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Metadata
slug: mayer-2021-zero-fidelity-tightness
bibkey: mayer2021zerofidelity
doi: 10.48550/arXiv.2109.09629
url: https://arxiv.org/abs/2109.09629v1
triage: theorem
motivation_gids:
  - D5/S3/Quantum/QuantumChannels/MayerZeroFidelityTightness.result

Tightness of the 0-fidelity lower bound and the worst-case processes

Problem

K. Mayer, A short note on the 0-fidelity, arXiv:2109.09629v1, proves for every -qubit process that , where is the process fidelity and the 0-fidelity on tensor products of single-qubit SIC-POVM states, and writes:

This leads us to conjecture that the lower bound in Th.~1 is tight for all .

A description of the worst-case process is an open problem.

The verbatim statements are in the literature note. Issue #14119 reads the two statements for every , every choice of single-qubit SIC-POVMs and every finite Kraus family: the lower bound holds with equality exactly when every Kraus operator lies in the span of the identity and the single-qubit Pauli operators, and every value of is attained with equality.

Motivation

The 0-fidelity is estimated from product states only. If the lower bound is tight for every , the worst-case process fidelity does not approach the 0-fidelity as grows, so an estimate of certifies only ; describing the worst cases identifies which errors the product-state estimate cannot see.

Gap

Issue #14119 records the literature check before any Lean: one arXiv version; arXiv full-text, web and Zenodo searches and the citing work arXiv:2312.08590 contain no proof of tightness and no description of the worst-case processes; the repository had no 0-fidelity result. not-found-in-searched-scope.

Route

Each qubit SIC is a 2-design: . Expanding a Kraus operator in Pauli strings (with non-identity factors) gives and , where and, by trace preservation, . Hence , with equality iff for every . Depolarizing noise on one qubit, , has and .

Falsifier

The statement concerns the 0-fidelity of the source (product single-qubit SIC states, uniform weights) and finite Kraus families on qubits; other input ensembles or weightings are outside the claim.

Evidence

The canonical source is D5/S3/Quantum/QuantumChannels/MayerZeroFidelityTightness.lean, with public IsQubitSIC, productState, zeroFidelity, processFidelity, HasWeightOneSupport, claim and result : claim. It contains the single-qubit SIC frame identity sic_frame (the 2-design property of SIC-POVMs, entered as a literature prerequisite; see the note). It reuses the frozen Pauli, pauliMatrix, tensorOp, wordOp and the tensor product law tensor_mul of D5/S3/Quantum/Information/StabilizerPairLocalUnitaryInequivalence, the frozen maximally entangled carrier maxEntangledVector, maxEntangled and its trace identity max_entangled_trace of D5/S3/QuantumBounds/PeritoTsirelson, the frozen two-qubit swap swapMatrix of D5/S3/Resource/CompositeConeProperness with its trace identity hswap_trace, Mathlib’s hammingDist for the Pauli weight, the frozen Kraus carrier MatrixMap.of_kraus and the rank-one transport hsandwich of D5/S3/Quantum/Measurement/ExactConditionalPreparationCost, and the Pauli-word expansion word_expansion, the unit wordUnit and the identities tensor_one, word_one, tensor_trace, pauli_trace_pair, pauli_hermitian and word_hermitian of D5/S3/Quantum/Measurement/StabilizerPovmMaximalEntanglementRefutation. Each of these was a private declaration or a local step at its origin and is made public there, with its statement and proof unchanged. The axiom closure of result is exactly propext, Classical.choice and Quot.sound; there is no sorry, native_decide, or new axiom. The module statement is sha256:207677a8f33b9dd5698be1a72aaddf2cf8220c1ef9d80607297f8da5d317cfda, the result statement sha256:a5920d009739edf5671ef0802d3d3bc20d9adaeeed545c59b97a1c554535c065 and the claim statement sha256:0c567f7c43c7080bc672bd69401520dbe949740e5b88791c3428680b44d326cf. The Freeze event is sha256:e354c9094fed1af2bbf82833bc9c8804febc056779ed106613cb31df97dac7ac.

Triage

Tier 1 conjecture and open problem of a 2021 note, preregistered in issue #14119 before any Lean. theorem; resolution proved.

declarationproof_shapeescape_witnessadmission_basis
resultcontentchannel_bound (the Pauli-weight form of and its equality case) and tight_channelopen-problem-resolution

The other theorems of the module lie on the proof path of result (CLAUDE.md §3.2 「有消费的辅助声明」); each has free arguments. Utility is none. There is no digestion atom.

What the settlement shows

Proved by result: for every , every choice of single-qubit SIC-POVMs and every finite Kraus family on qubits, , with equality if and only if every Kraus operator has zero coefficient on every Pauli string with at least two non-identity factors; and every is the 0-fidelity of a process with .

Established inside the proof, for general data. For every Kraus family, and with the Pauli-twirl weights , which are nonnegative and, for a trace-preserving family, sum to one.

Argued, not formalized.

  • Mechanism. Moving Pauli-twirl weight from the identity to a Pauli string of weight lowers by and by ; the decrease of is smallest, , for . So for a given the process fidelity is lowest exactly when all error weight sits on strings acting on one qubit; errors of higher weight are more visible to the product-state average. Below the affine bound is negative and is not the minimum (next item).
  • The low-fidelity range. Since and , every process has ; for the minimum of is , attained by Pauli channels supported on non-identity strings. So the tight lower boundary is on .
  • Upper bound. The paper’s upper bound and its SDP improvement are not addressed here.

Open. A closed form of the best-case process fidelity for given (the paper’s SDP upper bound) is not settled here.

Effect on the paper. The §III conjecture holds for every , and the §IV open problem has an answer on : the worst-case processes, that is, the equality cases of the bound , are exactly those whose Kraus operators lie in the span of the identity and the single-qubit Pauli operators. For the minimum of is (item above).

ASSUMED-UNVERIFIED

The bounded literature check does not establish exhaustive worldwide novelty, priority, or the absence of an independent proof.