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Ω(1/k²) spectral gap of the adiabatic clock Hamiltonian on the computational subspace

Proved
QAlgorithms.Childs.clockPathMatrix_gap

by Goku · Oct 13, 2026 · Mathlib 0df444a (Lean v4.33.1)

childslecture-notesquantum-information

Let k≥0k \ge 0k≥0 be the number of gates of a quantum circuit and let s∈[0,1]s \in [0,1]s∈[0,1]. In the adiabatic simulation of the circuit, the interpolated Hamiltonian H(s)=(1−s)HB+sHCH(s) = (1-s)H_B + sH_CH(s)=(1−s)HB​+sHC​ leaves invariant the (k+1)(k+1)(k+1)-dimensional computational subspace spanned by the history states ∣ψ0⟩,…,∣ψk⟩|\psi_0\rangle, \dots, |\psi_k\rangle∣ψ0​⟩,…,∣ψk​⟩, and on it acts, by ⟨ψj∣HB∣ψj′⟩=−δj,j′δj,0\langle\psi_j|H_B|\psi_{j'}\rangle = -\delta_{j,j'}\delta_{j,0}⟨ψj​∣HB​∣ψj′​⟩=−δj,j′​δj,0​ and ⟨ψj∣HC∣ψj′⟩=−(δj,j′+1+δj,j′−1)\langle\psi_j|H_C|\psi_{j'}\rangle = -(\delta_{j,j'+1}+\delta_{j,j'-1})⟨ψj​∣HC​∣ψj′​⟩=−(δj,j′+1​+δj,j′−1​), as the real symmetric (k+1)×(k+1)(k+1)\times(k+1)(k+1)×(k+1) matrix

Ak(s)=(s−1−s0⋯0−s0−s⋱⋮0−s0⋱0⋮⋱⋱⋱−s0⋯0−s0),A_k(s) = \begin{pmatrix} s-1 & -s & 0 & \cdots & 0 \\ -s & 0 & -s & \ddots & \vdots \\ 0 & -s & 0 & \ddots & 0 \\ \vdots & \ddots & \ddots & \ddots & -s \\ 0 & \cdots & 0 & -s & 0 \end{pmatrix},Ak​(s)=​s−1−s0⋮0​−s0−s⋱⋯​0−s0⋱0​⋯⋱⋱⋱−s​0⋮0−s0​​,

whose (0,0)(0,0)(0,0) entry is s−1s-1s−1, whose first off-diagonal entries are −s-s−s, and whose other entries vanish. Let λ0(s)≤λ1(s)≤⋯≤λk(s)\lambda_0(s) \le \lambda_1(s) \le \cdots \le \lambda_k(s)λ0​(s)≤λ1​(s)≤⋯≤λk​(s) be its eigenvalues, counted with multiplicity, and Δk(s)=λ1(s)−λ0(s)\Delta_k(s) = \lambda_1(s) - \lambda_0(s)Δk​(s)=λ1​(s)−λ0​(s) the gap between the smallest and the second smallest.

Lemma. The gap is Ω(1/k2)\Omega(1/k^2)Ω(1/k2) uniformly in s∈[0,1]s \in [0,1]s∈[0,1]: there are a constant c>0c > 0c>0 and a threshold k0k_0k0​ such that

Δk(s)≥ck2for all k≥k0 and all s∈[0,1].\Delta_k(s) \ge \frac{c}{k^2} \qquad \text{for all } k \ge k_0 \text{ and all } s \in [0,1].Δk​(s)≥k2c​for all k≥k0​ and all s∈[0,1].

This bound on the minimum gap along the whole interpolation path is what makes an adiabatic evolution time T=poly(k)T = \mathrm{poly}(k)T=poly(k) sufficient, and hence shows that adiabatic quantum computation can efficiently simulate the circuit model.

Formalization Note The matrix is the shared definition clockPathMatrix k s on Fin(k+1)\mathrm{Fin}(k+1)Fin(k+1); the gap is spectralGap, the second smallest minus the smallest eigenvalue of the Hermitian matrix with multiplicity (so a degenerate ground level would give gap 000). The constants ccc and k0k_0k0​ are quantified before kkk and sss.

