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Paper Citation Record · LEDGER

Provably Efficient Self-Calibrating Quantum Fault Tolerance

As of 13 August 2026, this Paper Citation Record lists 20 of 20 outbound references and 0 inbound Pith citation observations for arXiv:2608.05686.

A citation records a reference. It does not transfer a finding from one paper to another.

pith.paper-citation-record.v1
2608.05686 v1

Coverage vector

measured 20 of 20 reference resolution

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Source: paper_references, paper_reference_links, observed 2026-08-08T01:06:15.179769Z

measured 20 of 20 standing notices

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Source: scholarly_work_events, retraction_status_cache, observed 2026-08-12T06:34:41.77262+00:00

measured 0 of 0 inbound itemization

Pith citing papers itemized under the disclosed page cap.

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measured 0 of 1 external citation measurements

A source-named dated measurement, never combined with another source.

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Reference resolution

20 of 20 outbound references displayed

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External citation measurements

No source-named external measurement is stored.

Outbound references

Observation 327297be-da07-456a-af2e-1d313b00514c · outbound

This paper cites Recall from Eq.

Provably Efficient Self-Calibrating Quantum Fault Tolerance Recall from Eq

Reference 1

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Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-08T01:06:15.099676Z digest=sha256:1dd7c58b2c2c5897e32417ae1d37d973cc804b1bca7cc3425d7c1d421a37954b

Observation 8a71d8bc-52f6-45f7-85ce-4b3f32214139 · outbound

This paper cites Again, we need to choose a perturbation radiusλ >0and define the shrunk feasible set Qλ :={ ⃗θ∈Q: ⃗θ+λu∈Qand ⃗θ−λu∈Qfor allu∈ {±1} d}.

Provably Efficient Self-Calibrating Quantum Fault Tolerance Again, we need to choose a perturbation radiusλ >0and define the shrunk feasible set Qλ :={ ⃗θ∈Q: ⃗θ+λu∈Qand ⃗θ−λu∈Qfor allu∈ {±1} d}

Reference 2

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No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-08T01:06:15.103948Z digest=sha256:b603a58ef88c9f02bcffee5f23f835287dc5024ff7a669780439a5d6583d6fe8

Observation 7717f7e4-24d6-4281-ac40-4e8579b9fd37 · outbound

This paper cites This is sufficient for proving convergence, but it does not use the potential local structure of detector data in a QEC circuit.

Provably Efficient Self-Calibrating Quantum Fault Tolerance This is sufficient for proving convergence, but it does not use the potential local structure of detector data in a QEC circuit

Reference 3

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source=pdf_text observed=2026-08-08T01:06:15.094398Z digest=sha256:813c18c05a275b90a1e9cf639147319d97b1634c0e9151edecdd869bdbbf309d

Observation 83e3d841-4430-4dc8-ac15-4d124ced2c19 · outbound

This paper cites an unresolved cited work.

Provably Efficient Self-Calibrating Quantum Fault Tolerance Unresolved cited work

Reference 4

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source=pdf_text observed=2026-08-08T01:06:15.108285Z digest=sha256:e04c4fd6eb894964c8c4a3ffe4dafc5a553efde2fd05783a6ca1f4f95807979c

Observation a68603db-6b9c-4b5f-a6ed-86d13e25300a · outbound

This paper cites The setting is the same as for Theorem 9.

Provably Efficient Self-Calibrating Quantum Fault Tolerance The setting is the same as for Theorem 9

Reference 5

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Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-08T01:06:15.113156Z digest=sha256:0e2053a18e1ce82dba831aa68077b8f52065c1ad05179dfaef270abea1c2f184

Observation e6caaaa0-88b3-48ae-b39d-56428cc24190 · outbound

This paper cites However, now we do not assume that we remain inside the convex ball of Appendix A.

Provably Efficient Self-Calibrating Quantum Fault Tolerance However, now we do not assume that we remain inside the convex ball of Appendix A

Reference 6

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source=pdf_text observed=2026-08-08T01:06:15.117923Z digest=sha256:aeab7c24b6c246da28afdc915f9b3ca489e575b6a7892f6f474ec9259cc53bdc

Observation 30cd7a2c-f382-4576-adba-65751b7b6277 · outbound

This paper cites C(δ ⃗θ+νu)−C(δ ⃗θ) ν uj # . Stacking the coordinates proves the claim. Lemma 20(Hessian identity of Gaussian smoothing).For everyδ ⃗θ∈P, we have ∇2Cν(δ⃗θ) =E u.

