Typed states for the displayed outbound observations.
Source: paper_references, paper_reference_links, observed 2026-08-02T02:40:01.978372Z
Paper Citation Record · LEDGER
As of 14 August 2026, this Paper Citation Record lists 31 of 31 outbound references and 1 inbound Pith citation observation for arXiv:2607.14308.
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 2026-08-02T02:40:01.978372Z
One-hop event checks from named stored sources.
Source: scholarly_work_events, retraction_status_cache, observed 2026-08-14T06:32:32.682623+00:00
Pith citing papers itemized under the disclosed page cap.
Source: paper_references, paper_reference_links, observed 2026-07-31T07:47:18.817329Z
A source-named dated measurement, never combined with another source.
Source: cited_works
31 of 31 outbound references displayed
External citation measurements
No source-named external measurement is stored.
Observation f6c8a83d-3838-45d0-88d9-a8ee2d0d4b0e · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup Unresolved cited work
Reference 1
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation f877b256-53ee-44a5-a14f-5daad211c1fa · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup The precise statement is now given
Reference 2
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Unavailable: canonical work link unavailable.
Observation 6c6bbce2-f8c1-4d02-9127-4379ec7b9b7b · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup We make the natural choice of a hard-core cut-off for∥x∥ ≤a, whereais the cut-off scale
Reference 3
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Unavailable: canonical work link unavailable.
Observation da9ec89f-6104-45ec-a981-2ca95003fd6e · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup , NF}3, each spatial variable is represented by a finite Fourier series
Reference 4
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Unavailable: canonical work link unavailable.
Observation a2e3c833-9b7b-441d-a4e8-5a8229493f97 · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup We assume for simplicity that a given matrix transforms definite numbers of qubits, so the dimensions are power of 2
Reference 5
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Unavailable: canonical work link unavailable.
Observation 91b42c5c-fa8d-4400-9fdc-f15f5f9df7e9 · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup Unresolved cited work
Reference 6
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Unavailable: canonical work link unavailable.
Observation 91694e7a-c7a8-4c6b-9fdb-0fe842e528ee · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup blocks” associated to well-separated points and small “blocks
Reference 7
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Unavailable: canonical work link unavailable.
Observation 18b2f147-f3b8-4bf6-80fb-f5bb596fe58c · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup Unresolved cited work
Reference 8
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Observation 966b1d39-2236-4ecc-a674-6aab7f895f2f · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup 49 referenceadjacent(8 clusters)𝑙=4(27 clusters)𝑙=3(27 clusters)𝑙=2(7 clusters) FIG
Reference 9
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Observation c7b86913-d671-4661-b67c-1e6e27947136 · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup Unresolved cited work
Reference 10
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Unavailable: canonical work link unavailable.
Observation 3b5ac177-7a55-486d-b0e6-c717ee3927ec · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup Unresolved cited work
Reference 11
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Unavailable: canonical work link unavailable.
Observation 37371323-8ae3-4786-9369-09627c03be3d · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup Unresolved cited work
Reference 12
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Unavailable: canonical work link unavailable.
Observation 3944e99c-63ff-405b-9e46-1bb6c61488ee · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup clusters
Reference 13
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Unavailable: canonical work link unavailable.
Observation f5214dd7-2215-435d-9321-37ac68f54dd0 · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup Unresolved cited work
Reference 14
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Unavailable: canonical work link unavailable.
Observation 5440e46d-3bbf-41ce-925c-42d5897ad8c6 · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup Unresolved cited work
Reference 15
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Unavailable: canonical work link unavailable.
Observation bc38af62-0a4f-4c24-985f-6bebbf87547e · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup Unresolved cited work
Reference 16
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Unavailable: canonical work link unavailable.
Observation 72fd186e-a502-450f-b084-bb1489a2d18a · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup Unresolved cited work
Reference 17
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Unavailable: canonical work link unavailable.
Observation 8a9862c5-b6c8-4cca-9998-d9da86b7facf · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup ,2l −1, and all clusters are disjoint
Reference 18
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Unavailable: canonical work link unavailable.
Observation a32a81d1-0ef5-4244-8e6d-c096fb87ce57 · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup internal
Reference 19
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Unavailable: canonical work link unavailable.
Observation 141b6919-4000-4008-8ec6-43e1c5e672fc · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup To handle this neatly we give a theorem that is sufficiently flexible to accommodate all cases of interest here
Reference 20
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Unavailable: canonical work link unavailable.
Observation 0271b721-09ec-4a03-8d6e-8680e2091c8f · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup Unresolved cited work
Reference 21
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 7f3baa34-a42e-4da6-a30f-016fa114ec3c · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup We explained how this can be obtained from a block-encodingU K of the real-space dataKdefined earlier, through controlled discrete Fourier transforms
Reference 22
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Unavailable: canonical work link unavailable.
Observation a7d39144-12b1-4e97-b417-75ce60abee09 · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup Then, d dt M(t) =−νM(t).(G1) Consequently, M(t) = e −νtM(0).(G2) In particular, ifM(0) = 0, thenM(t) = 0for allt∈[0, T]
Reference 23
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Observation 44f8e56a-3930-4b7c-8348-5549e5464fba · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup Unresolved cited work
Reference 24
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Unavailable: canonical work link unavailable.
Observation 575ec138-e0a2-4734-bc73-3eb28df6c138 · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup Unresolved cited work
Reference 25
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Unavailable: canonical work link unavailable.
Observation 2caab783-2a64-45a6-b28a-a2fb8388ce42 · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup Moreover, the initial data (8) satisfies (67) att= 0
Reference 26
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Observation 5f1439ca-7fba-4c2e-91d5-a9b54e43ed9b · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup Unresolved cited work
Reference 27
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Observation b9aba1d2-10bb-454a-8299-fb82ce63f9c8 · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup Since the partial sums (H38) are monotone increasing inN F andN H, we also obtain sup (NF,NH)∈N2 ∥u0∥2 2 = X n∈Z3 α∈N3 0 |gn,α(0)|2.(H39) Combining (H36) and (H39) gives (H35)
Reference 28
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Unavailable: canonical work link unavailable.
Observation 7a5704d7-9d09-48fb-9f68-e4bf6edbf679 · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup For any subset Ω⊆Z 3×N3 0, define the truncation operatorT Ω through its Fourier-Hermite coefficients, by (TΩg)n,α := ( gn,α (n,α)∈Ω, 0 (n,α)/∈Ω
Reference 29
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Unavailable: canonical work link unavailable.
Observation 669f1232-2055-4f54-a34e-1ced982d0aa1 · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup Unresolved cited work
Reference 30
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Unavailable: canonical work link unavailable.
Observation 8dfbb960-de95-4107-b1d0-c82a2019cda7 · outbound
An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup We must therefore construct a state preparation routine for the normalized state| ¯ℓK,k⟩
Reference 31
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Observation 2ac84d3b-5ff3-4229-9c5e-343c03d3d962 · inbound
Improved Convergence of Carleman-Embedded Quantum Algorithm for the Vlasov-Poisson System An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup
Reference 35
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Unavailable: canonical work link unavailable.