decreasing_part1

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

accelerationp2o-batch-p100bp2o-gran-per-chapterp2o-plan-paperp2o-v1stepsize

Let μB≥0\mu_B \ge 0μB​≥0, μC>0\mu_C > 0μC​>0, η∈(0,1)\eta \in (0,1)η∈(0,1) and γ0>0\gamma_0 > 0γ0​>0, and let (γk)k≥0(\gamma_k)_{k \ge 0}(γk​)k≥0​ be generated by the stepsize rule (3.6). Then for every k≥0k \ge 0k≥0, γk+1>0\gamma_{k+1} > 0γk+1​>0 and

γk2−γk+12=γkγk+1(2γk+1μB+2γkμCη)>0.\gamma_k^2 - \gamma_{k+1}^2 = \gamma_k\gamma_{k+1}\big(2\gamma_{k+1}\mu_B + 2\gamma_k\mu_C\eta\big) > 0.γk2​−γk+12​=γk​γk+1​(2γk+1​μB​+2γk​μC​η)>0.

In particular (γk)(\gamma_k)(γk​) is decreasing and (1/γk)(1/\gamma_k)(1/γk​) is increasing, which is the monotonicity hypothesis needed to apply the Stolz–Cesàro theorem in the proof of Theorem 3.3.

Formalization Note The paper prints the bracket as 2γkμB+2γk+1μCη2\gamma_k\mu_B + 2\gamma_{k+1}\mu_C\eta2γk​μB​+2γk+1​μC​η, with γk\gamma_kγk​ and γk+1\gamma_{k+1}γk+1​ swapped. That version is false in general (for μB=0.7\mu_B = 0.7μB​=0.7, μC=1.3\mu_C = 1.3μC​=1.3, η=0.4\eta = 0.4η=0.4, γk=0.5\gamma_k = 0.5γk​=0.5 the two sides are 0.15110.15110.1511 and 0.16160.16160.1616). Multiplying the identity (1+2γkμB)/γk2=(1−2γk+1μCη)/γk+12(1+2\gamma_k\mu_B)/\gamma_k^2 = (1-2\gamma_{k+1}\mu_C\eta)/\gamma_{k+1}^2(1+2γk​μB​)/γk2​=(1−2γk+1​μC​η)/γk+12​ by γk2γk+12\gamma_k^2\gamma_{k+1}^2γk2​γk+12​ gives the corrected form stated here. The positivity claim and the rest of the proof are unaffected, since γk/γk+1→1\gamma_k/\gamma_{k+1} \to 1γk​/γk+1​→1.

Preamble
import Mathlib
import Definitions.Def_ThreeOpSplitting_Accel_Stepsizes

open Filter Topology
Formal statement
namespace ThreeOpSplitting.Accel

/-- Proof of Theorem 3.3, Part 1 (p. 845): the stepsizes (3.6) are positive and strictly
decreasing, with `γ_k² - γ_{k+1}² = γ_kγ_{k+1}(2γ_{k+1}μ_B + 2γ_kμ_Cη) > 0` for all `k ≥ 0`.
The page prints the bracket as `2γ_kμ_B + 2γ_{k+1}μ_Cη` (indices swapped), which is false in
general; the identity above is the one that follows from (3.6). -/
theorem stepsizes_decreasing_part1 (μB μC η γ0 : ℝ)
    (hμB : 0 ≤ μB) (hμC : 0 < μC) (hη0 : 0 < η) (hη1 : η < 1) (hγ0 : 0 < γ0) (k : ℕ) :
    0 < stepsPart1 μB μC η γ0 (k + 1) ∧
    stepsPart1 μB μC η γ0 k ^ 2 - stepsPart1 μB μC η γ0 (k + 1) ^ 2
      = stepsPart1 μB μC η γ0 k * stepsPart1 μB μC η γ0 (k + 1)
        * (2 * stepsPart1 μB μC η γ0 (k + 1) * μB + 2 * stepsPart1 μB μC η γ0 k * μC * η) ∧
    0 < stepsPart1 μB μC η γ0 k ^ 2 - stepsPart1 μB μC η γ0 (k + 1) ^ 2 := by sorry

end ThreeOpSplitting.Accel
Source
Davis and Yin, A Three-Operator Splitting Scheme and its Optimization Applications, Set-Valued Var. Anal. 25 (2017), https://doi.org/10.1007/s11228-017-0421-z, p. 845, Section 3.3, proof of Theorem 3.3, Part 1 (unnumbered display)
Read-back

What the Lean code literally says, in plain math · claude-opus-5-5

The hypotheses and the sequence are the same as in the previous read-back. μB,μC,η,γ0\mu_B, \mu_C, \eta, \gamma_0μB​,μC​,η,γ0​ are reals with μB≥0\mu_B \ge 0μB​≥0, μC>0\mu_C > 0μC​>0, 0<η<10 < \eta < 10<η<1 and γ0>0\gamma_0 > 0γ0​>0. The sequence (γj)(\gamma_j)(γj​) starts at γ0\gamma_0γ0​ and follows

γj+1=−2γj2μCη+(2γj2μCη)2+4(1+2γjμB)γj22(1+2γjμB),\gamma_{j+1} = \frac{-2\gamma_j^2\mu_C\eta + \sqrt{(2\gamma_j^2\mu_C\eta)^2 + 4(1+2\gamma_j\mu_B)\gamma_j^2}}{2(1+2\gamma_j\mu_B)},γj+1​=2(1+2γj​μB​)−2γj2​μC​η+(2γj2​μC​η)2+4(1+2γj​μB​)γj2​​​,

with the square root of a negative number read as 000 and division by 000 giving 000.

The theorem states that for every k∈Nk \in \mathbb{N}k∈N, including k=0k = 0k=0, all three of the following hold:

  1. γk+1>0\gamma_{k+1} > 0γk+1​>0;
  2. γk2−γk+12=γkγk+1(2γk+1μB+2γkμCη)\gamma_k^2 - \gamma_{k+1}^2 = \gamma_k\gamma_{k+1}\big(2\gamma_{k+1}\mu_B + 2\gamma_k\mu_C\eta\big)γk2​−γk+12​=γk​γk+1​(2γk+1​μB​+2γk​μC​η);
  3. γk2−γk+12>0\gamma_k^2 - \gamma_{k+1}^2 > 0γk2​−γk+12​>0.

Combined with γ0>0\gamma_0 > 0γ0​>0, these give a strictly positive sequence whose squares, and hence whose terms, strictly decrease. The case μB=0\mu_B = 0μB​=0 is allowed; the bracket in item 2 then reduces to 2γkμCη2\gamma_k\mu_C\eta2γk​μC​η. No degenerate zero or empty cases arise beyond this, since all parameters are constrained as stated.

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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