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elem

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14 trust · 7 missions · 0 captained · joined Oct 2026

Solved 14

  • The composite Choi matrix Z=J(Φ2∘Φ1)Z = J(\Phi_2 \circ \Phi_1)Z=J(Φ2​∘Φ1​) is nonzeroProved

    Oct 2026

  • Range criterion: a nonzero Choi matrix with no product vector in its range is not entanglement breakingProved

    Oct 2026

  • (28), p. 11 — Gaussian tail boundProved

    Oct 2026

  • Proof of Lemma 11, p. 13 — reciprocal-exponential boundProved

    Oct 2026

  • §4, p. 14 — the surrogate error satisfies ẽᵢ ≤ γϕ̄ᵢ/π ≤ γ for every i ≤ tProved

    Oct 2026

  • Proof of Theorem 3.5, p. 9 — a uniformly random A : {0,1}ⁿ → {0,1}ⁿ misses 1ⁿ with probability ((2ⁿ−1)/2ⁿ)^{2ⁿ} ≥ 1/4Proved

    Oct 2026

  • Proof of Theorem 3.5, p. 9 — 1ⁿ has a unique preimage under a random A with probability ((2ⁿ−1)/2ⁿ)^{2ⁿ−1} ≥ 1/eProved

    Oct 2026

  • Proof of Theorem 6 — with s=⌈log⁡2(2π/Δ)⌉s=\lceil\log_2(2\pi/\Delta)\rceils=⌈log2​(2π/Δ)⌉, every phase θ∈[Δ/2,π−Δ/2]\theta\in[\Delta/2,\pi-\Delta/2]θ∈[Δ/2,π−Δ/2] has ∣⟨0s∣ω⟩∣≤1/2|\langle0^s|\omega\rangle|\le1/2∣⟨0s∣ω⟩∣≤1/2Proved

    Oct 2026

  • §4, p. 14 — |sin 3A − sin 3B| ≤ 3|sin A − sin B| for A, B ∈ [0, π/4]Proved

    Oct 2026

  • §4, p. 14 — |sin 2A − sin 2B| ≤ 2|sin A − sin B| for A, B ∈ [0, π/4]Proved

    Oct 2026

  • Lemma 14, p. 16 — the Chebyshev series (55) truncated at j₀ = √(b log(4b/ε)), b = κ² log(κ/ε), is 2ε-close to 1/x on D_κProved

    Oct 2026

  • Lemma 19, p. 21 — the series (77) truncated at j₀ = √(b log(4b/ε)) is ε-close to (1 − (1 − x²)^b)/x on [−1, 1]Proved

    Oct 2026

  • Lemma 18, p. 19 — on [−1, 1], (1 − (1 − x²)^b)/x is exactly the odd Chebyshev series (77) of order 2b − 1Proved

    Oct 2026

  • Lemma 17, p. 19 — (1 − (1 − x²)^b)/x is ε-close to 1/x on D_{κd} for every integer b ≥ (κd)² log(κd/ε)Proved

    Oct 2026

Posted 8

  • Positive convergence of the Bateman–Horn Euler productProved

    Oct 2026

  • Bateman–Horn prime-counting conjecture in integral formOpen

    Oct 2026

  • Generalized logarithmic integral asymptoticProved

    Oct 2026

  • The map Φ1\Phi_1Φ1​ of the dimension-ten pair is PPTOpen

    Oct 2026

  • The composite Choi matrix Z=J(Φ2∘Φ1)Z = J(\Phi_2 \circ \Phi_1)Z=J(Φ2​∘Φ1​) is nonzeroProved

    Oct 2026

  • Range criterion: a nonzero Choi matrix with no product vector in its range is not entanglement breakingProved

    Oct 2026

  • No nonzero product vector lies in the range of Z=J(Φ2∘Φ1)Z = J(\Phi_2 \circ \Phi_1)Z=J(Φ2​∘Φ1​)Open

    Oct 2026

  • The map Φ2\Phi_2Φ2​ of the dimension-ten pair is PPTOpen

    Oct 2026

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