Pith. sign in

Paper Citation Record · LEDGER

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits

As of 22 August 2026, this Paper Citation Record lists 38 of 38 outbound references and 2 inbound Pith citation observations for arXiv:2605.21346.

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

pith.paper-citation-record.v1
2605.21346 v1

Coverage vector

measured 38 of 38 reference resolution

Typed states for the displayed outbound observations.

Source: paper_references, paper_reference_links, observed 2026-05-21T04:26:05.688196Z

measured 40 of 40 standing notices

One-hop event checks from named stored sources.

Source: scholarly_work_events, retraction_status_cache, observed 2026-08-22T06:32:14.747728+00:00

measured 2 of 2 inbound itemization

Pith citing papers itemized under the disclosed page cap.

Source: paper_references, paper_reference_links, observed 2026-08-16T01:05:10.328636Z

measured 0 of 1 external citation measurements

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

Source: pith, observed 2026-08-16T01:05:10.722603Z

Reference resolution

38 of 38 outbound references displayed

  • verified exact0
  • verified fuzzy23
  • unresolved14
  • parse uncertain0
  • malformed identifier1
  • metadata mismatch0

External citation measurements

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Outbound references

Observation ca56ffbe-9994-4e4f-a11e-dd53165d97fa · outbound

This paper cites 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.

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

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:28fb6e195d9ec9f7c4e607ecfd65781dd96fcb7829719e02b0cebe84b3fbe152

Observation f6125908-2974-4531-a0ac-efad3e240be0 · outbound

This paper cites This motivates the decomposition of the register into: A(α) :={i:α i = 1},P(α) :={i:α i = 0},(D4) with|A|=|α|.

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

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:ce5ba34b561ef0e1569b3063fe989ee7d552f4c4d75c44ea149ca4a75d831926

Observation 8a2e7774-8906-4fed-83aa-8e9d7a019763 · outbound

This paper cites feeding terms.

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits feeding terms

Reference 3

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:9255aefa855813f48b80ccd18de71b9a9ec3875ced724a167faa637d38f340df

Observation a593cc02-0e03-4923-aa0a-3820d140ea86 · outbound

This paper cites On an active qubit, the relevant local operator is |0⟩ ⟨1|or|1⟩ ⟨0|, both of which acquire a minus sign under conjugation byZ.

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

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:7acdd509f6fc0c5a805c0c724c432bffbd6e3c0d15cfe658944b3d12d535ca6d

Observation 07561294-0501-4cf7-905c-8a51e7aae867 · outbound

This paper cites 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.

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

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:f4bd9651374974dc5ec4125221a65d43a6445e88caa7b2688fa24b7fcdac946d

Observation a2ae289f-6a36-4f73-8c96-d98542acb8d9 · outbound

This paper cites For an active qubit, the only index-preserving contribution comes fromK0, givingK 0 |0⟩ ⟨1|K† 0 = p1−ϵ p |0⟩ ⟨1|.

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

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:2c50f15ca5399a4ef6158fcae17453098f0841bdcc4c53b606570de5e5605870

Observation 860b1c9f-0233-490a-921a-7e9d19c6811a · outbound

This paper cites 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.

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

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:ff74ec55c807d4c4b70a75f923a2c3d06204c0fe67cbabf8e2e57456470a665f

Observation 2ba2fa27-610d-4ba1-a18c-887fd875a72b · outbound

This paper cites an unresolved cited work.

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work

Reference 8

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:3d6c44076841063ccb9d2672753da8f4609ab15441f3505dea877297755d926c

Observation 7bcbd172-3b7c-401b-9f77-f162d5a29c83 · outbound

This paper cites These platforms feature native all-to-all connectivity, achieved through shared motional bus modes or the coherent transport of qubits [63, 64].

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

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:2c3349988b9a3352937da4a40aa511fa63d20ba0883117de0a0acaeecacb4c0c

Observation 985c4f54-1a5a-4478-ac1c-21f554d2b53b · outbound

This paper cites an unresolved cited work.

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work

Reference 10

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:ea61156859789f13e1bcfc63d014e41cf67df41035aaef4ffda934f08236d613

Observation 4b7f6129-e7ab-4df0-80dc-474cbd3d49c9 · outbound

This paper cites an unresolved cited work.

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work

Reference 11

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:d8f0d19c9c4faa93c153eec449e011a7960d5f45aff96eb942af1a7c7032cdb9

Observation c7fbcb7f-2b39-4b87-9013-dde978b1a51f · outbound

This paper cites an unresolved cited work.

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work

Reference 12

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:69704934d87e31e0cc43fb10b56662b33762cc941dd32cbd9349612d944b1b2f

Observation 9697ce90-5039-4645-b8ba-7073fd37cb3c · outbound

This paper cites Like superconducting qubits, theygenerallyrelyonplanarnearest-neighborconnectivityviaexchangeinteractions, incurringidenticalSWAP routing penalties [95].

