Typed states for the displayed outbound observations.
Source: paper_references, paper_reference_links, observed 2026-08-08T01:06:15.179769Z
Paper Citation Record · LEDGER
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.
Typed states for the displayed outbound observations.
Source: paper_references, paper_reference_links, observed 2026-08-08T01:06:15.179769Z
One-hop event checks from named stored sources.
Source: scholarly_work_events, retraction_status_cache, observed 2026-08-13T06:32:02.005865+00:00
Pith citing papers itemized under the disclosed page cap.
Source: paper_references, paper_reference_links
A source-named dated measurement, never combined with another source.
Source: cited_works
20 of 20 outbound references displayed
External citation measurements
No source-named external measurement is stored.
Observation 327297be-da07-456a-af2e-1d313b00514c · outbound
Provably Efficient Self-Calibrating Quantum Fault Tolerance Recall from Eq
Reference 1
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation 8a71d8bc-52f6-45f7-85ce-4b3f32214139 · outbound
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
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation 7717f7e4-24d6-4281-ac40-4e8579b9fd37 · outbound
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
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation 83e3d841-4430-4dc8-ac15-4d124ced2c19 · outbound
Provably Efficient Self-Calibrating Quantum Fault Tolerance Unresolved cited work
Reference 4
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation a68603db-6b9c-4b5f-a6ed-86d13e25300a · outbound
Provably Efficient Self-Calibrating Quantum Fault Tolerance The setting is the same as for Theorem 9
Reference 5
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation e6caaaa0-88b3-48ae-b39d-56428cc24190 · outbound
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
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation 30cd7a2c-f382-4576-adba-65751b7b6277 · outbound
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
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation 79ce06ca-ba0e-46b8-8043-eeeaed6d95ff · outbound
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
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation f1c5edc4-63cd-492d-9e35-0be7acac3834 · outbound
Provably Efficient Self-Calibrating Quantum Fault Tolerance follow the regularized leader
Reference 9
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation c4d52fb5-ec1f-480e-9fbc-6697798b1a29 · outbound
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
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation fca25a25-1715-4393-a0a0-f4b59a00f64b · outbound
Provably Efficient Self-Calibrating Quantum Fault Tolerance The CZ condition requiresξ 11 − ξ01 −ξ 10 =π
Reference 11
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation b0b683ca-4b48-4fec-9513-1c446e70132f · outbound
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
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation 30d335d4-7c05-4885-a401-efd0aa2cdcb4 · outbound
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
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation fe7a4e58-1b99-4e91-855b-2b6711a1a291 · outbound
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
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation 26f45665-d317-4db7-9e62-a6335437e9c6 · outbound
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
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation 9d3ed87a-c1d8-4d6c-8404-20cd3bb3dbd6 · outbound
Provably Efficient Self-Calibrating Quantum Fault Tolerance The key computational tool is thequantum instrumentformalism using Kraus operators
Reference 16
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation 8e680519-2439-49ae-b53a-12bd6e3f6558 · outbound
Provably Efficient Self-Calibrating Quantum Fault Tolerance Unresolved cited work
Reference 17
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation 8148590b-1e71-4174-8aef-b26e14ff1a5b · outbound
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
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation 9d4dab79-2a08-4846-8c7e-b8dd5dda4d2e · outbound
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
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
Observation 7fe961f9-05fd-41b2-9750-466f9ae0260c · outbound
Provably Efficient Self-Calibrating Quantum Fault Tolerance calibration event
Reference 42
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.
No inbound Pith citation observations are available.