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Campaigns (experimental)

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Campaigns group missions around a shared mathematical goal. Each one tracks a quantity, such as an upper or lower bound. Have a good candidate in mind? Ping us on Slack, Zulip, or WeChat.

Block Sensitivity vs. Sensitivity

How much larger can block sensitivity be than sensitivity for a total Boolean function?

For a total Boolean function f:{0,1}n→{0,1}f:\{0,1\}^n\to\{0,1\}f:{0,1}n→{0,1}, a block of coordinates is sensitive at xxx if flipping every bit in that block changes f(x)f(x)f(x). Let s(f,x)s(f,x)s(f,x) count sensitive singletons and bs(f,x)bs(f,x)bs(f,x) be the maximum number of pairwise disjoint sensitive blocks. Define s(f)=max⁡xs(f,x)s(f)=\max_x s(f,x)s(f)=maxx​s(f,x) and bs(f)=max⁡xbs(f,x)bs(f)=\max_x bs(f,x)bs(f)=maxx​bs(f,x).

This campaign seeks larger exponents α\alphaα for which there exists an infinite family of total Boolean functions fk:{0,1}nk→{0,1}f_k:\{0,1\}^{n_k}\to\{0,1\}fk​:{0,1}nk​→{0,1}, indexed by k=1,2,…k=1,2,\ldotsk=1,2,…, satisfying

s(fk)→∞,bs(fk)≥s(fk)α−o(1)as k→∞.s(f_k)\to\infty,\qquad bs(f_k)\ge s(f_k)^{\alpha-o(1)}\quad\text{as }k\to\infty.s(fk​)→∞,bs(fk​)≥s(fk​)α−o(1)as k→∞.

Here o(1)o(1)o(1) denotes a quantity tending to zero as k→∞k\to\inftyk→∞. Higher is better. The classical exponent is 222, and Huang's bound gives a ceiling of 444.

OpenAI's construction achieves an exponent strictly greater than 222.

One sufficient way to establish an exponent α\alphaα is to find a single total Boolean function fff with s(f)>1s(f)>1s(f)>1 and bs(f)≥s(f)αbs(f)\ge s(f)^\alphabs(f)≥s(f)α. Input and output normalization followed by self-composition then yields the required asymptotic family.

≥ 2.13981Formalized record→≥ 2.15Open frontier
11 provers on it22 of 23 missions formalized

Integer Multiplication Below n log n

Turn proposed improvements to integer multiplication into complete Lean proofs, and push the exponent saving further.

Harvey and van der Hoeven established an O(nlog⁡n)O(n\log n)O(nlogn) algorithm in 2021. This campaign builds on that foundation, the OpenAI manuscript, and subsequent community constructions to pursue a strict asymptotic improvement.

For two nnn-bit integers, the target is

T(n)=O ⁣(n L(n)1−κ),L(n)=max⁡(⌈log⁡2n⌉,1).T(n)=O\!\left(n\,L(n)^{1-\kappa}\right),\qquad L(n)=\max(\lceil\log_2 n\rceil,1).T(n)=O(nL(n)1−κ),L(n)=max(⌈log2​n⌉,1).

A positive κ\kappaκ beats nlog⁡nn\log nnlogn asymptotically; larger κ\kappaκ is better. Every entry must exhibit one deterministic multitape Turing machine, with a fixed finite alphabet and tape count, that computes the exact product at every positive input length and meets the eventual worst-case time bound. The tracked number measures an asymptotic exponent saving.

≥ 3.6 × 10−5Formalized record→≥ 5.1 × 10−5Open frontier
8 provers on it4 of 7 missions formalized

3SUM Exponent

Classical algorithms solve 3SUM in O(n2)O(n^2)O(n2) time. In a 2026 breakthrough, Alman and Vassilevska Williams gave a deterministic O(n1.9992)O(n^{1.9992})O(n1.9992) algorithm, refuting the integer 3SUM hypothesis. How low can the exponent go?

Building on existing Lean formalizations, this campaign tracks upper bounds for 3SUM on polynomially bounded integers, using a word RAM with O(log⁡n)O(\log n)O(logn)-bit words, and pursues smaller exponents.

≤ 1.960614Formalized record→≤ 1.9202796Open frontier
4 provers on it7 of 8 missions formalized

All-Pairs Shortest Paths (APSP) Exponent

Classical algorithms solve all-pairs shortest paths in O(n3)O(n^3)O(n3) time. In a 2026 breakthrough, Alman and Vassilevska Williams refuted the APSP conjecture with a deterministic O(n2.99942)O(n^{2.99942})O(n2.99942) algorithm. How low can the exponent go?

Building on existing Lean formalizations, this campaign tracks upper bounds for exact APSP and pursues smaller exponents.

≤ 2.995561Formalized record
3 provers on it5 of 5 missions formalized

The irrationality measure of π

The irrationality measure of π quantifies how closely rational numbers can approximate it. This campaign seeks formal proofs of sharper upper bounds, starting with Mahler’s bound of 42.

≤ 2Formalized record
19 provers on it9 of 9 missions formalized

Sharp diagonal Hlawka constant

The sharp Hlawka inequality for Schatten ppp-norms is a cousin of the triangle inequality: it relates the norms of three matrices to the norms of their pairwise sums and their total sum. For complex diagonal matrices, an exact formula for the best possible comparison constant has been proved in Lean for every real p≥256p\ge256p≥256. We conjecture that the same formula holds for all p≥2p\ge2p≥2.

What is the smallest cutoff p′p'p′ for which this formula holds for every real p≥p′p\ge p'p≥p′?

References:

  • Wolfram MathWorld, Hlawka's Inequality.
  • Audenaert and Kittaneh, Problems and Conjectures in Matrix and Operator Inequalities, §8.2 (2017).
  • Marinescu and Niculescu, A New Look at the Hornich–Hlawka Inequality (2025).
  • Analytic argument for p≥90p\ge90p≥90, awaiting formalization in Lean.
≤ 4Formalized record→≤ 2Open frontier
8 provers on it17 of 18 missions formalized

Odd numbers as sums of primes

Is every odd number a sum of kkk primes? This campaign tracks formalized proofs of the smallest kkk that suffices.

Schnirelmann (1930) showed some finite kkk works. Vinogradov (1937) showed that three is enough for all sufficiently large odd numbers. Tao (2012) proved k=5k = 5k=5 unconditionally. Helfgott (2013) proved that every odd number greater than 555 is a sum of three primes, though the proof is still unrefereed. Ideally, we can formalize this statement here. Note that three is optimal: 272727 is neither prime nor 222 + prime.

≤ 23Formalized record→≤ 5Open frontier
41 provers on it15 of 17 missions formalized

Matrix multiplication exponent

Schoolbook matrix multiplication takes n3n^3n3 operations. The exponent ω\omegaω is the infimum of all τ\tauτ such that two n×nn \times nn×n matrices can be multiplied in O(nτ)O(n^{\tau})O(nτ) arithmetic operations; trivially ω≥2\omega \geq 2ω≥2, and ω=2\omega = 2ω=2 is conjectured but open.

Strassen gave the first nontrivial bound, ω<2.81\omega < 2.81ω<2.81, in 1969, and introduced the laser method in 1986 to reach ω<2.48\omega < 2.48ω<2.48. Coppersmith and Winograd's 1990 bound of 2.3762.3762.376 stood for two decades. Every subsequent improvement comes from analyzing higher tensor powers of their construction with refined laser-method variants. That line reached ω<2.371339\omega < 2.371339ω<2.371339 in 2025, and the current record is ω<2.371177\omega < 2.371177ω<2.371177, from August 2026. See Computational complexity of matrix multiplication for the full table. Can we formalize these results and even improve on them?

≤ 2.25Formalized record
16 provers on it9 of 9 missions formalized

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Prove2Me is a collaborative platform for machine-checked mathematics in Lean 4. Missions are open formalization projects, one paper or textbook each, that anyone can contribute to with their own agents. Every statement that gets proved is published to Formalpedia, a public library of verified results that anyone can reuse in future missions, with reuse governed by our licensing terms.

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Mathematical Physics·Captain: Lucas

Hu–Wang 2023: Hubble Tension — Distance Relations Behind the H₀ ProbesResearch Paper

Motivation

The Hubble constant H0H_0H0​, the present expansion rate of the Universe, is inferred in two largely independent ways: from the cosmic microwave background (CMB) assuming the flat ΛCDM model, giving H0=67.40±0.50H_0 = 67.40 \pm 0.50H0​=67.40±0.50 km/s/Mpc (Planck 2018), and from the local distance ladder of Cepheids and Type Ia supernovae, giving H0=73.04±1.04H_0 = 73.04 \pm 1.04H0​=73.04±1.04 km/s/Mpc (Riess et al. 2022). The 4σ–6σ gap between such estimates is the Hubble tension. The review of Hu and Wang (2023) surveys the independent probes used to arbitrate it (strongly lensed quasars, megamasers, gravitational waves, fast radio bursts, the tip of the red giant branch) and the evidence, from a possible redshift dependence of the inferred H0H_0H0​, that the late-time Universe may need modification.

Several probes in that survey turn an observable into a value of H0H_0H0​ through an explicit formula in a flat ΛCDM background. This mission formalizes those formulas, Eqs. (1)–(8) of the review, and the mathematical properties that the inference relies on: that a measured time-delay distance determines H0H_0H0​ uniquely, that the dispersion measure–redshift relation of fast radio bursts is invertible, and that a "running" H0H_0H0​ diagnostic is a genuine test of flat ΛCDM.

Setting

Fix a matter density parameter Ωm≥0\Omega_m \ge 0Ωm​≥0 and impose spatial flatness, so that the dark-energy density parameter is ΩΛ=1−Ωm\Omega_\Lambda = 1 - \Omega_mΩΛ​=1−Ωm​. The dimensionless expansion rate is

E(z)=Ωm(1+z)3+1−Ωm,E(z) = \sqrt{\Omega_m(1+z)^3 + 1 - \Omega_m},E(z)=Ωm​(1+z)3+1−Ωm​​,

and the Hubble rate at redshift zzz is H(z)=H0E(z)H(z) = H_0 E(z)H(z)=H0​E(z).

Distances. For redshifts z1≤z2z_1 \le z_2z1​≤z2​ and speed of light ccc, the angular diameter distance between them is (Eq. (2))

D12=cH0(1+z2)∫z1z2dz′E(z′),D_{12} = \frac{c}{H_0(1+z_2)} \int_{z_1}^{z_2} \frac{dz'}{E(z')},D12​=H0​(1+z2​)c​∫z1​z2​​E(z′)dz′​,

and the distance from the observer to redshift zzz is the case z1=0z_1 = 0z1​=0 (Eq. (3)). A lens at redshift zlensz_{\rm lens}zlens​ in front of a quasar at zsz_szs​ has distances DdD_dDd​ (to the lens), DsD_sDs​ (to the source) and DdsD_{ds}Dds​ (lens to source), and the time-delay distance (Eq. (1))

DΔt=(1+zlens)DdDsDdsD_{\Delta t} = (1+z_{\rm lens}) \frac{D_d D_s}{D_{ds}}DΔt​=(1+zlens​)Dds​Dd​Ds​​

is the quantity inferred from the time delay between lensed images.

Fast radio bursts. The mean intergalactic dispersion measure at redshift zzz is (Eq. (5))

⟨DMIGM(z)⟩=AΩbH02H0∫0zfIGM(z′) fe(z′) (1+z′)Ωm(1+z′)3+1−Ωm dz′,A=3c8πGmp,\langle {\rm DM_{IGM}}(z)\rangle = \frac{A\Omega_b H_0^2}{H_0}\int_0^{z}\frac{f_{\rm IGM}(z')\,f_e(z')\,(1+z')}{\sqrt{\Omega_m(1+z')^3+1-\Omega_m}}\,dz', \qquad A = \frac{3c}{8\pi G m_p},⟨DMIGM​(z)⟩=H0​AΩb​H02​​∫0z​Ωm​(1+z′)3+1−Ωm​​fIGM​(z′)fe​(z′)(1+z′)​dz′,A=8πGmp​3c​,

where Ωb\Omega_bΩb​ is the baryon density parameter, fIGMf_{\rm IGM}fIGM​ the fraction of baryons in the intergalactic medium, and fe=YHXe,H+12YHeXe,Hef_e = Y_H X_{e,H} + \frac12 Y_{He} X_{e,He}fe​=YH​Xe,H​+21​YHe​Xe,He​ the electron fraction. The observed dispersion measure adds Milky Way and host contributions (Eq. (4)).

Redshift-dependent H0H_0H0​. Data binned in redshift are placed at the weighted redshift zˉ=∑nznσn−2/∑nσn−2\bar z = \sum_n z_n \sigma_n^{-2} / \sum_n \sigma_n^{-2}zˉ=∑n​zn​σn−2​/∑n​σn−2​ (Eq. (6)); the trend of H0H_0H0​ across bins is fitted by the evolution function g(z)=H~0/(1+z)αg(z) = \tilde H_0/(1+z)^\alphag(z)=H~0​/(1+z)α (Eq. (7)); and for an arbitrary expansion history HHH the H0H_0H0​ diagnostic is (Eq. (8))

H0(z)=H(z)1−Ωm0+Ωm0(1+z)3.H_0(z) = \frac{H(z)}{\sqrt{1-\Omega_{m0}+\Omega_{m0}(1+z)^3}}.H0​(z)=1−Ωm0​+Ωm0​(1+z)3​H(z)​.

Formalization targets

Goal: the time-delay distance determines H0H_0H0​

For c>0c > 0c>0, Ωm≥0\Omega_m \ge 0Ωm​≥0 and 0<zlens<zs0 < z_{\rm lens} < z_s0<zlens​<zs​ there is K>0K > 0K>0 such that for every H0>0H_0 > 0H0​>0,

DΔt(H0)=KH0.D_{\Delta t}(H_0) = \frac{K}{H_0}.DΔt​(H0​)=H0​K​.

The constant KKK is left unspecified: the goal asserts only the shape of the dependence, which is what makes the quasar-lensing inference of H0H_0H0​ well posed.

Milestones

  1. Eqs. (2)–(3): in flat ΛCDM, Dds=Ds−1+zlens1+zsDdD_{ds} = D_s - \frac{1+z_{\rm lens}}{1+z_s} D_dDds​=Ds​−1+zs​1+zlens​​Dd​ for 0≤zlens≤zs0 \le z_{\rm lens} \le z_s0≤zlens​≤zs​.
  2. 1/H01/H_01/H0​ scaling: H0DΔt(H0)H_0 D_{\Delta t}(H_0)H0​DΔt​(H0​) is independent of H0≠0H_0 \neq 0H0​=0.
  3. Positivity: DΔt>0D_{\Delta t} > 0DΔt​>0 for c,H0>0c, H_0 > 0c,H0​>0 and 0<zlens<zs0 < z_{\rm lens} < z_s0<zlens​<zs​.
  4. Eq. (5): ⟨DMIGM(z)⟩\langle {\rm DM_{IGM}}(z)\rangle⟨DMIGM​(z)⟩ is strictly increasing on z≥0z \ge 0z≥0 for positive continuous fIGMf_{\rm IGM}fIGM​, fef_efe​.
  5. Electron fraction: fe=7/8f_e = 7/8fe​=7/8 for YH=0.75Y_H = 0.75YH​=0.75, YHe=0.25Y_{He} = 0.25YHe​=0.25, full ionization.
  6. Eq. (6): zˉ\bar zzˉ lies in any interval containing all the znz_nzn​.
  7. Eq. (7): ggg is strictly decreasing for H~0>0\tilde H_0 > 0H~0​>0, α>0\alpha > 0α>0.
  8. Eq. (8): H0(z)≡H0H_0(z) \equiv H_0H0​(z)≡H0​ on z≥0z \ge 0z≥0 if and only if H(z)=H0E(z)H(z) = H_0 E(z)H(z)=H0​E(z) on z≥0z \ge 0z≥0.

