Typed states for the displayed outbound observations.
Source: paper_references, paper_reference_links, observed 2026-05-21T04:26:05.688196Z
Paper Citation Record · LEDGER
As of 12 August 2026, this Paper Citation Record lists 38 of 38 outbound references and 1 inbound Pith citation observation for arXiv:2605.21346.
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 2026-05-21T04:26:05.688196Z
One-hop event checks from named stored sources.
Source: scholarly_work_events, retraction_status_cache, observed 2026-08-12T06:34:41.77262+00:00
Pith citing papers itemized under the disclosed page cap.
Source: paper_references, paper_reference_links, observed 2026-08-01T22:20:48.105856Z
A source-named dated measurement, never combined with another source.
Source: cited_works
38 of 38 outbound references displayed
External citation measurements
No source-named external measurement is stored.
Observation ca56ffbe-9994-4e4f-a11e-dd53165d97fa · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Utilizing the full pipeline from Appendix B, we compute exact points atnq ∈ {12,14} and|α| ∈ {n q/2, nq}across a selection of devices and noise channels affecting quantum data
Reference 1
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.
Observation f6125908-2974-4531-a0ac-efad3e240be0 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits This motivates the decomposition of the register into: A(α) :={i:α i = 1},P(α) :={i:α i = 0},(D4) with|A|=|α|
Reference 2
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.
Observation 8a2e7774-8906-4fed-83aa-8e9d7a019763 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits feeding terms
Reference 3
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.
Observation a593cc02-0e03-4923-aa0a-3820d140ea86 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits On an active qubit, the relevant local operator is |0⟩ ⟨1|or|1⟩ ⟨0|, both of which acquire a minus sign under conjugation byZ
Reference 4
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.
Observation 07561294-0501-4cf7-905c-8a51e7aae867 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits For an active qubit, the X- andY-terms map|0⟩ ⟨1|to|1⟩ ⟨0|(feeding terms that average to zero), while theZ-term contributes a minus sign
Reference 5
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.
Observation a2ae289f-6a36-4f73-8c96-d98542acb8d9 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits For an active qubit, the only index-preserving contribution comes fromK0, givingK 0 |0⟩ ⟨1|K† 0 = p1−ϵ p |0⟩ ⟨1|
Reference 6
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.
Observation 860b1c9f-0233-490a-921a-7e9d19c6811a · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits From Appendix A, the ensemble-averaged accuracy is: AQ(α) :=E f[AQ(α|f)] = 1 2 1 + ¯γ(α) ,(D13) 28 where¯γ(α) = 1 2nq −1 P y′ γy,α
Reference 7
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.
Observation 2ba2fa27-610d-4ba1-a18c-887fd875a72b · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work
Reference 8
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.
Observation 7bcbd172-3b7c-401b-9f77-f162d5a29c83 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits These platforms feature native all-to-all connectivity, achieved through shared motional bus modes or the coherent transport of qubits [63, 64]
Reference 9
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.
Observation 985c4f54-1a5a-4478-ac1c-21f554d2b53b · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work
Reference 10
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.
Observation 4b7f6129-e7ab-4df0-80dc-474cbd3d49c9 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work
Reference 11
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.
Observation c7fbcb7f-2b39-4b87-9013-dde978b1a51f · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work
Reference 12
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.
Observation 9697ce90-5039-4645-b8ba-7073fd37cb3c · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Like superconducting qubits, theygenerallyrelyonplanarnearest-neighborconnectivityviaexchangeinteractions, incurringidenticalSWAP routing penalties [95]
Reference 13
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.
Observation 3079c4df-ae42-4c60-abe5-8c7eb7fb5949 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work
Reference 14
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.
Observation 9d1f59fc-a9f7-49fa-b1cc-84e30c6ec0f9 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits In the local-Clifford shadow protocol, each measurement shotk∈ {1
Reference 15
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.
Observation 9b426785-aaad-4cc5-9c4d-be3f772481ea · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work
Reference 16
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.
Observation bc8a56fa-8015-4a63-bc42-12d1d8813a0d · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work
Reference 17
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.
