Alphabeta Math
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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.

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✓ 1 result · all verified · 1 also independently AI-judged
Every result on this page is machine-checked by a proof checker and read in full and owner-audited; the judge is an additional, independent cross-model AI review of the proofs; all 1 also cleared it.

Bell States, Teleportation, and Dense Coding — Examples

1 · Prerequisites

2 · Summary

Objective

This companion expands the teleportation circuit for a general normalized qubit, lists each measured branch, and checks the Pauli correction in the declared phase-bit/flip-bit order, including the two-bit case where operator order matters.

3 · Logical flowchart

4 · Definitions, theorems and proofs

None yet.

5 · Examples, counterexamples and false statements

ExampleConstruction: Literature-sourcedVerification: AI-generatedprecheck passjudge pass (gpt-6-luna)Open item page →

Teleportation branch and Pauli correction

Example

Let ∣ψ⟩=α∣0⟩+β∣1⟩ with ∣α∣2+∣β∣2=1. On input ∣ψ⟩A and shared resource ∣Φ+⟩BC, compute the four post-gate measurement branches and verify the correction on wire C for each label (a,b).

Facts & Assumptions

Given: The normalized input, the ordered wires A,B,C, and the teleportation gates, measurement, and correction.

[A1]

α,β∈C and ∣α∣2+∣β∣2=1.

[F1]

Teleportation Bell-basis expansion gives the post-gate expansion 12∑a,b∣ab⟩⊗XbZa∣ψ⟩.

[F2]

Teleportation outcomes are equiprobable proves that each outcome label has probability 1/4.

[F3]

The Pauli matrices gives X∣0⟩=∣1⟩, X∣1⟩=∣0⟩, Z∣0⟩=∣0⟩, and Z∣1⟩=−∣1⟩.

Verification

1.1givenA1F1algebra

Expanding the input with the Bell resource and applying CNOT A→B gives 2−1/2(α∣000⟩+α∣011⟩+β∣110⟩+β∣101⟩). Applying HA and grouping by AB yields 12(∣00⟩(α∣0⟩+β∣1⟩)+∣01⟩(α∣1⟩+β∣0⟩)+∣10⟩(α∣0⟩−β∣1⟩)+∣11⟩(α∣1⟩−β∣0⟩)), which is [F1]'s expansion.

2.1step 1.1A1F2F3algebra

For each label, the receiver vector is respectively ψ, Xψ, Zψ, and XZψ by [F3]. Each has the same norm as ψ, since X swaps its two coordinates and Z changes only the sign of the second. Thus each projected branch has squared norm 14∥ψ∥2=1/4, agreeing with the probability in [F2].

2.2step 1.1F3algebra

For label 00, the correction is I and leaves α∣0⟩+β∣1⟩ unchanged. For 01, it is X, and X(α∣1⟩+β∣0⟩)=α∣0⟩+β∣1⟩. For 10, it is Z, and Z(α∣0⟩−β∣1⟩)=α∣0⟩+β∣1⟩.

3.1step 2.2F3algebra∎

For label 11, the branch is α∣1⟩−β∣0⟩=XZ∣ψ⟩ and the correction is ZX. Hence ZX(XZ∣ψ⟩)=Z(XX)Z∣ψ⟩=Z2∣ψ⟩=∣ψ⟩ using [F3]; this fixed order has no residual phase. Together the four calculations return the input on every branch.

Sources