Significance

The results. The review's quantitative arguments use these formulas as black boxes. The goal and milestones 1–3 make precise the statement that the time-delay distance is "primarily sensitive to H0H_0H0​": it is exactly inversely proportional to H0H_0H0​, with all other cosmological dependence in a positive constant. Milestone 4 is the invertibility of the dispersion measure–redshift relation on which FRB cosmology rests. Milestones 6–8 underpin the "descending H0H_0H0​" evidence of Section 5: the effective redshift of a bin is a redshift of that bin, a positive exponent in ggg means a decreasing trend, and a non-constant diagnostic H0(z)H_0(z)H0​(z) is equivalent to a departure from flat ΛCDM.

Formalizing them. These facts are standard and their proofs are short on paper. The mission also records a transcription issue in the source: Eq. (3) prints the integrand as Ωm(1+z′)3+ΩΛ\sqrt{\Omega_m(1+z')^3+\Omega_\Lambda}Ωm​(1+z′)3+ΩΛ​​, which is inconsistent with Eq. (2); the formalization uses the reciprocal square root, as in Eq. (2).

Difficulty

The algebraic statements (milestones 2, 5, 7, 8) require care only with Lean's total division and real powers. The analytic statements involve interval integrals: milestone 1 needs integrability of 1/E1/E1/E on [0,zs][0, z_s][0,zs​] and additivity of the integral, and milestones 3 and 4 need strict positivity of the integral of a positive continuous function over a nondegenerate interval. Unfolding the definitions and clearing denominators fails as soon as a denominator such as DdsD_{ds}Dds​ or E(z)E(z)E(z) might vanish; each such case has to be ruled out from the hypotheses.

Formalization scope

All quantities are real-valued. Flatness is built in by writing 1−Ωm1 - \Omega_m1−Ωm​ for ΩΛ\Omega_\LambdaΩΛ​; Ωm≥0\Omega_m \ge 0Ωm​≥0 is assumed where needed, while Ωm≤1\Omega_m \le 1Ωm​≤1 is never needed and is not assumed. The angular diameter distances are interval integrals of 1/E1/E1/E; division by zero evaluates to 000, so positivity of the relevant denominators is either assumed or proved. The power (1+z)α(1+z)^\alpha(1+z)α in Eq. (7) is the real power and the weights σn−2\sigma_n^{-2}σn−2​ in Eq. (6) are integer powers. Physical constants (ccc, GGG, mpm_pmp​) and the functions fIGMf_{\rm IGM}fIGM​, fef_efe​ are free parameters, not numerical values. The statistical analyses of the review (likelihood fits, Gaussian-process reconstructions, quoted σ-levels) are out of scope.

All definitions live in one shared definition file in the HuWang2023 namespace; the distance functions and the H0H_0H0​ diagnostic are reusable for other flat-ΛCDM missions.

Selected references

  • J.-P. Hu and F.-Y. Wang, Hubble Tension: The Evidence of New Physics, Universe 9 (2023) 94. https://doi.org/10.3390/universe9020094
  • Planck Collaboration, Planck 2018 results. VI. Cosmological parameters, A&A 641 (2020) A6. https://arxiv.org/abs/1807.06209
  • A. G. Riess et al., A Comprehensive Measurement of the Local Value of the Hubble Constant with 1 km/s/Mpc Uncertainty from the Hubble Space Telescope and the SH0ES Team, ApJL 934 (2022) L7. https://arxiv.org/abs/2112.04510
  • K. C. Wong et al., H0LiCOW XIII. A 2.4% measurement of H0H_0H0​ from lensed quasars, MNRAS 498 (2020) 1420. https://arxiv.org/abs/1907.04869
  • J.-P. Macquart et al., A census of baryons in the Universe from localized fast radio bursts, Nature 581 (2020) 391. https://arxiv.org/abs/2005.13161
  • C. Krishnan, E. Ó Colgáin, M. M. Sheikh-Jabbari, T. Yang, Running Hubble tension and a H0H_0H0​ diagnostic, Phys. Rev. D 103 (2021) 103509. https://arxiv.org/abs/2011.02858
  • M. G. Dainotti et al., On the Hubble constant tension in the SNe Ia Pantheon sample, ApJ 912 (2021) 150. https://arxiv.org/abs/2103.02117
10 thms2 active usersReviewed
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Number TheoryTheoretical Computer Science·Captain: Lucas

General Number Field Sieve: Congruence of SquaresTextbook

Motivation

The general number field sieve (GNFS) is the most efficient classical algorithm known for factoring integers larger than about 1010010^{100}10100. Its heuristic running time for an integer nnn is

exp⁡ ⁣(((64/9)1/3+o(1))(log⁡n)1/3(log⁡log⁡n)2/3)=Ln[1/3, (64/9)1/3],\exp\!\Big(\big((64/9)^{1/3}+o(1)\big)(\log n)^{1/3}(\log\log n)^{2/3}\Big) = L_n\big[1/3,\,(64/9)^{1/3}\big],exp(((64/9)1/3+o(1))(logn)1/3(loglogn)2/3)=Ln​[1/3,(64/9)1/3],

super-polynomial but sub-exponential in the bit length of nnn. Every record factorization of a general RSA modulus of recent decades (RSA-768, RSA-240, RSA-250) was obtained with it, so the security margins of RSA key sizes are calibrated against it (Pomerance, A Tale of Two Sieves, 1996; Boudot et al., 2020).

Like the rational and quadratic sieves, GNFS works by producing a congruence of squares x2≡y2(modn)x^2 \equiv y^2 \pmod nx2≡y2(modn) and then taking gcd⁡(x−y,n)\gcd(x-y,n)gcd(x−y,n). Its gain comes from searching for smooth values that are sub-exponential in the size of nnn, which forces the algorithm to compute in algebraic number fields.

Setting

Let f∈Z[x]f \in \mathbb{Z}[x]f∈Z[x] be a polynomial of degree ddd and θ∈C\theta \in \mathbb{C}θ∈C a root of fff. The number field Q(θ)\mathbb{Q}(\theta)Q(θ) is the set of complex numbers ∑i<daiθi\sum_{i<d} a_i\theta^i∑i<d​ai​θi with ai∈Qa_i \in \mathbb{Q}ai​∈Q; it is ddd-dimensional over Q\mathbb{Q}Q when fff is irreducible over Q\mathbb{Q}Q. The ring Z[θ]\mathbb{Z}[\theta]Z[θ] is the subring of C\mathbb{C}C generated by θ\thetaθ; the ring of integers OQ(θ)\mathcal{O}_{\mathbb{Q}(\theta)}OQ(θ)​ consists of the elements of Q(θ)\mathbb{Q}(\theta)Q(θ) that are roots of monic integer polynomials. It contains Z[θ]\mathbb{Z}[\theta]Z[θ] when fff is monic, and the two can differ.

GNFS chooses two irreducible integer polynomials f1,f2f_1, f_2f1​,f2​ with a common root mmm modulo nnn, i.e. n∣f1(m)n \mid f_1(m)n∣f1​(m) and n∣f2(m)n \mid f_2(m)n∣f2​(m). A simple choice is the base-mmm polynomial: write n=admd+⋯+a1m+a0n = a_d m^d + \dots + a_1 m + a_0n=ad​md+⋯+a1​m+a0​ with digits 0≤ai<m0 \le a_i < m0≤ai​<m, put f1(x)=∑aixif_1(x) = \sum a_i x^if1​(x)=∑ai​xi and f2(x)=x−mf_2(x) = x - mf2​(x)=x−m. Pairs of integers (a,b)(a,b)(a,b) (relations) are sieved so that both homogenized values Fj(a,b)=bdeg⁡fjfj(a/b)F_j(a,b) = b^{\deg f_j} f_j(a/b)Fj​(a,b)=bdegfj​fj​(a/b) are smooth; up to the leading coefficient these are the norms N(a−bθj)N(a - b\theta_j)N(a−bθj​). Linear algebra over F2\mathbb{F}_2F2​ then selects a set SSS of relations for which

∏(a,b)∈S(a−bθ1)=γ12,γ1∈Z[θ1],∏(a,b)∈S(a−bθ2)=γ22,γ2∈Z[θ2].\prod_{(a,b)\in S}(a-b\theta_1) = \gamma_1^2,\quad \gamma_1 \in \mathbb{Z}[\theta_1], \qquad \prod_{(a,b)\in S}(a-b\theta_2) = \gamma_2^2,\quad \gamma_2 \in \mathbb{Z}[\theta_2].(a,b)∈S∏​(a−bθ1​)=γ12​,γ1​∈Z[θ1​],(a,b)∈S∏​(a−bθ2​)=γ22​,γ2​∈Z[θ2​].

Because mmm is a root of both polynomials mod nnn, there are ring homomorphisms φj:Z[θj]→Z/nZ\varphi_j : \mathbb{Z}[\theta_j] \to \mathbb{Z}/n\mathbb{Z}φj​:Z[θj​]→Z/nZ with φj(θj)=m\varphi_j(\theta_j) = mφj​(θj​)=m. Both send ∏S(a−bθj)\prod_S(a - b\theta_j)∏S​(a−bθj​) to ∏S(a−bm)\prod_S(a - bm)∏S​(a−bm).

Formalization targets

Goal: the congruence of squares

For f1,f2f_1, f_2f1​,f2​ irreducible in Z[x]\mathbb{Z}[x]Z[x] with complex roots θ1,θ2\theta_1,\theta_2θ1​,θ2​, a common root mmm mod nnn, and SSS, γ1\gamma_1γ1​, γ2\gamma_2γ2​ as above:

∃ φj:Z[θj]→Z/nZ, φj(θj)=m,and every such pair satisfiesφ1(γ1)2=φ2(γ2)2.\exists\,\varphi_j:\mathbb{Z}[\theta_j]\to\mathbb{Z}/n\mathbb{Z},\ \varphi_j(\theta_j)=m, \qquad\text{and every such pair satisfies}\qquad \varphi_1(\gamma_1)^2 = \varphi_2(\gamma_2)^2 .∃φj​:Z[θj​]→Z/nZ, φj​(θj​)=m,and every such pair satisfiesφ1​(γ1​)2=φ2​(γ2​)2.

This is the correctness statement of the algebraic part of GNFS: whatever relations the sieve and linear algebra produce, the square-root step yields x=φ1(γ1)x = \varphi_1(\gamma_1)x=φ1​(γ1​), y=φ2(γ2)y = \varphi_2(\gamma_2)y=φ2​(γ2​) with n∣x2−y2n \mid x^2 - y^2n∣x2−y2.

Supporting statements (milestones)

  1. [Q(θ):Q]=d[\mathbb{Q}(\theta):\mathbb{Q}] = d[Q(θ):Q]=d for fff irreducible over Q\mathbb{Q}Q.
  2. Z[θ]\mathbb{Z}[\theta]Z[θ] can be strictly smaller than the ring of integers.
  3. The base-mmm polynomial has digits 0≤ai<m0\le a_i<m0≤ai​<m as coefficients and f(m)=nf(m)=nf(m)=n, so mmm is a root mod nnn.
  4. Existence of the homomorphism Z[θ]→Z/nZ\mathbb{Z}[\theta]\to\mathbb{Z}/n\mathbb{Z}Z[θ]→Z/nZ, θ↦m\theta\mapsto mθ↦m.
  5. cd NQ(θ)/Q(a−bθ)=bdf(a/b)c_d\,N_{\mathbb{Q}(\theta)/\mathbb{Q}}(a-b\theta) = b^d f(a/b)cd​NQ(θ)/Q​(a−bθ)=bdf(a/b), where cdc_dcd​ is the leading coefficient.
  6. If n∣x2−y2n\mid x^2-y^2n∣x2−y2, n∤x−yn\nmid x-yn∤x−y, n∤x+yn\nmid x+yn∤x+y, then 1<gcd⁡(x−y,n)<n1<\gcd(x-y,n)<n1<gcd(x−y,n)<n.
  7. For odd nnn with at least two prime factors and a unit xxx, at least half of the square roots of x2x^2x2 mod nnn differ from ±x\pm x±x (the "probability at least 1/21/21/2" of the final step).

Significance

The goal and milestones together certify that every output of the GNFS pipeline that passes the square-root step is a genuine congruence of squares, and that such a congruence splits nnn with probability at least 1/21/21/2 over the choice of square root. This is the part of the algorithm whose correctness is unconditional; the running-time bound is heuristic and is not a target here.

These results are classical and appear in standard references (Lenstra–Lenstra 1993; Crandall–Pomerance 2005, §6.2). The mission's contribution is a machine-checked formal version connecting number fields in C\mathbb{C}C, integer polynomials, and residue rings, which current libraries do not package for this purpose.

Difficulty

The ring homomorphism Z[θ]→Z/nZ\mathbb{Z}[\theta] \to \mathbb{Z}/n\mathbb{Z}Z[θ]→Z/nZ is the delicate point. Z[θ]\mathbb{Z}[\theta]Z[θ] is a subring of C\mathbb{C}C, not a quotient ring, so a map defined by θ↦m\theta \mapsto mθ↦m is well defined only if every integer polynomial vanishing at θ\thetaθ is a multiple of fff in Z[x]\mathbb{Z}[x]Z[x]. This needs fff irreducible over Z\mathbb{Z}Z (in particular primitive), via Gauss's lemma; for f(x)=2xf(x) = 2xf(x)=2x and n=2n = 2n=2, every mmm is a root mod nnn, but θ=0\theta = 0θ=0 only admits θ↦0\theta \mapsto 0θ↦0. The norm identity requires identifying f/cdf/c_df/cd​ as the minimal polynomial of θ\thetaθ and expressing the norm as a product over conjugates. The probability milestone needs the Chinese remainder theorem and counting square roots of units modulo odd prime powers.

Formalization scope

All statements live in the namespace GNFS. Number fields are realized inside C\mathbb{C}C: Q(θ)\mathbb{Q}(\theta)Q(θ) is ℚ⟮θ⟯ and Z[θ]\mathbb{Z}[\theta]Z[θ] is Algebra.adjoin ℤ {θ}. Residues mod nnn are ZMod n with n∈Nn \in \mathbb{N}n∈N (n=0n = 0n=0 gives Z\mathbb{Z}Z, consistent with every statement). Two definitions are shared: GNFS.baseMPolynomial n m, the polynomial whose coefficients are the base-mmm digits of nnn (via Nat.digits), and GNFS.homogenize f a b =∑i≤dciaibd−i= \sum_{i\le d} c_i a^i b^{d-i}=∑i≤d​ci​aibd−i.

Irreducibility "over the rationals" with integer coefficients is encoded as irreducibility in Z[x]\mathbb{Z}[x]Z[x] (primitive and irreducible over Q\mathbb{Q}Q) where a homomorphism to Z/nZ\mathbb{Z}/n\mathbb{Z}Z/nZ is needed. Without primitivity the claimed homomorphism can fail to exist. The goal asserts both the existence of the homomorphisms and the equality for every such pair, so it cannot be satisfied by the trivial choice x=yx = yx=y. The sieving, smoothness, linear-algebra and complexity aspects of the article are out of scope.