Observation 1248a7bf-1d02-4021-a52a-e64ba7683e37 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits If the two masks differ, the corresponding Pauli support sets are disjoint, and the covariance vanishes
Reference 18
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.
Observation ddeafa47-73ec-4359-9bd1-09599028f903 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Define the canonical representative setS ∆ :={n∈ {0,1} nq :n h(∆) = 0}
Reference 19
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.
Observation 0c3f778d-dabf-4dbb-a106-45867cdfee79 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits What remains is only the subtraction term from the mean, yielding: R(∆) n,p =− 4−nq nc δn,p.(F23) Thus the residual pseudo-covariance is diagonal and exponentially small innq
Reference 20
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.
Observation b41ed722-1bbc-43ac-89e6-341b064b6b0c · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work
Reference 21
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.
Observation c04d3f78-97ad-48aa-855d-85aa42f0bb16 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits We find that the surrogate accurately reproduces the scaling of the element-wise variances across the system sizes and shot counts relevant to this work
Reference 22
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.
Observation caacdc48-7fbe-4467-99e2-43faf52d15a3 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits We define the Signal- to-Noise Ratio asSN R= |µ| σ
Reference 23
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.
Observation 92361016-f07e-4a51-bdc6-989e62d4ad37 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work
Reference 24
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.
Observation 7b81cdac-1d94-42f8-8018-bf122f4eafd5 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work
Reference 25
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.
Observation 3c6e5f70-63fb-40e0-8542-ac2bd178384b · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits We partition the qubit indices into the Active SetA(whereαk = 1) and the Passive SetP(whereα k = 0)
Reference 26
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.
Observation 31149a30-08ce-4fed-a22f-358e84a23fb8 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work
Reference 27
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.
Observation 50905c47-196d-4bc5-8f28-c7d24ed6924f · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits 3 2 w(y⊕α,t) −4 −nq # ,(H6) Ef[Varsh(∆ct |f)] = 1 nc
Reference 28
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.
Observation bb3183bd-2b69-4144-a6c4-a6c06bd84a99 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Since the numerical study is performed in the gaugey= 0nq, Hamming shells around the target locationyare indexed simply by the Hamming weight of the intermediate bit stringt
Reference 29
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.
Observation 166ca66c-0f77-41f1-82c5-5e17c8c86f32 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits The model assigns to each sample a score s(x) =w ⊤x+β 0,(H14) wherewis the vector of feature weights andβ0 is an intercept parameter
Reference 30
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.
Observation 7c1b15fc-549c-447f-b8de-f1a66a013cb0 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work
Reference 31
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.
Observation f5cc97da-f58e-4ce7-bc70-edd0a0c1b125 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work
Reference 32
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.
Observation f6b0fd65-cdc5-4032-8bb8-a79543e0f3e0 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits To recover the true coefficients, we sort the rows of the augmented matrix[Y|b]in descending order based on empirical observation frequencies
Reference 33
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.
Observation ff77123d-9305-4b54-9a65-d875d58735e0 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work
Reference 34
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.
Observation 95a809c3-2566-47e2-bf8d-eab7a9639d6a · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits This yields, for each thresholdT, n k(b) x (T, nq) oB b=1 ,(J10) withB= 1600in the production runs
Reference 35
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.
Observation a849c3d7-679b-4541-b876-1b0eb78859ea · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Equation (J14) is used here as the minimal phenomenological extrapolation ansatz
Reference 36
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.
Observation d6a29ff6-611c-4fc1-8d10-9ef3aac18971 · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits The readout contributionϵr enters only through this quantum target, because the classical measure-first estimators themselves do not depend directly on readout noise
Reference 37
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.
Observation 96d09961-01fe-415d-a727-c3621fa322db · outbound
Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Because the model (J14) is fit independently at each threshold, small violations of this property can appear after interpolation in T
Reference 38
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.
Observation a2a4f161-1401-456f-867d-c01aca893cd4 · inbound
The Fourier Wall: Why Public Tabular Datasets Refuse Quantum Advantage, and a Certified Recipe for Where It Lives Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits
Reference 23
Source-reported events for the cited work
Unavailable: canonical work link unavailable.