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Like superconducting qubits, theygenerallyrelyonplanarnearest-neighborconnectivityviaexchangeinteractions, incurringidenticalSWAP routing penalties [95]

Reference 13

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:941a31257c132a1cc3f020abdcd899dbd64bd1f5609705ddef3e2b7efd470fe1

Observation 3079c4df-ae42-4c60-abe5-8c7eb7fb5949 · outbound

This paper cites an unresolved cited work.

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work

Reference 14

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:5f1bd5325eac1580b5ffdd1d89bb833e23e93b8c75b21551895b2ae9844b291f

Observation 9d1f59fc-a9f7-49fa-b1cc-84e30c6ec0f9 · outbound

This paper cites In the local-Clifford shadow protocol, each measurement shotk∈ {1.

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits In the local-Clifford shadow protocol, each measurement shotk∈ {1

Reference 15

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:3cbdb3e2a4064303fdaf0e7ff2ea2bd772c0e09a72e2d55064691b05524c699d

Observation 9b426785-aaad-4cc5-9c4d-be3f772481ea · outbound

This paper cites an unresolved cited work.

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work

Reference 16

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:b47f2a4e49168ee938d63f85bf47012488262949377ad833cf6ea67c771edc7b

Observation bc8a56fa-8015-4a63-bc42-12d1d8813a0d · outbound

This paper cites an unresolved cited work.

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work

Reference 17

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:820e9d7e25d8abb234371b71a4f1991749dbcd7da85253aa89f750240f87bfc7

Observation 1248a7bf-1d02-4021-a52a-e64ba7683e37 · outbound

This paper cites If the two masks differ, the corresponding Pauli support sets are disjoint, and the covariance vanishes.

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

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:57ac0032a57dd52fdd2b85c8adb48d488235a6539b2d8bf9e5aacc9d823e5b8e

Observation ddeafa47-73ec-4359-9bd1-09599028f903 · outbound

This paper cites Define the canonical representative setS ∆ :={n∈ {0,1} nq :n h(∆) = 0}.

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

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:8d18a5ed4cb299a8d5fee48ba09e1d98156be43792f0930f89fd51c5cfe4c6de

Observation 0c3f778d-dabf-4dbb-a106-45867cdfee79 · outbound

This paper cites 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.

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

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:7564d9a851e53f5ba602ac03eca18369f05f243ea8b5554ede08fd42a0664a39

Observation b41ed722-1bbc-43ac-89e6-341b064b6b0c · outbound

This paper cites an unresolved cited work.

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:cb7ddfcf027de6290c240404f145dbc2c2c298e6be11d6c849c96ccfa2aea308

Observation c04d3f78-97ad-48aa-855d-85aa42f0bb16 · outbound

This paper cites 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.

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

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:4880e1c52a6d06b44e14baacb943cfcf7a599d78280a9a9e3c9bd0c8da7996bc

Observation caacdc48-7fbe-4467-99e2-43faf52d15a3 · outbound

This paper cites We define the Signal- to-Noise Ratio asSN R= |µ| σ.

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits We define the Signal- to-Noise Ratio asSN R= |µ| σ

Reference 23

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:955a65ecc205b500b4c77182d5e016319b5209673b3b412636a11248474bc3f4

Observation 92361016-f07e-4a51-bdc6-989e62d4ad37 · outbound

This paper cites an unresolved cited work.

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work

Reference 24

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:de3fc9def5ed9c4bd4a491856d1b5d287a9c21081d26f910031f10cf11738fea

Observation 7b81cdac-1d94-42f8-8018-bf122f4eafd5 · outbound

This paper cites an unresolved cited work.

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:a776b21a72cde860ef4e84b0ada5451a8c15706415f6d982b8c1527c12ae7518

Observation 3c6e5f70-63fb-40e0-8542-ac2bd178384b · outbound

This paper cites We partition the qubit indices into the Active SetA(whereαk = 1) and the Passive SetP(whereα k = 0).

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

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:84a4b3c37d096c843a05784b044160d05f55d1def83f7bea068f2bf557c00ef6

Observation 31149a30-08ce-4fed-a22f-358e84a23fb8 · outbound

This paper cites an unresolved cited work.

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work

Reference 27

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:39498d55576d73eb839e9d0c89ef87a5187a2a7709aeb73daa965c6366486ae6

Observation 50905c47-196d-4bc5-8f28-c7d24ed6924f · outbound

This paper cites 3 2 w(y⊕α,t) −4 −nq # ,(H6) Ef[Varsh(∆ct |f)] = 1 nc.

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

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source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:ed23dbe1cab66d745d24c4dc9ecf5e50fce69063ea21b166892db40901b71c7c

Observation bb3183bd-2b69-4144-a6c4-a6c06bd84a99 · outbound

This paper cites 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.