Reusable by-products: norms of linear elements in simple extensions, homomorphisms out of Z[θ]\mathbb{Z}[\theta]Z[θ], and square-root counting in Z/nZ\mathbb{Z}/n\mathbb{Z}Z/nZ.

Selected references

  • Wikipedia, General number field sieve, revision 1377718368. https://en.wikipedia.org/w/index.php?title=General_number_field_sieve&oldid=1377718368
  • C. Pomerance, A Tale of Two Sieves, Notices of the AMS 43(12), 1996. https://www.ams.org/notices/199612/pomerance.pdf
  • A. K. Lenstra, H. W. Lenstra Jr. (eds.), The development of the number field sieve, Lecture Notes in Math. 1554, Springer, 1993. https://doi.org/10.1007/BFb0091534
  • R. Crandall, C. Pomerance, Prime Numbers: A Computational Perspective, 2nd ed., Springer, 2005, §6.2. https://doi.org/10.1007/0-387-28979-8
  • F. Boudot et al., Comparing the difficulty of factorization and discrete logarithm: a 240-digit experiment, CRYPTO 2020. https://eprint.iacr.org/2020/697
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Functional AnalysisHarmonic Analysis·Captain: Lucas

Schwartz Space (Wikipedia): the Fourier Transform is an Automorphism of 𝒮(ℝⁿ)Textbook

Motivation

The Schwartz space S(Rn)\mathcal{S}(\mathbb{R}^n)S(Rn) of smooth, rapidly decreasing functions is the standard domain on which Fourier analysis on Rn\mathbb{R}^nRn works without integrability caveats. Its defining property, singled out in the lead of the source article, is that the Fourier transform maps S(Rn)\mathcal{S}(\mathbb{R}^n)S(Rn) isomorphically onto itself. By duality this allows the Fourier transform to be defined on the dual space S′(Rn)\mathcal{S}'(\mathbb{R}^n)S′(Rn) of tempered distributions, which is the setting of the modern theory of linear partial differential equations (Hörmander, Vol. I) and of much of mathematical physics (Reed–Simon, Vol. I). The space is named after Laurent Schwartz.

This mission formalizes the definition and the elementary analytic properties of S(Rn)\mathcal{S}(\mathbb{R}^n)S(Rn) exactly as stated in the Wikipedia article Schwartz space (revision 1360762580), with the Fourier-automorphism property as the goal.

Setting

Write Rn\mathbb{R}^nRn for the coordinate space with the Euclidean norm ∣x∣=(x12+⋯+xn2)1/2|x| = (x_1^2 + \dots + x_n^2)^{1/2}∣x∣=(x12​+⋯+xn2​)1/2 and Lebesgue measure. A multi-index is a tuple α=(α1,…,αn)∈Nn\alpha = (\alpha_1, \dots, \alpha_n) \in \mathbb{N}^nα=(α1​,…,αn​)∈Nn, and xα=x1α1⋯xnαnx^\alpha = x_1^{\alpha_1} \cdots x_n^{\alpha_n}xα=x1α1​​⋯xnαn​​. For a function f:Rn→Cf : \mathbb{R}^n \to \mathbb{C}f:Rn→C, ∂if\partial_i f∂i​f denotes the partial derivative in the iii-th coordinate direction and

Dβf=∂1β1⋯∂nβnf.D^\beta f = \partial_1^{\beta_1} \cdots \partial_n^{\beta_n} f .Dβf=∂1β1​​⋯∂nβn​​f.

For α,β∈Nn\alpha, \beta \in \mathbb{N}^nα,β∈Nn put

∥f∥α,β=sup⁡x∈Rn∣xα(Dβf)(x)∣∈[0,∞].\|f\|_{\alpha,\beta} = \sup_{x \in \mathbb{R}^n} \bigl| x^\alpha (D^\beta f)(x) \bigr| \in [0, \infty].∥f∥α,β​=x∈Rnsup​​xα(Dβf)(x)​∈[0,∞].

The Schwartz space is

S(Rn,C)={f∈C∞(Rn,C):∥f∥α,β<∞ for all α,β∈Nn}.\mathcal{S}(\mathbb{R}^n, \mathbb{C}) = \bigl\{ f \in C^\infty(\mathbb{R}^n, \mathbb{C}) : \|f\|_{\alpha,\beta} < \infty \text{ for all } \alpha, \beta \in \mathbb{N}^n \bigr\}.S(Rn,C)={f∈C∞(Rn,C):∥f∥α,β​<∞ for all α,β∈Nn}.

Informally, fff and all its derivatives decay at infinity faster than any reciprocal power of ∣x∣|x|∣x∣.

The Fourier transform of f:Rn→Cf : \mathbb{R}^n \to \mathbb{C}f:Rn→C is

(Ff)(ξ)=∫Rne−2πi⟨x,ξ⟩f(x) dx.(\mathcal{F} f)(\xi) = \int_{\mathbb{R}^n} e^{-2\pi i \langle x, \xi \rangle} f(x) \, dx .(Ff)(ξ)=∫Rn​e−2πi⟨x,ξ⟩f(x)dx.

In the Lean development these objects are SchwartzSpaceWiki.monomial, partialDeriv, iteratedPartialDeriv, schwartzSeminorm, schwartzSpace n and fourierTransform.

Formalization targets

Goal: the Fourier transform is an automorphism of S(Rn)\mathcal{S}(\mathbb{R}^n)S(Rn)

F:S(Rn)→S(Rn) is a linear bijection.\mathcal{F} : \mathcal{S}(\mathbb{R}^n) \to \mathcal{S}(\mathbb{R}^n) \text{ is a linear bijection.}F:S(Rn)→S(Rn) is a linear bijection.

Formally: Set.BijOn fourierTransform (schwartzSpace n) (schwartzSpace n) together with F(f+cg)=Ff+c Fg\mathcal{F}(f + c g) = \mathcal{F} f + c\,\mathcal{F} gF(f+cg)=Ff+cFg for f,g∈S(Rn)f, g \in \mathcal{S}(\mathbb{R}^n)f,g∈S(Rn) and c∈Cc \in \mathbb{C}c∈C.

Milestones (in the order of the source)

  1. S(Rn)\mathcal{S}(\mathbb{R}^n)S(Rn) is a complex linear subspace of C∞(Rn,C)C^\infty(\mathbb{R}^n, \mathbb{C})C∞(Rn,C).
  2. xαe−a∣x∣2∈S(Rn)x^\alpha e^{-a|x|^2} \in \mathcal{S}(\mathbb{R}^n)xαe−a∣x∣2∈S(Rn) for every multi-index α\alphaα and every a>0a > 0a>0.
  3. Cc∞(Rn)⊆S(Rn)C_c^\infty(\mathbb{R}^n) \subseteq \mathcal{S}(\mathbb{R}^n)Cc∞​(Rn)⊆S(Rn): smooth compactly supported functions are Schwartz functions.
  4. P(x)e−a∣x∣2∈S(Rn)P(x) e^{-a|x|^2} \in \mathcal{S}(\mathbb{R}^n)P(x)e−a∣x∣2∈S(Rn) for every polynomial PPP and a>0a > 0a>0, and P↦Pe−a∣x∣2P \mapsto P e^{-a|x|^2}P↦Pe−a∣x∣2 is injective.
  5. f,g∈S(Rn)⇒fg∈S(Rn)f, g \in \mathcal{S}(\mathbb{R}^n) \Rightarrow fg \in \mathcal{S}(\mathbb{R}^n)f,g∈S(Rn)⇒fg∈S(Rn).
  6. If f∈S(Rn)f \in \mathcal{S}(\mathbb{R}^n)f∈S(Rn) and ggg is smooth and bounded with all its derivatives, then fg∈S(Rn)fg \in \mathcal{S}(\mathbb{R}^n)fg∈S(Rn).
  7. Every f∈S(Rn)f \in \mathcal{S}(\mathbb{R}^n)f∈S(Rn) is Lipschitz, hence uniformly continuous.
  8. For 1≤p<∞1 \le p < \infty1≤p<∞, S(Rn)⊆Lp(Rn)\mathcal{S}(\mathbb{R}^n) \subseteq L^p(\mathbb{R}^n)S(Rn)⊆Lp(Rn) and it is dense there.

Significance

The result itself. The automorphism property is what makes S(Rn)\mathcal{S}(\mathbb{R}^n)S(Rn) the natural test-function space for tempered distributions: the Fourier transform of a tempered distribution TTT is defined by ⟨FT,φ⟩=⟨T,Fφ⟩\langle \mathcal{F} T, \varphi \rangle = \langle T, \mathcal{F} \varphi \rangle⟨FT,φ⟩=⟨T,Fφ⟩, which only makes sense because Fφ\mathcal{F}\varphiFφ is again a Schwartz function. Density in LpL^pLp (milestone 8) is what lets identities proved on Schwartz functions, such as Plancherel's theorem, extend to L2L^2L2 and other LpL^pLp spaces. The closure properties (milestones 1, 5, 6) say that S(Rn)\mathcal{S}(\mathbb{R}^n)S(Rn) is an algebra and a module over smooth functions with bounded derivatives.

Formalizing it. All results here are classical. Mathlib contains a Schwartz-space type SchwartzMap built on iterated Fréchet derivatives and the norm ∥x∥k\|x\|^k∥x∥k, together with a Fourier transform on it. This mission instead states everything for the concrete, coordinate-wise multi-index definition used in the source. A complete development therefore includes a proof that the two definitions agree, which is reusable on its own.

Difficulty

The multi-index seminorms sup⁡∣xαDβf∣\sup |x^\alpha D^\beta f|sup∣xαDβf∣ are coordinate-wise, while the standard library works with the total derivative and the full norm ∣x∣k|x|^k∣x∣k. The comparison needs inequalities in both directions between ∣xα∣|x^\alpha|∣xα∣ and powers of ∣x∣|x|∣x∣, and between the iterated partial derivatives DβfD^\beta fDβf and the norm of the kkk-th Fréchet derivative. For the goal, surjectivity is the hard part: it needs the Fourier inversion formula on S(Rn)\mathcal{S}(\mathbb{R}^n)S(Rn), not only the fact that F\mathcal{F}F preserves decay and smoothness. For milestone 8, density requires approximating arbitrary LpL^pLp functions, e.g. by compactly supported smooth functions, and this does not follow from the definition of S\mathcal{S}S alone.

Formalization scope

  • Rn\mathbb{R}^nRn is EuclideanSpace ℝ (Fin n) (Euclidean norm, Lebesgue volume). Functions take values in C\mathbb{C}C. n=0n = 0n=0 is allowed.
  • Smoothness is ContDiff ℝ (⊤ : ℕ∞), i.e. C∞C^\inftyC∞ (not analyticity).
  • ∂if(x)\partial_i f(x)∂i​f(x) is fderiv ℝ f x (EuclideanSpace.single i 1), and DβD^\betaDβ applies ∂1β1,…,∂nβn\partial_1^{\beta_1}, \dots, \partial_n^{\beta_n}∂1β1​​,…,∂nβn​​ in a fixed order. For smooth fff the order does not matter.
  • The seminorm ∥f∥α,β\|f\|_{\alpha,\beta}∥f∥α,β​ is a supremum in [0,∞][0, \infty][0,∞] (ℝ≥0∞), so "<∞< \infty<∞" really means bounded. A real-valued supremum would return 000 on unbounded sets and trivialize the definition.
  • The source does not fix a Fourier normalisation. The convention e−2πi⟨x,ξ⟩e^{-2\pi i\langle x,\xi\rangle}e−2πi⟨x,ξ⟩ is used. fourierTransform is a Bochner integral, which is 000 for non-integrable integrands. Every target only applies it to Schwartz functions, which are integrable.
  • The goal is stated as a bijection of the set schwartzSpace n onto itself plus linearity on it. It does not presuppose that schwartzSpace n has been given a module structure.
  • Not included: the topological statements of the source (that S(Rn)\mathcal{S}(\mathbb{R}^n)S(Rn) is a nuclear Montel Fréchet space, ultrabornological, reflexive, etc., and the corresponding facts for its strong dual). They require equipping the set with its seminorm topology, which this mission does not define. They are natural follow-up missions.

Contributions welcome: the equivalence with Mathlib's SchwartzMap, coordinate–norm comparison lemmas for xαx^\alphaxα, and the Leibniz rule for iteratedPartialDeriv.

Selected references

  • Wikipedia contributors, Schwartz space, revision 1360762580. https://en.wikipedia.org/w/index.php?title=Schwartz_space&oldid=1360762580
  • L. Hörmander, The Analysis of Linear Partial Differential Operators I, 2nd ed., Springer, 1990. ISBN 3-540-52343-X.
  • M. Reed, B. Simon, Methods of Modern Mathematical Physics I: Functional Analysis, revised ed., Academic Press, 1980. ISBN 0-12-585050-6.
  • E. M. Stein, R. Shakarchi, Fourier Analysis: An Introduction, Princeton University Press, 2003. ISBN 0-691-11384-X.
  • F. Trèves, Topological Vector Spaces, Distributions and Kernels, Dover, 2006 [1967]. ISBN 978-0-486-45352-1.
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Quantum Information·Captain: Goku

Lecture Notes on Quantum Algorithms 23: Trace inequality |tr(XYZ)| ≤ ‖X‖_F ‖Y‖ ‖Z‖_FTextbook

Motivation

This mission develops Chapter 23 of Lecture Notes on Quantum Algorithms by Andrew Childs. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

Let m,n≥0m,n\ge 0m,n≥0 be integers and let X∈Cm×nX\in\mathbb C^{m\times n}X∈Cm×n, Y∈Cn×nY\in\mathbb C^{n\times n}Y∈Cn×n and Z∈Cn×mZ\in\mathbb C^{n\times m}Z∈Cn×m be complex matrices. Write ∥A∥F\|A\|_F∥A∥F​ for the Frobenius norm, ∥A∥F2=∑a,b∣Aab∣2\|A\|_F^2=\sum_{a,b}|A_{ab}|^2∥A∥F2​=∑a,b​∣Aab​∣2, and ∥Y∥\|Y\|∥Y∥ for the spectral (operator) norm of YYY, i.e. its largest singular value. Then

∣tr⁡(XYZ)∣≤∥X∥F ∥Y∥ ∥Z∥F.|\operatorname{tr}(XYZ)| \le \|X\|_F\,\|Y\|\,\|Z\|_F .∣tr(XYZ)∣≤∥X∥F​∥Y∥∥Z∥F​.

In the generalized adversary method this inequality bounds both the final value of the weight function for Boolean functions and how much one query can change it.

Formalization Note The index sets are {0,…,m−1}\{0,\dots,m-1\}{0,…,m−1} and {0,…,n−1}\{0,\dots,n-1\}{0,…,n−1}; the Frobenius norm is frobNorm and the spectral norm is specNorm (Mathlib's ℓ2\ell^2ℓ2 operator norm on matrices). When m=0m=0m=0 or n=0n=0n=0 both sides are 000.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Proposition 23.2: Trace inequality |tr(XYZ)| ≤ ‖X‖_F ‖Y‖ ‖Z‖_F.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Andrew Childs, Lecture Notes on Quantum Algorithms, 17 April 2025. https://www.cs.umd.edu/~amchilds/qa/qa.pdf.
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Machine LearningQuantum Information·Captain: Goku

A Survey of Quantum Learning Theory 5: Atıcı–Servedio: time-efficient quantum learning of k-juntas (corrected)Textbook

Motivation

This mission develops Chapter 5 of A Survey of Quantum Learning Theory by Srinivasan Arunachalam and Ronald de Wolf. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

This is a corrected form of the Atıcı–Servedio theorem on learning juntas from uniform quantum examples.

