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.
Finite quantum promise-computation model
Definition
Let be a promise problem: are disjoint, and no answer is required outside (Promise problem). For every input length , let be the number of auxiliary qubits. The input wires are ordered with the first wire most significant: for , is the computational-basis vector indexed by (Finite registers and their ordered computational bases, Big-endian encoding of ordered bit strings). The auxiliary register has wires and is initialized to . When or , the corresponding zero-qubit register is the one-dimensional space , not the zero vector space.
For each , a finite circuit acts on the ordered register of wires and has the unitary denotation specified by Finite circuit syntax and ordered wire labels and Denotational semantics of a finite layered circuit. The circuit syntax designates an ordered tuple of distinct output-wire indices; an acceptance specification uses that same tuple , whose indices lie in . It consists of this tuple and a total predicate for and . The tuple may be empty; then its measured output set contains only the empty word. Auxiliary wires are initialized to zero, but this definition does not require them to return to zero after the computation; that stronger clean-ancilla condition is defined in Clean and dirty ancillas.
A finite quantum promise computation is the data with these registers and predicates. Its output is classical: measure only the named output wires in the computational basis and accept exactly when . No intermediate measurement is part of this base model. Unless a full-list uniformity condition is imposed separately, the family need not be generated uniformly. When uniformity or cost is claimed, is supplied by one fixed deterministic Turing machine with an explicit polynomial worst-case time bound in the encoded pair (Deterministic one-tape Turing machines with designated accept and reject states, Partial functions computed by a machine under fixed encodings, Worst-case time and space complexity of a machine). This is a mathematical finite-circuit model and makes no assertion about physical realization.
Depends on
- Promise problem
- Finite registers and their ordered computational bases
- Big-endian encoding of ordered bit strings
- Ordered tensor registers, their inner product, and wire permutations
- Finite circuit syntax and ordered wire labels
- Denotational semantics of a finite layered circuit
- Finite circuit resource accounting
- Clean and dirty ancillas
- Deterministic one-tape Turing machines with designated accept and reject states
- Partial functions computed by a machine under fixed encodings
- Worst-case time and space complexity of a machine
Used by
- Bounded-error repetition amplification Algorithm
- EQP on promise problems in the QC14 model Definition
- Normalized output law for finite quantum query branches Definition
- Oracle-aware full-list quantum circuit family Definition
- Quantum acceptance probability for a finite promise computation Definition
- Quantum query algorithm Definition
- Uniform verifier interface with a quantum witness Definition
- ZQP on promise problems with bounded failure Definition
- Bounded-error repetition amplification is correct and uniform Theorem
- The partial-output acceptance law is a finite probability law Theorem
Dependency tree · two levels
35 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
- John Watrous, Quantum Computational Complexity, Sections IV.1–IV.2 (standard reference, not scraped)
- Ronald de Wolf, Quantum Computing: Lecture Notes, Chapter 13, Section 13.2 (standard reference, not scraped)