Provably Efficient Self-Calibrating Quantum Fault Tolerance C(δ ⃗θ+νu)−C(δ ⃗θ) ν uj # . Stacking the coordinates proves the claim. Lemma 20(Hessian identity of Gaussian smoothing).For everyδ ⃗θ∈P, we have ∇2Cν(δ⃗θ) =E u

Reference 7

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No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-08T01:06:15.122670Z digest=sha256:f7e13ee516c2ff180bf60f259d62316ea677bc9499b79304ffb03369617fab74

Observation 79ce06ca-ba0e-46b8-8043-eeeaed6d95ff · outbound

This paper cites This is the same mechanism as Corollary 3 and Corollary 4 applied to the Gaussian-smoothed gradient and Hessian estimators used for finding anε-SOSP.

Provably Efficient Self-Calibrating Quantum Fault Tolerance This is the same mechanism as Corollary 3 and Corollary 4 applied to the Gaussian-smoothed gradient and Hessian estimators used for finding anε-SOSP

Reference 8

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source=pdf_text observed=2026-08-08T01:06:15.127332Z digest=sha256:c27ebea3d0769d2c0c73ce4d0a9c080d0574191fdad1cfbbdaf02d9a29408bb4

Observation f1c5edc4-63cd-492d-9e35-0be7acac3834 · outbound

This paper cites follow the regularized leader.

Provably Efficient Self-Calibrating Quantum Fault Tolerance follow the regularized leader

Reference 9

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source=pdf_text observed=2026-08-08T01:06:15.131871Z digest=sha256:962be892713d1be9faf2910690a0b2b37c98d0d12161c8deba30e960cd13c1da

Observation c4d52fb5-ec1f-480e-9fbc-6697798b1a29 · outbound

This paper cites These two states can be coupled by the laser, and single qubit gates can be implemented with high fidelity by tuning the Rabi frequency and the detuning of the laser.

Provably Efficient Self-Calibrating Quantum Fault Tolerance These two states can be coupled by the laser, and single qubit gates can be implemented with high fidelity by tuning the Rabi frequency and the detuning of the laser

Reference 10

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source=pdf_text observed=2026-08-08T01:06:15.136695Z digest=sha256:158f126f3aa06395dcee545d6be4837068515851bdf5e990d7d10654f5a50076

Observation fca25a25-1715-4393-a0a0-f4b59a00f64b · outbound

This paper cites The CZ condition requiresξ 11 − ξ01 −ξ 10 =π.

Provably Efficient Self-Calibrating Quantum Fault Tolerance The CZ condition requiresξ 11 − ξ01 −ξ 10 =π

Reference 11

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No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-08T01:06:15.141355Z digest=sha256:407b250a68f496d9b614764ccde5740968be30df9a71325f0be7a3c02b466132

Observation b0b683ca-4b48-4fec-9513-1c446e70132f · outbound

This paper cites As shown before, there are two pulse control parameters: the laser phaseφ(t)and the laser amplitude|Ω|.

Provably Efficient Self-Calibrating Quantum Fault Tolerance As shown before, there are two pulse control parameters: the laser phaseφ(t)and the laser amplitude|Ω|

Reference 12

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source=pdf_text observed=2026-08-08T01:06:15.145507Z digest=sha256:6557c00cd4d358fc45f0b20ee74f9a6f8349d7eaaf3985a504223f7e7c90a6f9

Observation 30d335d4-7c05-4885-a401-efd0aa2cdcb4 · outbound

This paper cites The code is the[ [4,1,2] ]quantum detection code with four physical qubits and three ancillary qubits.

Provably Efficient Self-Calibrating Quantum Fault Tolerance The code is the[ [4,1,2] ]quantum detection code with four physical qubits and three ancillary qubits

Reference 13

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source=pdf_text observed=2026-08-08T01:06:15.150062Z digest=sha256:dd8f3201bb954432255c10c587803756816494477fc5a7f88162e9c512dddbcd

Observation fe7a4e58-1b99-4e91-855b-2b6711a1a291 · outbound

This paper cites The correctionQ= CZ·P·CZ † (which is also a Pauli up to phase since CZ is Clifford) is applied after.