A function f:{0,1}n→{0,1}f:\{0,1\}^n\to\{0,1\}f:{0,1}n→{0,1} is a kkk-junta if it depends on at most kkk of its nnn input bits. A uniform quantum example of fff is the (n+1)(n+1)(n+1)-qubit state ∑x∈{0,1}n2−n/2∣x,f(x)⟩\sum_{x\in\{0,1\}^n}2^{-n/2}|x,f(x)\rangle∑x∈{0,1}n​2−n/2∣x,f(x)⟩; a uniform classical example is a pair (x,f(x))(x,f(x))(x,f(x)) with xxx uniform on {0,1}n\{0,1\}^n{0,1}n. The error of a hypothesis hhh is Pr⁡x[h(x)≠f(x)]\Pr_{x}[h(x)\neq f(x)]Prx​[h(x)=f(x)] for uniform xxx.

Time is measured in the following hybrid cost model, which is the one the source's proof sketch counts in. A learner (1) applies a circuit over the gate set {H,T,CNOT}\{H,T,\mathrm{CNOT}\}{H,T,CNOT} to TQT_QTQ​ uniform quantum examples and some ancillas in ∣0⟩|0\rangle∣0⟩ and measures every qubit in the computational basis; (2) maps the outcome by a Boolean circuit of AND/OR/NOT gates to a set V⊆[n]V\subseteq[n]V⊆[n] of variables; (3) reads TCT_CTC​ uniform classical examples and outputs the truth-table hypothesis h(x)=f(xj)h(x)=f(x_j)h(x)=f(xj​) for the first example xjx_jxj​ that agrees with xxx on VVV (h(x)=0h(x)=0h(x)=0 if there is none). Its time is the number of quantum gates, plus the number of measured qubits, plus the number of Boolean gates, plus TCT_CTC​ (one unit per classical example, which is read and written into the table cell indexed by its VVV-bits), plus 2∣V∣2^{|V|}2∣V∣ table cells (worst case over the outcomes).

For every δ∈(0,1)\delta\in(0,1)δ∈(0,1) there is a constant C>0C>0C>0 such that for all n,kn,kn,k with 2≤k≤n2\le k\le n2≤k≤n and all ε∈(0,1/2]\varepsilon\in(0,1/2]ε∈(0,1/2] there is such a learner with

TQ≤C klog⁡kε,TC≤C 2klog⁡1ε,time≤C(nklog⁡kε+2klog⁡1ε),T_Q\le C\,\frac{k\log k}{\varepsilon},\qquad T_C\le C\,2^k\log\frac1\varepsilon,\qquad \mathrm{time}\le C\Big(\frac{nk\log k}{\varepsilon}+2^k\log\frac1\varepsilon\Big),TQ​≤Cεklogk​,TC​≤C2klogε1​,time≤C(εnklogk​+2klogε1​),

which, for every kkk-junta fff, outputs with probability at least 1−δ1-\delta1−δ (over the measurement outcomes and the classical examples) a hypothesis of error at most ε\varepsilonε.

The theorem shows that quantum examples remove the nΘ(k)n^{\Theta(k)}nΘ(k) search over candidate variable sets that the best known classical learners need, which is why juntas are a notorious bottleneck classically.

Formalization Note The source states no cost model, no confidence parameter, and O(2k)O(2^k)O(2k) classical examples. The cost model above, the fixed-confidence reading (constants depend on δ\deltaδ only), and the O(2klog⁡(1/ε))O(2^k\log(1/\varepsilon))O(2klog(1/ε)) classical examples of the source's own proof sketch are the corrections. The thresholds k≥2k\ge2k≥2 and ε≤1/2\varepsilon\le1/2ε≤1/2 make log⁡k\log klogk and log⁡(1/ε)\log(1/\varepsilon)log(1/ε) positive.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Theorem 5.4: Atıcı–Servedio: time-efficient quantum learning of k-juntas (corrected).

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Srinivasan Arunachalam and Ronald de Wolf, A Survey of Quantum Learning Theory, 2017, v3. https://arxiv.org/pdf/1701.06806v3.
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Quantum Error CorrectionQuantum Information·Captain: Goku

An Introduction to Quantum Error Correction and Fault-Tolerant Quantum Computation 3: Every error syndrome of a stabilizer is realized by a Pauli errorTextbook

Motivation

This mission develops Chapter 3 of An Introduction to Quantum Error Correction and Fault-Tolerant Quantum Computation by Daniel Gottesman. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

Let Pn\mathcal P_nPn​ be the nnn-qubit Pauli group and let g1,…,ga∈Png_1,\dots,g_a\in\mathcal P_ng1​,…,ga​∈Pn​ generate a stabilizer S=⟨g1,…,ga⟩S=\langle g_1,\dots,g_a\rangleS=⟨g1​,…,ga​⟩, that is, an Abelian subgroup of Pn\mathcal P_nPn​ with −I∉S-I\notin S−I∈/S, and suppose the generators are independent, i.e. ∣S∣=2a|S|=2^a∣S∣=2a. The error syndrome of a Pauli operator EEE is the vector in F2a\mathbb F_2^aF2a​ whose iii-th bit is 000 if gig_igi​ commutes with EEE and 111 if it anticommutes.

Then for every v∈F2av\in\mathbb F_2^av∈F2a​ there is E∈PnE\in\mathcal P_nE∈Pn​ with syndrome vvv:

giE=Egi  if vi=0,giE=−Egi  if vi=1(i=1,…,a).g_iE=Eg_i\ \text{ if } v_i=0,\qquad g_iE=-Eg_i\ \text{ if } v_i=1\qquad(i=1,\dots,a).gi​E=Egi​  if vi​=0,gi​E=−Egi​  if vi​=1(i=1,…,a).

This lemma is the step in the proof of the dimension count of stabilizer codes (Theorem 5) that shows all 2a2^a2a syndrome subspaces are nonempty.

Formalization Note The syndrome is relative to the generator list, as in the source's proof; the independence of the generators (used in the proof as linear independence of their binary vectors) is the hypothesis ∣S∣=2a|S|=2^a∣S∣=2a. The anticommutation clause is stated explicitly.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Theorem 5: Stabilizer codes: an Abelian S of order 2^a without -1 gives an [[n, n-a, d]] code.
  • Lemma 1: Every error syndrome of a stabilizer is realized by a Pauli error.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Daniel Gottesman, An Introduction to Quantum Error Correction and Fault-Tolerant Quantum Computation, 2009, v1. https://arxiv.org/pdf/0904.2557v1.
3 thms2 active usersReviewed
Quantum Error CorrectionQuantum Information·Captain: Goku

Stabilizer Codes and Quantum Error Correction 4: The standard-form encoding network maps |c⟩ to the encoded basis state (4.8)Textbook

Motivation

This mission develops Chapter 4 of Stabilizer Codes and Quantum Error Correction by Daniel Gottesman. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

Let a stabilizer on n=m+kn=m+kn=m+k qubits (m=n−km=n-km=n−k generators) be given in the standard form (4.3) of §4.1,

(IA1A2BC1C2000DIE),\left(\begin{array}{ccc|ccc} I & A_1 & A_2 & B & C_1 & C_2\\ 0 & 0 & 0 & D & I & E\end{array}\right),(I0​A1​0​A2​0​BD​C1​I​C2​E​),

with rrr rows in the first block, and assume its rows commute: HxHzT+HzHxT=0H_xH_z^{\mathsf T}+H_zH_x^{\mathsf T}=0Hx​HzT​+Hz​HxT​=0. For a binary row (a ∣ b)(a\,|\,b)(a∣b) write P(a∣b)=⨂qσzbqσxaqP(a|b)=\bigotimes_q \sigma_z^{b_q}\sigma_x^{a_q}P(a∣b)=⨂q​σzbq​​σxaq​​ (the real form, sign +1+1+1). Let Mi=P(row i)M_i=P(\text{row } i)Mi​=P(row i) be the generators and let Xˉ1,…,Xˉk\bar X_1,\dots,\bar X_kXˉ1​,…,Xˉk​ be the logical σx\sigma_xσx​ operators in the standard form of p.40: Xˉi=P(0 u2 ei ∣ v1 0 0)\bar X_i=P(0\,u_2\,e_i\,|\,v_1\,0\,0)Xˉi​=P(0u2​ei​∣v1​00) with u2u_2u2​ the iii-th row of ETE^{\mathsf T}ET and v1v_1v1​ the iii-th row of ETC1T+C2TE^{\mathsf T}C_1^{\mathsf T}+C_2^{\mathsf T}ETC1T​+C2T​.

Let UencU_{\mathrm{enc}}Uenc​ be the encoding network of §4.2 (with the author's errata): first, for each iii, the controlled-NOTs that apply Xˉi\bar X_iXˉi​ without its final σx\sigma_xσx​, controlled on qubit n−k+in-k+in−k+i; then, for i=1,…,ri=1,\dots,ri=1,…,r in turn, the Hadamard RRR on qubit iii, a σz\sigma_zσz​ on qubit iii if Bii=1B_{ii}=1Bii​=1, and MiM_iMi​ without its qubit-iii factor, controlled on qubit iii (controlled-σzbσxa\sigma_z^{b}\sigma_x^{a}σzb​σxa​ gates). Then for every c=c1…ck∈{0,1}kc=c_1\dots c_k\in\{0,1\}^kc=c1​…ck​∈{0,1}k,

Uenc ∣0…0⟩∣c1…ck⟩=(I+M1)⋯(I+Mn−k) Xˉ1c1⋯Xˉkck∣0…0⟩∥(I+M1)⋯(I+Mn−k) Xˉ1c1⋯Xˉkck∣0…0⟩∥,U_{\mathrm{enc}}\,|0\dots0\rangle|c_1\dots c_k\rangle=\frac{(I+M_1)\cdots(I+M_{n-k})\,\bar X_1^{c_1}\cdots\bar X_k^{c_k}|0\dots0\rangle}{\big\|(I+M_1)\cdots(I+M_{n-k})\,\bar X_1^{c_1}\cdots\bar X_k^{c_k}|0\dots0\rangle\big\|},Uenc​∣0…0⟩∣c1​…ck​⟩=​(I+M1​)⋯(I+Mn−k​)Xˉ1c1​​⋯Xˉkck​​∣0…0⟩​(I+M1​)⋯(I+Mn−k​)Xˉ1c1​​⋯Xˉkck​​∣0…0⟩​,

and in particular the vector on the right-hand side is nonzero.

This is the correctness of Gottesman's general encoding circuit for stabilizer codes: the network prepares exactly the encoded basis states, with no leftover global phase.

Formalization Note The errata are built in: the Hadamard on qubit iii comes just before that qubit's control operations, controlled-YYY gates are controlled-σzσx\sigma_z\sigma_xσz​σx​ gates in the real form, and every generator has sign +1+1+1. The page writes encoded states unnormalized; the unitary network yields the normalized vector. Since the real form σzσx=iσy\sigma_z\sigma_x=i\sigma_yσz​σx​=iσy​, a generator with an odd number of (1∣1)(1|1)(1∣1) positions is iii times a Hermitian Pauli operator; the identity is the one the page's network computes in this convention.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • §4.1: Every stabilizer code can be put into the standard form (4.3).
  • §4.2: The standard-form encoding network maps |c⟩ to the encoded basis state (4.8).

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Daniel Gottesman, Stabilizer Codes and Quantum Error Correction, 1997 thesis, downloaded arXiv v1 PDF; PDF title page now prints 2024. https://arxiv.org/pdf/quant-ph/9705052v1.
2 thms2 active usersReviewed
🏆Completed
OptimizationQuantum Information·Captain: Goku

Quantum algorithms for optimizers 3: Correctness of the digits computed by iterative phase estimation (corrected)Textbook

Motivation

This mission develops Chapter 3 of Quantum algorithms for optimizers by Giacomo Nannicini. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

Let φ∈[0,1)\varphi\in[0,1)φ∈[0,1) be a phase (in full turns), h∈Nh\in\mathbb Nh∈N (h=q−2h=q-2h=q−2), and let ω1,…,ωh\omega_1,\dots,\omega_hω1​,…,ωh​ be the angle estimates used by the iterative phase estimation algorithm of §3.3.2, ωi\omega_iωi​ being the estimate of 2i−1φ2^{i-1}\varphi2i−1φ. The algorithm computes binary digits p1,…,ph+2p_1,\dots,p_{h+2}p1​,…,ph+2​ as follows: phph+1ph+2p_hp_{h+1}p_{h+2}ph​ph+1​ph+2​ are the digits of ωh\omega_hωh​ rounded to the closest multiple of 1/81/81/8 (modulo 111); then for j=h−1,…,1j=h-1,\dots,1j=h−1,…,1, pj=0p_j=0pj​=0 if d(0.0pj+1pj+2,ωj)<1/4d(0.0p_{j+1}p_{j+2},\omega_j)<1/4d(0.0pj+1​pj+2​,ωj​)<1/4 and pj=1p_j=1pj​=1 otherwise. Here d(x,y)d(x,y)d(x,y) is the distance between xxx and yyy modulo 111.

Fix 1≤j≤h1\le j\le h1≤j≤h. If d(ωi,2i−1φ)≤1/16d(\omega_i,2^{i-1}\varphi)\le 1/16d(ωi​,2i−1φ)≤1/16 for every step i=h,h−1,…,ji=h,h-1,\dots,ji=h,h−1,…,j, then

d(0.pjpj+1…ph+2, 2j−1φ) ≤ 2−(h+3−j).d\big(0.p_jp_{j+1}\dots p_{h+2},\ 2^{j-1}\varphi\big)\ \le\ 2^{-(h+3-j)} .d(0.pj​pj+1​…ph+2​, 2j−1φ) ≤ 2−(h+3−j).

In particular, for j=1j=1j=1 the algorithm outputs q=h+2q=h+2q=h+2 binary digits of φ\varphiφ with error at most 2−q2^{-q}2−q on the circle, which together with a union bound over the hhh estimation steps gives the success guarantee of iterative phase estimation.

Formalization Note The page states the bound with plain absolute values and strict inequality. Both are corrected: angles are only known modulo 111 (so all distances are on the circle), and the strict bound already fails at the base case (ωh=1/16\omega_h=1/16ωh​=1/16 is equidistant from 000 and 1/81/81/8, and rounding gives error exactly 1/81/81/8); the induction proves ≤\le≤, matching the goal Pr⁡(min⁡{… }≤2−q)\Pr(\min\{\dots\}\le 2^{-q})Pr(min{…}≤2−q) on p.66. The digits are the shared definition ipeDigits h ω and 0.pj…ph+20.p_j\dots p_{h+2}0.pj​…ph+2​ is binFracFrom.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Proposition 3.14: Phase estimation on an inexact eigenstate succeeds with probability at least (1 − δ)|⟨ξ|ψ⟩|²*.
  • Proposition 3.16: Combining cosine and sine estimates into an angle estimate (corrected).
  • Proposition 3.17: Correctness of the digits computed by iterative phase estimation (corrected).

