Alphabeta Math
AlgorithmAlgorithm: AI-adaptedProof: Not applicablePipeline-generated
How statement and proof provenance work

The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

Sparse-oracle Gibbs-state purification

Definition

Input a finite Hermitian matrix H, a nonnegative coefficient η, a rational certified bound K≥∥ηH∥, dimension d≥1, costed reference preparation Φd, controlled sparse evolution circuits and their inverses, an output accuracy, and shift-confidence and implementation budgets. For the optional normalized-output branch, supply εout>0 and a rational amplification failure target 0<ρ<1. All access, coefficient generation, rotations, arithmetic, precision synthesis, reference preparation and memory operations have declared costs. The supplied finite decoded matrix may approximate the target matrix only with a stated operator-norm error budget included below.

  1. Freeze the energy shift. Choose 0<e≤1/2 and an exact finite decoded Hermitian L^ with ∥L^−ηH∥≤δ≤min⁡(1/8,e/100) and certified norm bound K+δ. Run the explicit finite coherent spectral sampler and capped generalized minimum procedure in Coherent spectral minimum and a frozen Gibbs energy shift on L^. Measure its rational output once, set λ~=s−1/8, and freeze the decoded G^=L^−(λ~−3/2)I and target G=ηH−(λ~−3/2)I, their norm certificates and all ensuing circuit parameters. On the shift good event the decoded minimum is in [3/2,7/4]; the variational bound ∣λmin(L^)−λmin(ηH)∣≤δ puts the target minimum in [1,2]. For η=0 the normalized output is the supplied Φd directly. A shift failure belongs to the declared confidence budget.
  2. Generate the finite block. Choose 0<e≤1/2 and a rational KG≥max⁡(∥G∥,∥G^∥)/2. Construct the block for G^ and include its target perturbation ∥e−G^/2−e−G/2∥≤δ/2 in the allocated error. For f(x)=e−x/2 use x0=KG+1/2, r=KG, Δ=1/2, B=1. Its Taylor coefficients are ak=e−x0/2(−1/2)k/k!. Execute the finite arcsine convolution, truncation, signed-binomial coefficient construction, coefficient rounding and normalization in Certified finite smooth Fourier approximation and LCU normalization. Use its explicit finite K,L,M cutoffs, enlarged by certified upper enclosures when necessary. Prepare the finite coefficient vector, apply the signed-frequency controlled evolutions, unprepare it and dilute the clean flag to common normalization BG+=1+e/8. Allocate coefficient, rotation, evolution and decoded-matrix errors so the final successful compression differs from e−G/2/BG+ by at most e. Their sum is an input certificate, and every circuit is retained with its actual adjoint and controlled implementation.
  3. Unmeasured flag interface. Prepare Φd and apply the block on its first factor. The ideal zero-work vector is ((e−G/2/BG+)⊗I)Φd, with probability tr⁡(e−G)/[d(BG+)2]. Return this entire unmeasured circuit and its actual inverse when a coherent flagged sampler is requested. A caller constructing indexed trace samplers reuses these frozen parameters; it does not rerun ShiftMin within that sampler.
  4. Optional normalized output. To output a normalized purification, use step 2 with accuracy 0<e≤min⁡(1,εout)/(10000d), invoke the finite direct-sample/random-iteration capped amplification construction of Capped randomized amplitude amplification preserves a flagged output with lower floor 1/(64d) and failure target ρ, and measure only its supplied good/bad flag. On a good outcome return the normalized flag branch; on cap failure return explicit FAIL. Do not measure score, label, or work registers in this branch. The amplification lemma supplies the finite success and branch-state contract; no exact Grover peak or unbounded rejection loop is used. A caller needing an inverse uses the unmeasured circuit from step 3, rather than an inverse of this measured conditional output.

The identity energy shift changes no normalized Gibbs state. Non-power-of-two dimensions use the declared CΦ input. The algorithm supplies no uncharged matrix exponential, spectral projector, coefficient oracle or sparse-sum oracle. Its successful-vector and normalized-state bounds are proved separately in Gibbs purification error and resource bound ↗.

Depends on

Used by

Dependency tree · two levels

51 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.

Sources