Provably Efficient Self-Calibrating Quantum Fault Tolerance The correctionQ= CZ·P·CZ † (which is also a Pauli up to phase since CZ is Clifford) is applied after

Reference 14

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No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-08T01:06:15.154403Z digest=sha256:c04035274dbe9889794a70fbeca776eddd8e595e8e24965e3e7c90bd7a255ff7

Observation 26f45665-d317-4db7-9e62-a6335437e9c6 · outbound

This paper cites The circuit consists of three phases: 1.MeasureS 1:Hadamard on data qubitsq 0–q3 (basis changeX→Z), Hadamard ona 0, four CZ gates(q i, a0), Hadamard ona 0, Hadamard on data qubits.

Provably Efficient Self-Calibrating Quantum Fault Tolerance The circuit consists of three phases: 1.MeasureS 1:Hadamard on data qubitsq 0–q3 (basis changeX→Z), Hadamard ona 0, four CZ gates(q i, a0), Hadamard ona 0, Hadamard on data qubits

Reference 15

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source=pdf_text observed=2026-08-08T01:06:15.158427Z digest=sha256:9268bc7aa8668fad8807c7a1a3685da0557ba5bacd074c3f3b2635e342c3ba8f

Observation 9d3ed87a-c1d8-4d6c-8404-20cd3bb3dbd6 · outbound

This paper cites The key computational tool is thequantum instrumentformalism using Kraus operators.

Provably Efficient Self-Calibrating Quantum Fault Tolerance The key computational tool is thequantum instrumentformalism using Kraus operators

Reference 16

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source=pdf_text observed=2026-08-08T01:06:15.162482Z digest=sha256:7fb202d9e4d0898bbfe70dd1f27ea51f6c7c206c2f40e5118a8a811615179c50

Observation 8e680519-2439-49ae-b53a-12bd6e3f6558 · outbound

This paper cites an unresolved cited work.

Provably Efficient Self-Calibrating Quantum Fault Tolerance Unresolved cited work

Reference 17

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source=pdf_text observed=2026-08-08T01:06:15.166972Z digest=sha256:6fa16dde745aa9bb33c90ef2951fcd5c260d5db9f4228da689982cd4ed9a52b1

Observation 8148590b-1e71-4174-8aef-b26e14ff1a5b · outbound

This paper cites , ngate}carriesPlocal control parameters (we useP= 5throughout), collected inp i ∈R P , and the corresponding hardware setpoint drifts top drift i.

Provably Efficient Self-Calibrating Quantum Fault Tolerance , ngate}carriesPlocal control parameters (we useP= 5throughout), collected inp i ∈R P , and the corresponding hardware setpoint drifts top drift i

Reference 18

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source=pdf_text observed=2026-08-08T01:06:15.171275Z digest=sha256:b0c01b8fb753327f0dcc56d5a960be43060554262e41472ece44812e53278118

Observation 9d4dab79-2a08-4846-8c7e-b8dd5dda4d2e · outbound

This paper cites Its objective is the mean detection rate DR(p) = 1 ND NDX k=1 DRk(p), DR k(p) = Pr[detectorkfires],(F4) estimated frommMonte Carlo shots of the compiled detector sampler.

Provably Efficient Self-Calibrating Quantum Fault Tolerance Its objective is the mean detection rate DR(p) = 1 ND NDX k=1 DRk(p), DR k(p) = Pr[detectorkfires],(F4) estimated frommMonte Carlo shots of the compiled detector sampler

Reference 20

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source=pdf_text observed=2026-08-08T01:06:15.179769Z digest=sha256:66b61908cfb5c41267a40feea23b48fa1a750b18281aac92dffe42558ba1296c

Observation 7fe961f9-05fd-41b2-9750-466f9ae0260c · outbound

This paper cites calibration event.

Provably Efficient Self-Calibrating Quantum Fault Tolerance calibration event

Reference 42

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source=pdf_text observed=2026-08-08T01:06:15.175476Z digest=sha256:75f9ef58c1b20bf981f6ba93de1d0ba237df27d586da56e297446396df06a931

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