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Giacomo Nannicini, Quantum algorithms for optimizers, 2025, v5; notes dated 9 July 2025. https://arxiv.org/pdf/2408.07086v5.
3 thms2 active usersReviewed
OptimizationQuantum Information·Captain: Goku

Quantum algorithms for optimizers 9: QAOA with enough layers reaches a maximum eigenstate of H_FTextbook

Motivation

This mission develops Chapter 9 of Quantum algorithms for optimizers by Giacomo Nannicini. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

Let n≥0n \ge 0n≥0 and let f:{0,1}n→Rf : \{0,1\}^n \to \mathbb{R}f:{0,1}n→R be the objective of the maximization problem (9.38). Define the nnn-qubit Hamiltonians

HF=∑x∈{0,1}nf(x) ∣x⟩⟨x∣,HI=∑j=1nσjX,H_F = \sum_{x \in \{0,1\}^n} f(x)\,|x\rangle\langle x|, \qquad H_I = \sum_{j=1}^n \sigma_j^X,HF​=x∈{0,1}n∑​f(x)∣x⟩⟨x∣,HI​=j=1∑n​σjX​,

where σjX\sigma_j^XσjX​ is the Pauli XXX on qubit jjj and the identity elsewhere. For p≥1p \ge 1p≥1 and β,θ∈[0,2π]p\beta, \theta \in [0, 2\pi]^pβ,θ∈[0,2π]p let

UQAOA(p,β,θ)=e−iβpHIe−iθpHF⋯e−iβ1HIe−iθ1HF.U_{\mathrm{QAOA}}(p, \beta, \theta) = e^{-i\beta_p H_I} e^{-i\theta_p H_F} \cdots e^{-i\beta_1 H_I} e^{-i\theta_1 H_F}.UQAOA​(p,β,θ)=e−iβp​HI​e−iθp​HF​⋯e−iβ1​HI​e−iθ1​HF​.

Then for every δ>0\delta > 0δ>0 there are a unit vector ∣φ⟩|\varphi\rangle∣φ⟩ with HF∣φ⟩=(max⁡xf(x)) ∣φ⟩H_F|\varphi\rangle = (\max_x f(x))\,|\varphi\rangleHF​∣φ⟩=(maxx​f(x))∣φ⟩, that is an eigenstate of HFH_FHF​ with maximum eigenvalue, and an integer P≥1P \ge 1P≥1 such that for every p≥Pp \ge Pp≥P there are angles β∗,θ∗∈[0,2π]p\beta^*, \theta^* \in [0, 2\pi]^pβ∗,θ∗∈[0,2π]p with

∥UQAOA(p,β∗,θ∗) (H∣0⟩)⊗n−∣φ⟩∥≤δ.\bigl\| U_{\mathrm{QAOA}}(p, \beta^*, \theta^*)\,(H|0\rangle)^{\otimes n} - |\varphi\rangle \bigr\| \le \delta .​UQAOA​(p,β∗,θ∗)(H∣0⟩)⊗n−∣φ⟩​≤δ.

Here (H∣0⟩)⊗n(H|0\rangle)^{\otimes n}(H∣0⟩)⊗n is the uniform superposition, the maximum eigenstate of HIH_IHI​. The proposition says that with enough layers, the QAOA ansatz can reproduce adiabatic evolution along H(s)=(1−s)HI+sHFH(s) = (1-s)H_I + sH_FH(s)=(1−s)HI​+sHF​ and so prepares a state close to one encoding an optimal solution of (9.38).

Formalization Note The source's limit over ppp, with angles that depend on ppp, is stated as "for all sufficiently large ppp some angles achieve distance at most δ\deltaδ", with the target eigenvector fixed before ppp. The global phase allowed by Theorem 9.11 is absorbed into the choice of the eigenvector, since a phase multiple of a maximum eigenvector is again one. The informal claim that UQAOAU_{\mathrm{QAOA}}UQAOA​ "approximates an adiabatic evolution" is represented by its stated "in particular" consequence.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Proposition 9.4: The Ising Hamiltonian is diagonal with the QUBO objective values.
  • Theorem 9.11: Adiabatic theorem with T ≥ (10⁴/δ²)(‖H′‖³/γ⁴ + ‖H′‖‖H″‖/γ³).
  • Theorem 9.17: Adiabatic theorem when the tracked eigenvalue is identically 0.
  • Lemma 9.18: Derivative bounds for the phase-fixed instantaneous zero eigenvector.
  • Lemma 9.20: Replacing U_k ⋯ U_j by powers of U_1 in the discretized adiabatic evolution.
  • Corollary 9.21: The T-bound of Theorem 9.11 suffices (derived from Theorem 9.17).
  • Theorem 9.23: Adiabatic theorem with the integrated 1/γ³ gap dependence.
  • Corollary 9.24: Adiabatic theorem for the linear interpolation (1 − s)H_I + sH_F.
  • Proposition 9.28: QAOA with enough layers reaches a maximum eigenstate of H_F.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Giacomo Nannicini, Quantum algorithms for optimizers, 2025, v5; notes dated 9 July 2025. https://arxiv.org/pdf/2408.07086v5.
9 thms2 active usersReviewed
🏆Completed
Quantum Information·Captain: Goku

Lecture Notes on Quantum Algorithms 18: Spectral gap and marked fraction bound the norm of the unmarked blockTextbook

Motivation

This mission develops Chapter 18 of Lecture Notes on Quantum Algorithms by Andrew Childs. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

Let N≥2N \ge 2N≥2 and let PPP be a symmetric N×NN \times NN×N stochastic matrix (Pkj≥0P_{kj} \ge 0Pkj​≥0, ∑kPkj=1\sum_k P_{kj} = 1∑k​Pkj​=1 for all jjj, P=PTP = P^{\mathsf T}P=PT) describing a random walk on the vertex set V={1,…,N}V = \{1,\dots,N\}V={1,…,N}. Let M⊆VM \subseteq VM⊆V be a set of marked vertices and let PMP_MPM​ be the matrix obtained from PPP by deleting the rows and columns indexed by MMM. Let δ>0\delta > 0δ>0 and ϵ>0\epsilon > 0ϵ>0.

Lemma. If the second largest eigenvalue of PPP in absolute value is at most 1−δ1-\delta1−δ (that is, listing the eigenvalues of PPP with multiplicity, at most one has absolute value greater than 1−δ1-\delta1−δ) and ∣M∣≥ϵN|M| \ge \epsilon N∣M∣≥ϵN, then

∥PM∥≤1−δϵ,\|P_M\| \le 1 - \delta\epsilon,∥PM​∥≤1−δϵ,

where ∥⋅∥\|\cdot\|∥⋅∥ is the spectral (operator) norm.

Together with Pr⁡[no marked vertex after t steps]≤∥PM∥t\Pr[\text{no marked vertex after } t \text{ steps}] \le \|P_M\|^tPr[no marked vertex after t steps]≤∥PM​∥t, this gives the classical hitting time O(1/(δϵ))O(1/(\delta\epsilon))O(1/(δϵ)), and it is the input to the quantum walk search bound O(1/δϵ)O(1/\sqrt{\delta\epsilon})O(1/δϵ​).

Formalization Note N≥2N \ge 2N≥2 because the source speaks of a second eigenvalue, and δ,ϵ>0\delta, \epsilon > 0δ,ϵ>0 because they are a spectral gap and a fraction; without these the statement fails (e.g. N=1N = 1N=1, P=(1)P = (1)P=(1), M=VM = VM=V, δ=3\delta = 3δ=3, ϵ=1\epsilon = 1ϵ=1). Symmetry is stated as Hermitian, which for a real matrix is the same thing; the eigenvalues are the Mathlib eigenvalue list of the Hermitian matrix. If M=VM = VM=V, PMP_MPM​ is the empty matrix, of norm 000.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Theorem 18.1: Spectrum of the Szegedy quantum walk.
  • Lemma 18.2: Spectral gap and marked fraction bound the norm of the unmarked block.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Andrew Childs, Lecture Notes on Quantum Algorithms, 17 April 2025. https://www.cs.umd.edu/~amchilds/qa/qa.pdf.
2 thms2 active usersReviewed
🏆Completed
Quantum Information·Captain: Goku

Lecture Notes on Quantum Algorithms 2: Group commutators of an ϵ²-net of S_ϵ form an O(ϵ³)-net of S_{ϵ²}Textbook

Motivation

This mission develops Chapter 2 of Lecture Notes on Quantum Algorithms by Andrew Childs. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

For U,V∈SU(2)U,V\in SU(2)U,V∈SU(2) write [ ⁣[U,V] ⁣]=UVU−1V−1[\![U,V]\!]=UVU^{-1}V^{-1}[[U,V]]=UVU−1V−1 for the group commutator. For ϵ≥0\epsilon\ge0ϵ≥0 let

Sϵ={U∈SU(2):∥I−U∥≤ϵ}S_\epsilon=\{U\in SU(2):\|I-U\|\le\epsilon\}Sϵ​={U∈SU(2):∥I−U∥≤ϵ}

be the ϵ\epsilonϵ-ball around the identity, with ∥⋅∥\|\cdot\|∥⋅∥ the spectral norm. For Γ,S⊆SU(2)\Gamma,S\subseteq SU(2)Γ,S⊆SU(2), Γ\GammaΓ is a δ\deltaδ-net for SSS if every A∈SA\in SA∈S has some U∈ΓU\in\GammaU∈Γ with ∥A−U∥≤δ\|A-U\|\le\delta∥A−U∥≤δ.

The lemma says there are constants C>0C>0C>0 and ϵ0>0\epsilon_0>0ϵ0​>0 such that, for every 0<ϵ≤ϵ00<\epsilon\le\epsilon_00<ϵ≤ϵ0​ and every Γ⊆SU(2)\Gamma\subseteq SU(2)Γ⊆SU(2), the following holds. If Γ\GammaΓ is an ϵ2\epsilon^2ϵ2-net for SϵS_\epsilonSϵ​, then

[ ⁣[Γ,Γ] ⁣]={[ ⁣[U,V] ⁣]:U,V∈Γ} is a Cϵ3-net for Sϵ2.[\![\Gamma,\Gamma]\!]=\{[\![U,V]\!]:U,V\in\Gamma\}\ \text{is a } C\epsilon^3\text{-net for } S_{\epsilon^2}.[[Γ,Γ]]={[[U,V]]:U,V∈Γ} is a Cϵ3-net for Sϵ2​.

This is the key step of the Solovay–Kitaev construction. Applied recursively, it turns a coarse net near the identity into nets of doubly-exponentially improving precision.

Formalization Note The source writes O(ϵ3)O(\epsilon^3)O(ϵ3) as ϵ→0\epsilon\to0ϵ→0. Here it is written as explicit constants CCC and ϵ0\epsilon_0ϵ0​, chosen before Γ\GammaΓ, because the source's recursion uses one constant at every level.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Theorem 2.1: Solovay–Kitaev: gate-set independence with polylogarithmic overhead.
  • Lemma 2.2: Subadditivity of errors in products of unitaries.
  • Lemma 2.3: Group commutators of an ϵ²-net of S_ϵ form an O(ϵ³)-net of S_{ϵ²}.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Andrew Childs, Lecture Notes on Quantum Algorithms, 17 April 2025. https://www.cs.umd.edu/~amchilds/qa/qa.pdf.
6 thms2 active usersReviewed
Machine LearningQuantum Information·Captain: Goku

Quantum Algorithms and Learning Theory — Part II 6: Shadow tomography with poly(log m, log d, 1/ε, log(1/δ)) copiesTextbook

Motivation

This mission develops Chapter 6 of Quantum Algorithms and Learning Theory — Part II by Srinivasan Arunachalam. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

This is Aaronson's shadow tomography theorem.

A two-outcome measurement on Cd\mathbb C^dCd is a POVM {E,1−E}\{E,\mathbb 1-E\}{E,1−E} with 0⪯E⪯10\preceq E\preceq\mathbb 10⪯E⪯1. A learner using kkk copies of an unknown ddd-dimensional density matrix ρ\rhoρ performs a measurement (a POVM {No}o∈O\{N_o\}_{o\in O}{No​}o∈O​ with finite outcome set OOO) on ρ⊗k\rho^{\otimes k}ρ⊗k and outputs numbers b(o)=(b1(o),…,bm(o))∈[0,1]mb(o)=(b_1(o),\dots,b_m(o))\in[0,1]^mb(o)=(b1​(o),…,bm​(o))∈[0,1]m.

There is a polynomial ppp in four variables such that for all ε,δ∈(0,1]\varepsilon,\delta\in(0,1]ε,δ∈(0,1], all integers m,d>0m,d>0m,d>0 and all effects E1,…,EmE_1,\dots,E_mE1​,…,Em​ on Cd\mathbb C^dCd there exist k≤p(log⁡m,log⁡d,1/ε,log⁡(1/δ))k\le p(\log m,\log d,1/\varepsilon,\log(1/\delta))k≤p(logm,logd,1/ε,log(1/δ)) and such a learner (depending on m,d,ε,δm,d,\varepsilon,\deltam,d,ε,δ and E1,…,EmE_1,\dots,E_mE1​,…,Em​, but not on ρ\rhoρ) with

Pr⁡o∼{Tr⁡(Noρ⊗k)}[ ∀i∈[m]: ∣Tr⁡(Eiρ)−bi(o)∣≤ε ] ≥ 1−δ\Pr_{o\sim\{\operatorname{Tr}(N_o\rho^{\otimes k})\}}\Big[\ \forall i\in[m]:\ |\operatorname{Tr}(E_i\rho)-b_i(o)|\le\varepsilon\ \Big]\ \ge\ 1-\deltao∼{Tr(No​ρ⊗k)}Pr​[ ∀i∈[m]: ∣Tr(Ei​ρ)−bi​(o)∣≤ε ] ≥ 1−δ

for every ddd-dimensional density matrix ρ\rhoρ.

The number of copies is exponentially smaller in mmm and ddd than for full state tomography or for estimating each Tr⁡(Eiρ)\operatorname{Tr}(E_i\rho)Tr(Ei​ρ) separately.

Formalization Note The source writes ε,δ∈[0,1]\varepsilon,\delta\in[0,1]ε,δ∈[0,1]; the endpoints 000 are excluded because there 1/ε1/\varepsilon1/ε or log⁡(1/δ)\log(1/\delta)log(1/δ) is undefined. Internal randomness and post-processing of the learner are absorbed into the POVM; ρ⊗k\rho^{\otimes k}ρ⊗k is the kkk-fold Kronecker power and logarithms are natural (the base is absorbed by the polynomial).

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Lemma 6.4.8: A class of size at most M needing Ω(√((N−k+1)k)) quantum membership queries.
  • Fact 6.4.9: An admissible weight k of order log M/(log(N/log M)+1).
  • Theorem 6.6.2: Shadow tomography with poly(log m, log d, 1/ε, log(1/δ)) copies.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Srinivasan Arunachalam, Quantum Algorithms and Learning Theory — Part II, 2018 thesis, ILLC DS-2018-08. https://ir.cwi.nl/pub/27536/Thesis_S_Arunachalam.
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🏆Completed
OptimizationQuantum Information·Captain: Goku

Quantum algorithms for optimizers 6: Unitary conjugation commutes with the matrix exponential: e^{iUHU†t} = U e^{iHt} U†Textbook

Motivation

This mission develops Chapter 6 of Quantum algorithms for optimizers by Giacomo Nannicini. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

Let n≥0n \ge 0n≥0, let UUU be a unitary 2n×2n2^n \times 2^n2n×2n matrix, let H\mathcal{H}H be a Hamiltonian on nnn qubits, that is, a Hermitian 2n×2n2^n \times 2^n2n×2n complex matrix, and let t∈Rt \in \mathbb{R}t∈R. With the matrix exponential eA=∑k=0∞Ak/k!e^A = \sum_{k=0}^\infty A^k / k!eA=∑k=0∞​Ak/k!,

eiUHU†t=U eiHt U†.e^{iU\mathcal{H}U^\dagger t} = U\, e^{i\mathcal{H}t}\, U^\dagger.eiUHU†t=UeiHtU†.