Preamble
import Definitions.Def_QAlgorithms_Defs_Hamiltonian
set_option autoImplicit false
Formal statement
namespace QAlgorithms.Childs

/-- Childs, Lemma 33.1 (PDF p. 182; matrix (33.16) on PDF p. 181): the gap between the smallest
and second smallest eigenvalues of the matrix (33.16) for `s ∈ [0, 1]` is `Ω(1/k²)`. The
constant `c > 0` and the threshold `k₀` are chosen before `k` and are uniform over
`s ∈ [0, 1]`. -/
theorem clockPathMatrix_gap :
    ∃ c : ℝ, 0 < c ∧ ∃ k₀ : ℕ, ∀ k : ℕ, k₀ ≤ k → ∀ s ∈ Set.Icc (0 : ℝ) 1,
      c / (k : ℝ) ^ 2 ≤ spectralGap (clockPathMatrix k s) := by
  sorry

end QAlgorithms.Childs
Source
Andrew Childs, Lecture Notes on Quantum Algorithms, 17 April 2025, PDF p. 182, Lemma 33.1. https://www.cs.umd.edu/~amchilds/qa/qa.pdf
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What the Lean code literally says, in plain math · claude-opus-5-5

The statement asserts that there exist a real constant c>0c > 0c>0 and a natural number k0k_0k0​ such that for every natural number k≥k0k \ge k_0k≥k0​ and every real s∈[0,1]s \in [0,1]s∈[0,1],

ck2  ≤  Δ(Mk(s)).\frac{c}{k^2} \;\le\; \Delta\big(M_k(s)\big).k2c​≤Δ(Mk​(s)).

The matrix Mk(s)M_k(s)Mk​(s). This is the real (k+1)×(k+1)(k+1)\times(k+1)(k+1)×(k+1) matrix with rows and columns indexed by 0,1,…,k0,1,\dots,k0,1,…,k, with entries:

  • (Mk(s))00=s−1(M_k(s))_{00} = s - 1(Mk​(s))00​=s−1;
  • otherwise, (Mk(s))ij=−s(M_k(s))_{ij} = -s(Mk​(s))ij​=−s whenever ∣i−j∣=1|i-j| = 1∣i−j∣=1;
  • all other entries are 000.

So it is −s-s−s times the adjacency matrix of the path on k+1k+1k+1 vertices, plus s−1s-1s−1 in the top-left corner. For example, Mk(0)=diag⁡(−1,0,…,0)M_k(0) = \operatorname{diag}(-1,0,\dots,0)Mk​(0)=diag(−1,0,…,0). The matrix is symmetric for every kkk and sss.

The gap Δ\DeltaΔ. For a real square matrix AAA of size mmm:

  • If m≥2m \ge 2m≥2, Δ(A)=λ2−λ1\Delta(A) = \lambda_2 - \lambda_1Δ(A)=λ2​−λ1​, where λ1≤λ2≤⋯≤λm\lambda_1 \le \lambda_2 \le \dots \le \lambda_mλ1​≤λ2​≤⋯≤λm​ are the eigenvalues of AAA counted with multiplicity and sorted increasingly.
  • If m<2m < 2m<2, then Δ(A)=0\Delta(A) = 0Δ(A)=0.
  • If AAA is not symmetric (Hermitian), all "eigenvalues" are taken to be 000 by convention. This case does not arise here, since Mk(s)M_k(s)Mk​(s) is symmetric.

So for k≥1k \ge 1k≥1, Δ(Mk(s))\Delta(M_k(s))Δ(Mk​(s)) is the difference between the two smallest eigenvalues of Mk(s)M_k(s)Mk​(s). It is zero if the smallest eigenvalue is repeated.

Edge cases.

  • For k=0k = 0k=0 the matrix is 1×11\times 11×1, so Δ=0\Delta = 0Δ=0. The left side c/02c/0^2c/02 is evaluated with the convention that division by zero yields 000, so the inequality reads 0≤00 \le 00≤0.
  • Because k0k_0k0​ is existentially chosen, the claim only concerns all sufficiently large kkk. No explicit value of ccc or k0k_0k0​ is asserted.
  • The bound must hold uniformly in sss over the closed interval, including both endpoints s=0s = 0s=0 and s=1s = 1s=1.
Human review
  • Endorsed by Shuze Chen · Oct 13, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Goku · Oct 13, 2026

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

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