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

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No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.

source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:8b6ff0aaa75522a518341bc4133278d75b3191e84038fdd5c288d37f68ae57d3

Observation 166ca66c-0f77-41f1-82c5-5e17c8c86f32 · outbound

This paper cites 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.

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

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No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.

source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:b4c894882fc446dbfc33a80bbe6dbeeba56e38dba6cfa48f84386ea3136154e1

Observation 7c1b15fc-549c-447f-b8de-f1a66a013cb0 · outbound

This paper cites an unresolved cited work.

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work

Reference 31

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Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.

source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:05902a70629877861361445be196a4c3a4eabf3e870fa11815371412c0cfcade

Observation f5cc97da-f58e-4ce7-bc70-edd0a0c1b125 · outbound

This paper cites an unresolved cited work.

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work

Reference 32

Resolution
unresolved
raw_fallback, observed 2026-05-21T09:54:58.707906Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.

source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:49781f94433b966834c71920cb7973b5de9fb5da305ba78a937eaca2b9ae1d29

Observation f6b0fd65-cdc5-4032-8bb8-a79543e0f3e0 · outbound

This paper cites To recover the true coefficients, we sort the rows of the augmented matrix[Y|b]in descending order based on empirical observation frequencies.

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

Resolution
verified fuzzy
raw_fallback, observed 2026-05-21T09:54:58.692740Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.

source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:50c106c65ceb192b7b3659539c7417fadb9a318c94e33b2763568255105c1733

Observation ff77123d-9305-4b54-9a65-d875d58735e0 · outbound

This paper cites an unresolved cited work.

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Unresolved cited work

Reference 34

Resolution
unresolved
raw_fallback, observed 2026-05-21T09:54:58.655083Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.

source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:85a2f69ab3a598f6310d18ea7d4b043042dba0ef38a3b89bfb45e320c0a24984

Observation 95a809c3-2566-47e2-bf8d-eab7a9639d6a · outbound

This paper cites This yields, for each thresholdT, n k(b) x (T, nq) oB b=1 ,(J10) withB= 1600in the production runs.

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

Resolution
verified fuzzy
raw_fallback, observed 2026-05-21T09:54:58.666574Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.

source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:4b56cef96836f40ce37eff4e5dbc709c44d83e797a52ec7a5297a8551072c817

Observation a849c3d7-679b-4541-b876-1b0eb78859ea · outbound

This paper cites Equation (J14) is used here as the minimal phenomenological extrapolation ansatz.

Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits Equation (J14) is used here as the minimal phenomenological extrapolation ansatz

Reference 36

Resolution
verified fuzzy
raw_fallback, observed 2026-05-21T09:54:58.676222Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.

source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:ef127cf9ef4e0c9f8460fd2218e36ca2feac4f98a4b34399139d64e4ecc46bae

Observation d6a29ff6-611c-4fc1-8d10-9ef3aac18971 · outbound

This paper cites The readout contributionϵr enters only through this quantum target, because the classical measure-first estimators themselves do not depend directly on readout noise.

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

Resolution
verified fuzzy
raw_fallback, observed 2026-05-21T09:54:58.709834Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.

source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:4168c3e52aedd45f2a2cd6d79b07196d1cf3d8f8e515bc0473e5c5c257ecbb2c

Observation 96d09961-01fe-415d-a727-c3621fa322db · outbound

This paper cites Because the model (J14) is fit independently at each threshold, small violations of this property can appear after interpolation in T.

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

Resolution
verified fuzzy
raw_fallback, observed 2026-05-21T09:54:58.687496Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.

source=pdf_text observed=2026-05-21T04:26:05.688196Z digest=sha256:6d169c6a21968c9caaa45000d32c97091b4dbc3ce85664d561c22f1405fb51e6

Pith citing papers

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 cites this paper.

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

Resolution
unresolved
no resolver link, observed 2026-08-01T22:20:48.105856Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-01T22:20:48.105856Z digest=sha256:56713643399c5f4adf8b59b3f04893b31eb46d7b5fb3fb608bf747f890771b53

Observation ac03126c-014e-471e-8174-2775e71d9ce4 · inbound

Parity Floors in Quantum Denoisers: A Closed-Form Benchmark for Fixed-Map Denoising Networks cites this paper.

Parity Floors in Quantum Denoisers: A Closed-Form Benchmark for Fixed-Map Denoising Networks Evidence of Quantum Machine Learning Advantage with Tens of Noisy Qubits

Reference 5

Resolution
verified exact
local_arxiv, observed 2026-08-16T01:05:10.727548Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.

source=arxiv_source observed=2026-08-16T01:05:10.328636Z digest=sha256:daf11b4ea791560f3c6cc725c23766233e446aa2c53db585f918aa2faaffcc2d