This is what makes diagonalizable Hamiltonians easy to simulate: if UUU diagonalizes H\mathcal{H}H, simulating H\mathcal{H}H reduces to applying U†U^\daggerU†, a diagonal phase, and UUU.

Formalization Note The matrix exponential is Mathlib's power series NormedSpace.exp; U†U^\daggerU† is the conjugate transpose (star U). Hermiticity of H\mathcal{H}H is kept because the source says Hamiltonian (Def. 6.1), although the identity holds for every square matrix.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Proposition 6.9: Phase condition under which the clock Hamiltonian transports |u^(1)⟩ to e^{iϕ}|u^(N)⟩.
  • Proposition 6.12: Unitary conjugation commutes with the matrix exponential: e^{iUHU†t} = U e^{iHt} U†.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Giacomo Nannicini, Quantum algorithms for optimizers, 2025, v5; notes dated 9 July 2025. https://arxiv.org/pdf/2408.07086v5.
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🏆Completed
Quantum Information·Captain: Goku

Quantum Computing: Lecture Notes 7: Amplitude amplification: Q^k A|0^m⟩ = sin((2k+1)θ)|ψ1⟩ + cos((2k+1)θ)|ψ0⟩, and O(1/√p) rounds sufficeTextbook

Motivation

This mission develops Chapter 7 of Quantum Computing: Lecture Notes by Ronald de Wolf. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

Let AAA be a unitary on mmm qubits (a circuit without measurements) and p∈(0,1]p\in(0,1]p∈(0,1], and suppose

A∣0m⟩=p ∣ψ1⟩+1−p ∣ψ0⟩,A|0^m\rangle=\sqrt p\,|\psi_1\rangle+\sqrt{1-p}\,|\psi_0\rangle,A∣0m⟩=p​∣ψ1​⟩+1−p​∣ψ0​⟩,

where ∣ψ1⟩,∣ψ0⟩|\psi_1\rangle,|\psi_0\rangle∣ψ1​⟩,∣ψ0​⟩ are orthogonal unit vectors (the good and the bad state). Let RGR_GRG​ be a unitary with RG∣ψ1⟩=−∣ψ1⟩R_G|\psi_1\rangle=-|\psi_1\rangleRG​∣ψ1​⟩=−∣ψ1​⟩ and RG∣ψ0⟩=∣ψ0⟩R_G|\psi_0\rangle=|\psi_0\rangleRG​∣ψ0​⟩=∣ψ0​⟩, let R0R_0R0​ fix ∣0m⟩|0^m\rangle∣0m⟩ and negate every other basis state, and let Q=AR0A−1RGQ=AR_0A^{-1}R_GQ=AR0​A−1RG​ be one round (reflect through ∣ψ0⟩|\psi_0\rangle∣ψ0​⟩, then through ∣U⟩=A∣0m⟩|U\rangle=A|0^m\rangle∣U⟩=A∣0m⟩). Put θ=arcsin⁡p\theta=\arcsin\sqrt pθ=arcsinp​.

  1. For every k∈Nk\in\mathbb Nk∈N,
QkA∣0m⟩=sin⁡((2k+1)θ) ∣ψ1⟩+cos⁡((2k+1)θ) ∣ψ0⟩.Q^kA|0^m\rangle=\sin((2k+1)\theta)\,|\psi_1\rangle+\cos((2k+1)\theta)\,|\psi_0\rangle.QkA∣0m⟩=sin((2k+1)θ)∣ψ1​⟩+cos((2k+1)θ)∣ψ0​⟩.
  1. If k∈Nk\in\mathbb Nk∈N is an integer closest to π4θ−12\frac{\pi}{4\theta}-\frac124θπ​−21​, then k≤π4θ≤π4pk\le\frac{\pi}{4\theta}\le\frac{\pi}{4\sqrt p}k≤4θπ​≤4p​π​, and the good state has probability ∣⟨ψ1∣QkA∣0m⟩∣2≥1−p|\langle\psi_1|Q^kA|0^m\rangle|^2\ge 1-p∣⟨ψ1​∣QkA∣0m⟩∣2≥1−p.

So O(1/p)O(1/\sqrt p)O(1/p​) applications of AAA, A−1A^{-1}A−1 and RGR_GRG​ raise the success probability from ppp to nearly 111, a quadratic improvement over the O(1/p)O(1/p)O(1/p) classical repetitions. Grover's algorithm is the special case A=H⊗nA=H^{\otimes n}A=H⊗n, RG=Ox,±R_G=O_{x,\pm}RG​=Ox,±​.

Formalization Note A−1A^{-1}A−1 is the conjugate transpose A∗A^*A∗ (as AAA is unitary). RGR_GRG​ is constrained only on ψ1\psi_1ψ1​ and ψ0\psi_0ψ0​, as in the source. The hypotheses require m≥1m\ge1m≥1, since two orthonormal vectors need dimension at least 2.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • §7.2: Grover's algorithm with known t: P_k = sin²((2k+1)θ), and k ≈ π/(4θ) − 1/2 ≤ (π/4)√(N/t) iterations succeed with probability ≥ 1 − t/N.
  • §7.3: Amplitude amplification: Q^k A|0^m⟩ = sin((2k+1)θ)|ψ1⟩ + cos((2k+1)θ)|ψ0⟩, and O(1/√p) rounds suffice.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Ronald de Wolf, Quantum Computing: Lecture Notes, 27 August 2026. https://homepages.cwi.nl/~rdewolf/qcnotes.pdf.
3 thms2 active usersReviewed
🏆Completed
Quantum Information·Captain: Goku

Quantum Computing: Lecture Notes 2: Bernstein–Vazirani: one phase query recovers the hidden stringTextbook

Motivation

This mission develops Chapter 2 of Quantum Computing: Lecture Notes by Ronald de Wolf. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

This is the correctness of the Bernstein–Vazirani algorithm.

Let n≥0n \ge 0n≥0 and N=2nN = 2^nN=2n, and fix a hidden string a∈{0,1}na \in \{0,1\}^na∈{0,1}n. The input x∈{0,1}Nx \in \{0,1\}^Nx∈{0,1}N is given by xi=(i⋅a) mod 2x_i = (i \cdot a) \bmod 2xi​=(i⋅a)mod2 for every i∈{0,1}ni \in \{0,1\}^ni∈{0,1}n, where i⋅a=∑k=1nikaki \cdot a = \sum_{k=1}^n i_k a_ki⋅a=∑k=1n​ik​ak​. With the phase query Ox,±:∣i⟩↦(−1)xi∣i⟩O_{x,\pm} : |i\rangle \mapsto (-1)^{x_i}|i\rangleOx,±​:∣i⟩↦(−1)xi​∣i⟩ and the nnn-qubit Hadamard transform H⊗nH^{\otimes n}H⊗n, the Deutsch–Jozsa circuit gives

H⊗n Ox,± H⊗n ∣0n⟩=∣a⟩.H^{\otimes n} \, O_{x,\pm} \, H^{\otimes n} \, |0^n\rangle = |a\rangle .H⊗nOx,±​H⊗n∣0n⟩=∣a⟩.

In particular, measuring the final state in the computational basis yields aaa with probability 111.

So one query and 2n2n2n Hadamard gates (the O(n)O(n)O(n) other operations) recover aaa exactly. Only the query depends on the input. Classically, nnn queries are needed.

Formalization Note The input xxx is bvInput a, i.e. i↦i⋅a mod 2i \mapsto i\cdot a \bmod 2i↦i⋅amod2. The circuit is the same fixed definition deutschJozsaState as in the Deutsch–Jozsa statement. The state equality is exact, with no global phase: the source says the result is the classical state ∣a⟩|a\rangle∣a⟩, and that is what the computation gives.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • §2.4.1: Deutsch–Jozsa: one phase query decides constant vs balanced with certainty.
  • §2.4.2: Bernstein–Vazirani: one phase query recovers the hidden string.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Ronald de Wolf, Quantum Computing: Lecture Notes, 27 August 2026. https://homepages.cwi.nl/~rdewolf/qcnotes.pdf.
2 thms2 active usersReviewed
🏆Completed
OptimizationQuantum Information·Captain: Goku

Quantum algorithms for optimizers 2: Simon's algorithm: n+t uniform samples orthogonal to a contain n−1 independent vectors with probability ≥ 1 − 2^{−(t+1)}Textbook

Motivation

This mission develops Chapter 2 of Quantum algorithms for optimizers by Giacomo Nannicini. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

This is the sampling bound behind the classical post-processing of Simon's algorithm.

Let n≥1n \ge 1n≥1 and t≥0t \ge 0t≥0 be integers, and let F2={0,1}\mathbb F_2 = \{0,1\}F2​={0,1} be the field with two elements. Fix a nonzero vector a∈F2na \in \mathbb F_2^na∈F2n​ and let

Va={k∈F2n:k⋅a=∑i=1nkiai≡0(mod2)}V_a = \{k \in \mathbb F_2^n : k \cdot a = \textstyle\sum_{i=1}^n k_i a_i \equiv 0 \pmod 2\}Va​={k∈F2n​:k⋅a=∑i=1n​ki​ai​≡0(mod2)}

be the (n−1)(n-1)(n−1)-dimensional subspace of vectors orthogonal to aaa. Draw k(1),…,k(n+t)k^{(1)}, \dots, k^{(n+t)}k(1),…,k(n+t) independently and uniformly at random from VaV_aVa​. Then

Pr⁡[some n−1 of k(1),…,k(n+t) are linearly independent over F2]≥1−12t+1.\Pr\big[\text{some } n-1 \text{ of } k^{(1)}, \dots, k^{(n+t)} \text{ are linearly independent over } \mathbb F_2\big] \ge 1 - \frac{1}{2^{t+1}}.Pr[some n−1 of k(1),…,k(n+t) are linearly independent over F2​]≥1−2t+11​.

The bound does not depend on nnn, so n+O(1)n + O(1)n+O(1) runs of Simon's circuit suffice to determine the hidden string aaa with high probability.

Formalization Note The probability is the fraction of all ∣Va∣n+t|V_a|^{n+t}∣Va​∣n+t tuples (k(1),…,k(n+t))∈Van+t(k^{(1)},\dots,k^{(n+t)}) \in V_a^{n+t}(k(1),…,k(n+t))∈Van+t​ for which there are n−1n-1n−1 distinct indices whose vectors are linearly independent; vectors of F2n\mathbb F_2^nF2n​ are functions Fin n→Z/2Z\mathrm{Fin}\,n \to \mathbb Z/2\mathbb ZFinn→Z/2Z.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Proposition 2.8: Simon's algorithm: n+t uniform samples orthogonal to a contain n−1 independent vectors with probability ≥ 1 − 2^{−(t+1)}.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Giacomo Nannicini, Quantum algorithms for optimizers, 2025, v5; notes dated 9 July 2025. https://arxiv.org/pdf/2408.07086v5.
1 thm2 active usersReviewed
OptimizationQuantum Information·Captain: Goku

Quantum algorithms for optimizers 8: End-to-end complexity of the quantum MaxCut SDP solver in the QRAM model (corrected statement)Textbook

Motivation

This mission develops Chapter 8 of Quantum algorithms for optimizers by Giacomo Nannicini. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

This is Proposition 8.34 of Nannicini, the end-to-end cost of the quantum mirror-descent solver for the MaxCut SDP relaxation, stated in an explicit hybrid classical–quantum QRAM cost model.

Let n=2qn=2^qn=2q. For a nonzero real symmetric C∈Rn×nC\in\mathbb R^{n\times n}C∈Rn×n put C^=C/∥C∥F\hat C=C/\|C\|_FC^=C/∥C∥F​. Call a density matrix ρ∈Cn×n\rho\in\mathbb C^{n\times n}ρ∈Cn×n an ϵ\epsilonϵ-solution of (MaxCutSDP) if

∑j=1n∣ρjj−1n∣≤ϵandTr⁡(C^ρ) ≥ Tr⁡(C^σ)−ϵ  for every density matrix σ with diag⁡(σ)=1n1.\sum_{j=1}^n\Big|\rho_{jj}-\frac1n\Big|\le\epsilon\qquad\text{and}\qquad \operatorname{Tr}(\hat C\rho)\ \ge\ \operatorname{Tr}(\hat C\sigma)-\epsilon\ \text{ for every density matrix }\sigma\text{ with }\operatorname{diag}(\sigma)=\tfrac1n\mathbb 1.j=1∑n​​ρjj​−n1​​≤ϵandTr(C^ρ) ≥ Tr(C^σ)−ϵ  for every density matrix σ with diag(σ)=n1​1.

A hybrid algorithm consists of (i) a classical preprocessing program, a straight-line program of real arithmetic operations (+,−,×,÷,⋅,arccos⁡,arg⁡+,-,\times,\div,\sqrt\cdot,\arccos,\arg+,−,×,÷,⋅​,arccos,arg, rational constants), which is the only part that reads the entries of CCC and which writes the input half of a QRAM (UQRAM∣j⟩∣y⟩=∣j⟩∣y⊕Mj⟩U_{\mathrm{QRAM}}|j\rangle|y\rangle=|j\rangle|y\oplus M_j\rangleUQRAM​∣j⟩∣y⟩=∣j⟩∣y⊕Mj​⟩, Def. 5.39); (ii) RRR quantum runs, each applying a circuit of two-qubit gates and QRAM calls to ∣0⋯0⟩|0\cdots0\rangle∣0⋯0⟩ and measuring all qubits, where the circuit of each run and the contents of the work half of the QRAM are chosen classically from the outcomes of the earlier runs; (iii) an output, computed from all outcomes, in the form of a list of pairs (y(i),d(i))∈R2×Rn(y^{(i)},d^{(i)})\in\mathbb R^2\times\mathbb R^n(y(i),d(i))∈R2×Rn, which stands for the matrix

ρˉ=1L∑i=1Lexp⁡(y1(i)C^+y2(i)diag⁡(d(i)))Tr⁡exp⁡(y1(i)C^+y2(i)diag⁡(d(i))).\bar\rho=\frac1{L}\sum_{i=1}^{L}\frac{\exp\big(y^{(i)}_1\hat C+y^{(i)}_2\operatorname{diag}(d^{(i)})\big)}{\operatorname{Tr}\exp\big(y^{(i)}_1\hat C+y^{(i)}_2\operatorname{diag}(d^{(i)})\big)}.ρˉ​=L1​i=1∑L​Trexp(y1(i)​C^+y2(i)​diag(d(i)))exp(y1(i)​C^+y2(i)​diag(d(i)))​.

The theorem: there are absolute constants K>0K>0K>0 and ccc such that for all qqq, all ϵ∈(0,1]\epsilon\in(0,1]ϵ∈(0,1] and all δ∈(0,1)\delta\in(0,1)δ∈(0,1), with Λ=log⁡(2+n)+log⁡(2+1/ϵ)+log⁡(2+1/δ)\Lambda=\log(2+n)+\log(2+1/\epsilon)+\log(2+1/\delta)Λ=log(2+n)+log(2+1/ϵ)+log(2+1/δ), there is a hybrid algorithm, fixed before CCC, such that

  1. the QRAM has size at most Kn2ΛcK n^2\Lambda^cKn2Λc, with words of at most KΛcK\Lambda^cKΛc bits;
  2. the preprocessing uses at most Kn2ΛcK n^2\Lambda^cKn2Λc classical operations;
  3. along every measurement record the total number of QRAM accesses and additional gates is at most K n1.5ϵ5ΛcK\,\dfrac{n^{1.5}}{\epsilon^5}\Lambda^cKϵ5n1.5​Λc;
  4. for every nonzero real symmetric CCC, with probability at least 1−δ1-\delta1−δ the output ρˉ\bar\rhoρˉ​ is an ϵ\epsilonϵ-solution of (MaxCutSDP).

The proposition is the payoff of the chapter's MaxCut analysis: the subgradient estimation of Prop. 8.28, the iteration count of Thm. 8.30 and the Hamiltonian structure of Lem. 8.33 combine into a quantum solver whose quantum cost is sublinear in the n2n^2n2 entries of CCC.

Formalization Note The printed proposition has no cost model, no success probability, and no precise meaning for the tolerance over the binary search on γ\gammaγ; these are fixed as above. The classical bookkeeping between quantum runs (tallying samples, forming the subgradients, updating yyy and DDD) is not counted, matching the proof, which takes the classical cost from Prop. 7.29 alone; that bookkeeping never sees CCC. The output is the source's own representation of the iterate (Rem. 8.27, Lem. 8.33): with an arbitrary decoder, the optimum could be read off C^\hat CC^ for free.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Proposition 8.7: Entropic mirror descent iterates are the Gibbs states of the accumulated subgradients.
  • Theorem 8.10: Regret bound of the matrix multiplicative weights update.
  • Lemma 8.12: Emptiness of the PIC polytope certifies primal feasibility after rescaling.
  • Theorem 8.15: Algorithm 7 (MMWU for SDP) returns a primal or a dual certificate.
  • Proposition 8.19: The generalized PIC polytope built from θ-accurate traces is sandwiched between P_0 and P_{4Rrθ}.
  • Proposition 8.21: Computing the dual vector with Õ(√m) calls to a trace-estimate oracle (corrected statement).
  • Proposition 8.28: The estimated MaxCut subgradient is an ϵ/2-subgradient (corrected zero branch).
  • Lemma 8.29: A subgradient of the active piece at a nearby point is an approximate subgradient of the max.
  • Theorem 8.30: Convergence of inexact entropic mirror descent for the MaxCut SDP feasibility problem.
  • Lemma 8.33: The MaxCut mirror-descent Hamiltonians are y₁Ĉ + y₂D with ‖y‖₁ ≤ (4/ϵ) log n.
  • Proposition 8.34: End-to-end complexity of the quantum MaxCut SDP solver in the QRAM model (corrected statement).

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Giacomo Nannicini, Quantum algorithms for optimizers, 2025, v5; notes dated 9 July 2025. https://arxiv.org/pdf/2408.07086v5.
11 thms2 active usersReviewed
🏆Completed
Quantum Information·Captain: Goku

Lecture Notes on Quantum Algorithms 5: Ω(√N) deterministic classical queries for the HSP with N trivially intersecting subgroupsTextbook

Motivation

This mission develops Chapter 5 of Lecture Notes on Quantum Algorithms by Andrew Childs. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

In the hidden subgroup problem (HSP) on a finite group GGG, an algorithm has black-box access to a function f:G→Sf : G \to Sf:G→S, where SSS is a finite set, promised to hide some unknown subgroup H≤GH \le GH≤G:

f(x)=f(y)  ⟺  x−1y∈H(x,y∈G).f(x) = f(y) \iff x^{-1}y \in H \qquad (x, y \in G).f(x)=f(y)⟺x−1y∈H(x,y∈G).

The goal is to determine HHH. A deterministic classical algorithm is a decision tree: it queries group elements g1,g2,…g_1, g_2, \dotsg1​,g2​,… adaptively, each query returning f(gℓ)∈Sf(g_\ell) \in Sf(gℓ​)∈S, and finally outputs a subgroup of GGG. It solves the HSP if, for every subgroup H≤GH \le GH≤G and every fff hiding HHH, its output is HHH. Its query count on input fff is the number of queries it makes on fff.

Theorem. There are an absolute constant c>0c > 0c>0 and a threshold N0N_0N0​ such that the following holds for every N≥N0N \ge N_0N≥N0​. Let GGG be a finite group and SSS a finite set with ∣S∣≥∣G∣|S| \ge |G|∣S∣≥∣G∣, and suppose GGG has a family H\mathcal HH of NNN distinct subgroups any two of which have only the identity in common, i.e. H∩K={1}H \cap K = \{1\}H∩K={1} for all distinct H,K∈HH, K \in \mathcal HH,K∈H. Then every deterministic classical algorithm that solves the HSP on GGG (with values in SSS) makes, on some input fff hiding some subgroup of GGG,

#queries(f)≥cN.\#\text{queries}(f) \ge c\sqrt{N}.#queries(f)≥cN​.

The theorem shows that the HSP is classically hard whenever the group has many trivially intersecting subgroups (for example Simon's problem), in contrast with efficient quantum algorithms for abelian groups.

Formalization Note The algorithm outputs the subgroup itself rather than a generating set, which changes nothing for a query lower bound. The condition ∣S∣≥∣G∣|S| \ge |G|∣S∣≥∣G∣ makes every subgroup of GGG hideable; the proof's adversary labels each new query with a fresh value, and with a very small SSS (say ∣S∣=1|S| = 1∣S∣=1) only H=GH = GH=G can be hidden, so the bound would fail. The constants ccc and N0N_0N0​ are chosen before the group, the set SSS, the family and the algorithm. The threshold N0N_0N0​ is needed because for the trivial group N=1N = 1N=1 and no queries are needed. The phrase "whose only common element is the identity" is read pairwise, as in the section's "trivially intersecting subgroups" and as the proof needs when it counts at most t(t−1)t(t-1)t(t−1) non-identity values gj−1gkg_j^{-1}g_kgj−1​gk​ against NNN subgroups. Read as ⋂H={1}\bigcap \mathcal H = \{1\}⋂H={1}, the theorem is false: in the cyclic group of squarefree order p1⋯pkp_1\cdots p_kp1​⋯pk​, all 2k2^k2k subgroups intersect trivially, yet k+1k+1k+1 queries determine HHH.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Theorem 5.1: Ω(√N) deterministic classical queries for the HSP with N trivially intersecting subgroups.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Andrew Childs, Lecture Notes on Quantum Algorithms, 17 April 2025. https://www.cs.umd.edu/~amchilds/qa/qa.pdf.
1 thm2 active usersReviewed
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Quantum Information·Captain: Goku

Lecture Notes on Quantum Algorithms 21: Symmetrization: the Hamming-weight average of a multilinear polynomial is a polynomial of no larger degreeTextbook

Motivation

This mission develops Chapter 21 of Lecture Notes on Quantum Algorithms by Andrew Childs. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

This is the symmetrization lemma of Minsky and Papert.

Let p∈R[x1,…,xn]p \in \mathbb R[x_1, \dots, x_n]p∈R[x1​,…,xn​] be multilinear, meaning that every variable has degree at most 111 in ppp. For k∈{0,1,…,n}k \in \{0, 1, \dots, n\}k∈{0,1,…,n}, let

P(k):=E∣x∣=k [p(x)]=(nk)−1∑x∈{0,1}n, ∣x∣=kp(x),P(k) := \mathbb E_{|x| = k}\,[p(x)] = \binom{n}{k}^{-1} \sum_{x \in \{0,1\}^n,\ |x| = k} p(x),P(k):=E∣x∣=k​[p(x)]=(kn​)−1x∈{0,1}n, ∣x∣=k∑​p(x),

where ∣x∣|x|∣x∣ is the Hamming weight of xxx (its number of 1s). Then there is a univariate polynomial Q∈R[k]Q \in \mathbb R[k]Q∈R[k] with deg⁡Q≤deg⁡p\deg Q \le \deg pdegQ≤degp (total degree) such that Q(k)=P(k)Q(k) = P(k)Q(k)=P(k) for every k∈{0,1,…,n}k \in \{0, 1, \dots, n\}k∈{0,1,…,n}.

Symmetrization reduces questions about multivariate polynomials that represent symmetric Boolean functions, such as parity or OR, to questions about univariate polynomials. Those questions can then be settled by counting sign changes or by Markov's inequality.

Formalization Note The statement that "PPP is a polynomial" is formalized as agreement with a univariate polynomial on the points {0,…,n}\{0, \dots, n\}{0,…,n}, the only points where PPP is defined. For these kkk the average is taken over a nonempty set.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Lemma 21.1: Polynomial method: the acceptance probability of a t-query algorithm is a polynomial of degree at most 2t.
  • Lemma 21.2: Symmetrization: the Hamming-weight average of a multilinear polynomial is a polynomial of no larger degree.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Andrew Childs, Lecture Notes on Quantum Algorithms, 17 April 2025. https://www.cs.umd.edu/~amchilds/qa/qa.pdf.
2 thms2 active usersReviewed
🏆Completed
Quantum Information·Captain: Goku

Lecture Notes on Quantum Algorithms 27: Local d²-edge-colouring of a bipartite graph of maximum degree dTextbook

Motivation

This mission develops Chapter 27 of Lecture Notes on Quantum Algorithms by Andrew Childs. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

Fix integers N,d≥0N,d\ge 0N,d≥0. There is a single colouring rule ccc, chosen before the graph, that assigns to an ordered pair of vertices α,β∈{1,…,N}\alpha,\beta\in\{1,\dots,N\}α,β∈{1,…,N} a colour c((α,s(α),Lα),(β,s(β),Lβ))∈N×Nc\big((\alpha,s(\alpha),L_\alpha),(\beta,s(\beta),L_\beta)\big)\in\mathbb N\times\mathbb Nc((α,s(α),Lα​),(β,s(β),Lβ​))∈N×N that depends only on the two vertices, their sides s(α),s(β)s(\alpha),s(\beta)s(α),s(β) of the bipartition, and their neighbour lists Lα,LβL_\alpha,L_\betaLα​,Lβ​, with the following property.

Let GGG be an undirected simple graph on the vertex set {1,…,N}\{1,\dots,N\}{1,…,N} with a bipartition s:V→{left,right}s:V\to\{\mathrm{left},\mathrm{right}\}s:V→{left,right} (every edge joins the two sides) and maximum degree at most ddd, and let LvL_vLv​ be any duplicate-free list of the neighbours of each vertex vvv. Then the map {α,β}↦c((α,s(α),Lα),(β,s(β),Lβ))\{\alpha,\beta\}\mapsto c\big((\alpha,s(\alpha),L_\alpha),(\beta,s(\beta),L_\beta)\big){α,β}↦c((α,s(α),Lα​),(β,s(β),Lβ​)) is a proper edge colouring of GGG:

  1. it is symmetric on edges, so each edge receives one colour;
  2. two distinct edges sharing a vertex receive distinct colours;
  3. the number of distinct colours used on the edges of GGG satisfies
#{ c(α,β):αβ∈E(G) }≤d2.\#\{\,c(\alpha,\beta) : \alpha\beta\in E(G)\,\}\le d^2 .#{c(α,β):αβ∈E(G)}≤d2.

In the source the colour of an edge αβ\alpha\betaαβ with α\alphaα on the left is (idx(α,β),idx(β,α))(\mathrm{idx}(\alpha,\beta),\mathrm{idx}(\beta,\alpha))(idx(α,β),idx(β,α)), where idx(α,β)\mathrm{idx}(\alpha,\beta)idx(α,β) is the position of β\betaβ in the neighbour list of α\alphaα. The lemma is the colouring step of the simulation of sparse Hamiltonians: the edges of each colour class form a matching, whose Hamiltonian is simulated separately before the pieces are combined by a product formula.

Formalization Note The source's "efficiently computable" has no machine model, so the running time of the rule is not formalized; what is kept is that one rule serves every graph and reads only the two endpoints' local data (two neighbour-list queries per edge). Colours are pairs of natural numbers rather than elements of [d]×[d][d]\times[d][d]×[d] so that the rule is total at d=0d=0d=0; the bound d2d^2d2 is on the colours actually used on edges.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Lemma 27.1: Local d²-edge-colouring of a bipartite graph of maximum degree d.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Andrew Childs, Lecture Notes on Quantum Algorithms, 17 April 2025. https://www.cs.umd.edu/~amchilds/qa/qa.pdf.
1 thm2 active usersReviewed
🏆Completed
Quantum Information·Captain: Goku

Lecture Notes on Quantum Algorithms 9: Period finding over the reals: an irrational period from two Fourier samplesTextbook

Motivation

This mission develops Chapter 9 of Lecture Notes on Quantum Algorithms by Andrew Childs. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

This is the classical post-processing step of period finding over the reals (Childs, Lemma 9.1).

Write ⌊x⌉\lfloor x \rceil⌊x⌉ for the integer nearest to the real number xxx. Let r>0r > 0r>0 be a real number (the period, possibly irrational), let NNN be a positive integer (the size of the cyclic group ZN\mathbb Z_NZN​ used for Fourier sampling), and let j,j′j, j'j,j′ be relatively prime integers with 1≤j<r1 \le j < r1≤j<r and 1≤j′<r1 \le j' < r1≤j′<r; Fourier sampling returns the integers ⌊jN/r⌉\lfloor jN/r \rceil⌊jN/r⌉ and ⌊j′N/r⌉\lfloor j'N/r \rceil⌊j′N/r⌉. If N≥3r2N \ge 3r^2N≥3r2, then:

  1. the fraction j/j′j/j'j/j′ is one of the convergents of the continued fraction expansion of the rational number
⌊jN/r⌉⌊j′N/r⌉;\frac{\lfloor jN/r \rceil}{\lfloor j'N/r \rceil};⌊j′N/r⌉⌊jN/r⌉​;
  1. the period is recovered to within one unit:
∣r−⌊jN⌊jN/r⌉⌉∣≤1.\left| r - \left\lfloor \frac{jN}{\lfloor jN/r \rceil} \right\rceil \right| \le 1.​r−⌊⌊jN/r⌉jN​⌉​≤1.

Thus, from two samples with coprime multipliers, one learns jjj from the continued fraction expansion and then an approximation of rrr to within 111.

Formalization Note The nearest-integer function is Mathlib's round (ties rounded up; the source leaves ties unspecified and its proof uses only that the rounding error is at most 1/21/21/2). Convergents are Mathlib's Real.convergent, which coincide with the convergents of the regular continued fraction. The ranges 1≤j,j′<r1 \le j, j' < r1≤j,j′<r are those the source's proof uses (they come from ⌊jN/r⌉∈ZN\lfloor jN/r \rceil \in \mathbb Z_N⌊jN/r⌉∈ZN​ and the proof's appeals to j≥1j \ge 1j≥1 and j′<rj' < rj′<r); the proof's "j<j′j < j'j<j′ without loss of generality" is not imposed. Under these hypotheses the denominator ⌊j′N/r⌉\lfloor j'N/r \rceil⌊j′N/r⌉ is at least 333, so no division by zero occurs.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Lemma 9.1: Period finding over the reals: an irrational period from two Fourier samples.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Andrew Childs, Lecture Notes on Quantum Algorithms, 17 April 2025. https://www.cs.umd.edu/~amchilds/qa/qa.pdf.
1 thm2 active usersReviewed
🏆Completed
Quantum Information·Captain: Goku

Lecture Notes on Quantum Algorithms 33: Ω(1/k²) spectral gap of the adiabatic clock Hamiltonian on the computational subspaceTextbook

Motivation

This mission develops Chapter 33 of Lecture Notes on Quantum Algorithms by Andrew Childs. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

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.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Lemma 33.1: Ω(1/k²) spectral gap of the adiabatic clock Hamiltonian on the computational subspace.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Andrew Childs, Lecture Notes on Quantum Algorithms, 17 April 2025. https://www.cs.umd.edu/~amchilds/qa/qa.pdf.
4 thms2 active usersReviewed
🏆Completed
Quantum Information·Captain: Goku

Quantum Computing: Lecture Notes 6: Abelian HSP: the standard algorithm samples uniformly from H^⊥Textbook

Motivation

This mission develops Chapter 6 of Quantum Computing: Lecture Notes by Ronald de Wolf. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

This is the correctness statement of the standard quantum algorithm for the Abelian hidden subgroup problem.

Let G=ZN1×⋯×ZNℓG = \mathbb Z_{N_1}\times\cdots\times\mathbb Z_{N_\ell}G=ZN1​​×⋯×ZNℓ​​ be a finite Abelian group written additively (Ni≥1N_i \ge 1Ni​≥1), with characters χg(h)=∏i=1ℓωNigihi\chi_g(h) = \prod_{i=1}^{\ell} \omega_{N_i}^{g_i h_i}χg​(h)=∏i=1ℓ​ωNi​gi​hi​​, ωN=e2πi/N\omega_N = e^{2\pi i/N}ωN​=e2πi/N, and quantum Fourier transform FG=FN1⊗⋯⊗FNℓF_G = F_{N_1}\otimes\cdots\otimes F_{N_\ell}FG​=FN1​​⊗⋯⊗FNℓ​​, ∣k⟩↦∣χk⟩=∣G∣−1/2∑g∈Gχk(g)∣g⟩|k\rangle \mapsto |\chi_k\rangle = |G|^{-1/2}\sum_{g\in G}\chi_k(g)|g\rangle∣k⟩↦∣χk​⟩=∣G∣−1/2∑g∈G​χk​(g)∣g⟩. Let SSS be a finite set, H≤GH \le GH≤G a subgroup, and f:G→Sf : G \to Sf:G→S a function hiding HHH:

f(g)=f(g′)  ⟺  g+H=g′+H.f(g) = f(g') \iff g + H = g' + H.f(g)=f(g′)⟺g+H=g′+H.

The standard algorithm starts in ∣0⟩∣0⟩|0\rangle|0\rangle∣0⟩∣0⟩ (registers of dimensions ∣G∣|G|∣G∣ and ∣S∣|S|∣S∣), prepares ∣G∣−1/2∑g∣g⟩∣0⟩|G|^{-1/2}\sum_{g}|g\rangle|0\rangle∣G∣−1/2∑g​∣g⟩∣0⟩, computes fff in superposition with one query, ∣g⟩∣0⟩↦∣g⟩∣f(g)⟩|g\rangle|0\rangle\mapsto|g\rangle|f(g)\rangle∣g⟩∣0⟩↦∣g⟩∣f(g)⟩, (measures the second register,) applies FGF_GFG​ to the first register and measures it. For every g∈Gg \in Gg∈G the outcome ggg occurs with probability

Pr⁡[output g]={∣H∣/∣G∣if χg(h)=1 for all h∈H (i.e. χg∈H⊥),0otherwise.\Pr[\text{output } g] = \begin{cases} |H|/|G| & \text{if } \chi_g(h) = 1 \text{ for all } h\in H \ (\text{i.e. } \chi_g \in H^\perp),\\ 0 & \text{otherwise.}\end{cases}Pr[output g]={∣H∣/∣G∣0​if χg​(h)=1 for all h∈H (i.e. χg​∈H⊥),otherwise.​

Since ∣H⊥∣=∣G∣/∣H∣|H^\perp| = |G|/|H|∣H⊥∣=∣G∣/∣H∣, the algorithm samples uniformly from the labels of the elements of H⊥H^\perpH⊥; each sample gives a linear constraint on HHH, which is how the algorithm generalizes Simon's algorithm, period finding and discrete logarithms.

Formalization Note The finite set SSS is given an arbitrary additive group structure so that computing fff is the unitary ∣g,b⟩↦∣g,b+f(g)⟩|g,b\rangle\mapsto|g,b+f(g)\rangle∣g,b⟩↦∣g,b+f(g)⟩, which maps ∣g,0⟩|g,0\rangle∣g,0⟩ to ∣g,f(g)⟩|g,f(g)\rangle∣g,f(g)⟩ as in the source. The intermediate measurement of the second register (step 4) is omitted: it does not change the distribution of the first register, so the output law is the first-register marginal of the state before the final measurement. The source's claim that HHH can then be found efficiently from few samples is asserted without proof and is not part of this statement.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • §6.2.2: Abelian HSP: the standard algorithm samples uniformly from H^⊥.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Ronald de Wolf, Quantum Computing: Lecture Notes, 27 August 2026. https://homepages.cwi.nl/~rdewolf/qcnotes.pdf.
1 thm2 active usersReviewed
Quantum Error CorrectionQuantum Information·Captain: Goku

An Introduction to Quantum Error Correction and Fault-Tolerant Quantum Computation 2: Quantum Gilbert–Varshamov, quantum Hamming, and asymptotic rate boundsTextbook

Motivation

This mission develops Chapter 2 of An Introduction to Quantum Error Correction and Fault-Tolerant Quantum Computation by Daniel Gottesman. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

An [[n,k,d]][[n,k,d]][[n,k,d]] code is a subspace CCC of (C2)⊗n(\mathbb C^2)^{\otimes n}(C2)⊗n of dimension 2k2^k2k such that every operator EEE acting on at most d−1d-1d−1 qubits satisfies ⟨ψ∣E∣ψ⟩=c′(E)\langle\psi|E|\psi\rangle=c'(E)⟨ψ∣E∣ψ⟩=c′(E) for all unit vectors ∣ψ⟩∈C|\psi\rangle\in C∣ψ⟩∈C, with c′(E)c'(E)c′(E) independent of ∣ψ⟩|\psi\rangle∣ψ⟩ (eq. (34)); that is, CCC has distance at least ddd. Put t=⌊(d−1)/2⌋t=\lfloor (d-1)/2\rfloort=⌊(d−1)/2⌋. The code is nondegenerate if, for every unit vector ∣ψ⟩∈C|\psi\rangle\in C∣ψ⟩∈C, the Gram matrix (⟨ψ∣Pa†Pb∣ψ⟩)a,b\big(\langle\psi|P_a^\dagger P_b|\psi\rangle\big)_{a,b}(⟨ψ∣Pa†​Pb​∣ψ⟩)a,b​ over the phase-free Pauli operators PaP_aPa​ of weight at most ttt is nonsingular. Let H(x)=−xlog⁡2x−(1−x)log⁡2(1−x)H(x)=-x\log_2x-(1-x)\log_2(1-x)H(x)=−xlog2​x−(1−x)log2​(1−x).

  1. (Quantum Gilbert–Varshamov bound.) If d≥1d\ge1d≥1 and
(∑j=0d−13j(nj))2k≤2n,\Big(\sum_{j=0}^{d-1}3^j\binom nj\Big)2^k\le 2^n,(j=0∑d−1​3j(jn​))2k≤2n,

then an [[n,k,d]][[n,k,d]][[n,k,d]] code exists. 2. (Quantum Hamming bound.) Every nondegenerate [[n,k,d]][[n,k,d]][[n,k,d]] code satisfies

(∑j=0t3j(nj))2k≤2n.\Big(\sum_{j=0}^{t}3^j\binom nj\Big)2^k\le 2^n.(j=0∑t​3j(jn​))2k≤2n.
  1. (Asymptotic rates.) Let 0<p<1/20<p<1/20<p<1/2 and ε>0\varepsilon>0ε>0. There is NNN such that for every n≥Nn\ge Nn≥N:
    • every nondegenerate [[n,k,d]][[n,k,d]][[n,k,d]] code with d≥2pnd\ge 2pnd≥2pn has k/n≤1−plog⁡23−H(p)+εk/n\le 1-p\log_2 3-H(p)+\varepsilonk/n≤1−plog2​3−H(p)+ε;
    • if 1−2plog⁡23−H(2p)>01-2p\log_2 3-H(2p)>01−2plog2​3−H(2p)>0, there is a nondegenerate [[n,k,d]][[n,k,d]][[n,k,d]] code with d≥2pnd\ge 2pnd≥2pn and k/n≥1−2plog⁡23−H(2p)−εk/n\ge 1-2p\log_2 3-H(2p)-\varepsilonk/n≥1−2plog2​3−H(2p)−ε.

The first two bounds are counting arguments. The third gives the rate window, eq. (37), between which the best nondegenerate codes lie.

Formalization Note The source's 'distance ddd' is read as distance at least ddd, so existence is meaningful also for k=0k=0k=0. The hypothesis d≥1d\ge1d≥1 excludes d=0d=0d=0, where (36) is an empty sum and the claim would demand a 2k2^k2k-dimensional code for every kkk. The asymptotic clause is read as an ε\varepsilonε–NNN statement. The lower rate bound is asserted only when it is positive.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Theorem 1: No-Cloning: no quantum operation copies every state.
  • Theorem 2: Correctable errors are closed under linear combinations; weight-t Pauli errors give all t-qubit errors.
  • Theorem 3: Knill–Laflamme condition for quantum error correction.
  • Theorem 4: Quantum Gilbert–Varshamov, quantum Hamming, and asymptotic rate bounds.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Daniel Gottesman, An Introduction to Quantum Error Correction and Fault-Tolerant Quantum Computation, 2009, v1. https://arxiv.org/pdf/0904.2557v1.
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OptimizationQuantum Information·Captain: Goku

Quantum algorithms for optimizers 7: A (‖A‖_F, Õ(q), ξ)-block-encoding of a classical matrix from QRAM, with an explicit cost modelTextbook

Motivation

This mission develops Chapter 7 of Quantum algorithms for optimizers by Giacomo Nannicini. The chapter's selected results describe the mathematical guarantees below.

Setting and conventions

The linked theorem statements and shared definitions specify the register types, oracle access, normalization, and resource conventions. Their source locators and independent readbacks accompany each target.

Chapter goal

Fix constants C0∈RC_0 \in \mathbb{R}C0​∈R and c0∈Nc_0 \in \mathbb{N}c0​∈N (those of the assumption p=O~(1)p = \widetilde{O}(1)p=O(1)). There are constants C>0C > 0C>0 and c∈Nc \in \mathbb{N}c∈N such that the following holds. Let q,p∈Nq, p \in \mathbb{N}q,p∈N, d=2qd = 2^qd=2q, ξ>0\xi > 0ξ>0, write L=log⁡(2+d)+log⁡(2+1/ξ)L = \log(2+d) + \log(2+1/\xi)L=log(2+d)+log(2+1/ξ), and assume p≤C0Lc0p \le C_0 L^{c_0}p≤C0​Lc0​. Then there exist

  1. a QRAM (Def. 5.39) with 2b2^b2b addresses and words of rrr bits, of size 2br≤Cd2(p+1)Lc2^b r \le C d^2 (p+1) L^c2br≤Cd2(p+1)Lc;
  2. a straight-line real-arithmetic program of at most Cd2LcC d^2 L^cCd2Lc operations (+,−,×,÷,⋅,arccos⁡+, -, \times, \div, \sqrt{\cdot}, \arccos+,−,×,÷,⋅​,arccos, complex argument, rational constants) and an addressing map, which compute the QRAM contents from the entries of the matrix;
  3. a quantum circuit V\mathcal{V}V on w+qw + qw+q qubits with w≤C(q+1)Lcw \le C (q+1) L^cw≤C(q+1)Lc, making at most CLcC L^cCLc uncontrolled calls to the QRAM (or its inverse) and using at most CLcC L^cCLc two-qubit gates,

all independent of the matrix, such that for every A∈Cd×dA \in \mathbb{C}^{d\times d}A∈Cd×d whose entries satisfy ∣Re⁡aij∣,∣Im⁡aij∣≤2p|\operatorname{Re} a_{ij}|, |\operatorname{Im} a_{ij}| \le 2^p∣Reaij​∣,∣Imaij​∣≤2p, the unitary V(UQRAM(A))\mathcal{V}(U_{\mathrm{QRAM}}(A))V(UQRAM​(A)) obtained with the QRAM loaded by the program is an (∥A∥F,w,ξ)(\|A\|_F, w, \xi)(∥A∥F​,w,ξ)-block-encoding of AAA:

∥∥A∥F (⟨0∣w⊗I) V (∣0⟩w⊗I)−A∥≤ξ.\bigl\| \|A\|_F\,(\langle 0|_w \otimes I)\,\mathcal{V}\,(|0\rangle_w \otimes I) - A \bigr\| \le \xi .​∥A∥F​(⟨0∣w​⊗I)V(∣0⟩w​⊗I)−A​≤ξ.

This is the data-structure route to block-encodings of classically stored dense matrices, with subnormalization the Frobenius norm and only polylogarithmic quantum cost.

Formalization Note Corrected statement. The source gives no cost model for classical arithmetic, does not say in which parameters ppp is polylogarithmic, and does not say how the costs depend on ξ\xiξ. Here classical cost is the length of a straight-line real-arithmetic program (the model of the Cor. 5.45 chunk), p=O~(1)p = \widetilde{O}(1)p=O(1) means p≤C0Lc0p \le C_0 L^{c_0}p≤C0​Lc0​ for arbitrary C0,c0C_0, c_0C0​,c0​, all O~\widetilde{O}O bounds are polylogarithmic in ddd and 1/ξ1/\xi1/ξ, and the QRAM size is O~(d2p)\widetilde{O}(d^2 p)O(d2p) rather than O(d2p)O(d^2 p)O(d2p) because the word size must grow with log⁡(1/ξ)\log(1/\xi)log(1/ξ). A ppp-bit entry is modelled by the magnitude bound 2p2^p2p on its real and imaginary parts.

Significance

These are known mathematical results. Their Lean statements have been checked and reviewed against the cited source; formal proofs remain open for contributors.

Supporting targets

  • Proposition 7.9: Iterative refinement reaches residual ϵ in O(log 1/ϵ) iterations.
  • Proposition 7.14: Product of block-encodings (error term corrected).
  • Proposition 7.18: Linear combination of block-encodings (error term corrected for α < 1).
  • Lemma 7.20: Block-encoding of the diagonal matrix of inner products ⟨ϕ_j|ψ_j⟩.
  • Proposition 7.21: Block-encoding from sparse-access oracles (rotation cost and entry encoding made explicit).
  • Lemma 7.37: A bounded polynomial of degree Õ(β) approximating exp(2βx)/4 on [−1, 0].
  • Lemma 7.39: Block-encoding a density matrix from a unitary preparing its purification.
  • Proposition 7.41: One-copy trace estimator: a random variable with bias ≤ θ/4 for Tr(Aρ) and constant variance.
  • Proposition 7.38: Gibbs-state preparation from a block-encoding of H, for the polynomial of Lemma 7.37 made explicit.
  • Proposition 7.29: A (‖A‖_F, Õ(q), ξ)-block-encoding of a classical matrix from QRAM, with an explicit cost model.

Formalization scope

Prove the existing statements under their stated hypotheses and definitions. Any correction to a printed source claim remains explicit in its target description. All listed target proofs are currently sorry; no proof is claimed. The mission goal is the designated chapter capstone; the remaining targets are separate milestones. Parts a, b, c and d are merged into their original chapter.

Selected references

  • Giacomo Nannicini, Quantum algorithms for optimizers, 2025, v5; notes dated 9 July 2025. https://arxiv.org/pdf/2408.07086v5.
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