{"as_of":"2026-08-14T23:06:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:91a44a54ea0391acefe27a77dfb83bfd50e9f5509145792139929bf470814a7c","coverage":[{"denominator":31,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":31,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-02T02:40:01.978372Z","state":"measured"},{"denominator":32,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":32,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-14T06:32:32.682623+00:00","state":"measured"},{"denominator":1,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":1,"source":"paper_references, paper_reference_links","source_observed_at":"2026-07-31T07:47:18.817329Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2607.14308","snapshot_observed_at":"2026-07-31T07:47:18.817329Z","title":null,"venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.28426","last_updated":"2026-07-30T16:04:42Z","snapshot_observed_at":"2026-08-09T22:11:01.939004Z","submitted_at":"2026-07-30T16:04:42Z","title":"Improved Convergence of Carleman-Embedded Quantum Algorithm for the Vlasov-Poisson System","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-07-31T07:47:18.817329Z"},"links":{"cited_paper":"/paper/2607.14308","citing_paper":"/paper/2607.28426"},"observation_digest":"sha256:897c669a204515e7635143f0c20010486efb31cb0963860ff03c5b4b4ff3857f","observation_id":"2ac84d3b-5ff3-4229-9c5e-343c03d3d962","resolution":{"observed_at":"2026-07-31T07:47:18.817329Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2607.14308/citation-record","integrity":"/paper/2607.14308/integrity","json":"/paper/2607.14308/citation-record.json","paper":"/paper/2607.14308"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:39:56.803149Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-02T02:39:56.803149Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:70dc22b7985729c34e6e4a4c8069c47b8eb6d6936619b6365b3b1bb2fca13364","observation_id":"f6c8a83d-3838-45d0-88d9-a8ee2d0d4b0e","resolution":{"observed_at":"2026-08-02T02:39:56.803149Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:39:56.998318Z","title":"The precise statement is now given","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-02T02:39:56.998318Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:1475d606250e4e8c453d28850b7d363b15ddf0e643dbb86f5b3ab8b95ed6dbe3","observation_id":"f877b256-53ee-44a5-a14f-5daad211c1fa","resolution":{"observed_at":"2026-08-02T02:39:56.998318Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:39:57.226550Z","title":"We make the natural choice of a hard-core cut-off for∥x∥ ≤a, whereais the cut-off scale","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-02T02:39:57.226550Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:40cbf3cf383ab9e52c717b4c4ac9d06d708dfa36b99c5503478301ae2200c23e","observation_id":"6c6bbce2-f8c1-4d02-9127-4379ec7b9b7b","resolution":{"observed_at":"2026-08-02T02:39:57.226550Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:39:57.488256Z","title":", NF}3, each spatial variable is represented by a finite Fourier series","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-02T02:39:57.488256Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:203c27e46a764cd5ac942f189b3dbf466a7ced771218b5263fc288a8b68c0a47","observation_id":"da9ec89f-6104-45ec-a981-2ca95003fd6e","resolution":{"observed_at":"2026-08-02T02:39:57.488256Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:39:57.683408Z","title":"We assume for simplicity that a given matrix transforms definite numbers of qubits, so the dimensions are power of 2","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-02T02:39:57.683408Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:146f16e887f2967aa223e04da5b3ed84b639660de6e518071e46fbfb53da9319","observation_id":"a2e3c833-9b7b-441d-a4e8-5a8229493f97","resolution":{"observed_at":"2026-08-02T02:39:57.683408Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:39:57.910330Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-02T02:39:57.910330Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:b80839429d7342fa0e0e8da9a3365d9f83d3a605064bd053432b35dda83228e7","observation_id":"91b42c5c-fa8d-4400-9fdc-f15f5f9df7e9","resolution":{"observed_at":"2026-08-02T02:39:57.910330Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:39:58.066535Z","title":"blocks” associated to well-separated points and small “blocks","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-02T02:39:58.066535Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:76cac73023e221f86e83a32b8717e50f9f150429ed6b33daabd681e8ff051121","observation_id":"91694e7a-c7a8-4c6b-9fdb-0fe842e528ee","resolution":{"observed_at":"2026-08-02T02:39:58.066535Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:39:58.224717Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-02T02:39:58.224717Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:95892f02e0585af57740d9af4b5d3b99769a44ce16fab62c97dbc8a0ccbeb0c8","observation_id":"18b2f147-f3b8-4bf6-80fb-f5bb596fe58c","resolution":{"observed_at":"2026-08-02T02:39:58.224717Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:39:58.397383Z","title":"49 referenceadjacent(8 clusters)𝑙=4(27 clusters)𝑙=3(27 clusters)𝑙=2(7 clusters) FIG","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-02T02:39:58.397383Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:8a0e3ba7810af33a892f6ff92fee582ae63c0c4449b9b3d42aae34a3d4bc8922","observation_id":"966b1d39-2236-4ecc-a674-6aab7f895f2f","resolution":{"observed_at":"2026-08-02T02:39:58.397383Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:39:58.566349Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-02T02:39:58.566349Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:85f8705e4a6979ee1ce5e0324cdf361e07f4b3115cc22bab07fad0a5b1485d56","observation_id":"c7b86913-d671-4661-b67c-1e6e27947136","resolution":{"observed_at":"2026-08-02T02:39:58.566349Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:39:58.793577Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-02T02:39:58.793577Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:23601bccbb01694c214aab78eed4b04f915f0f7e009136dec99592ca28008c6b","observation_id":"3b5ac177-7a55-486d-b0e6-c717ee3927ec","resolution":{"observed_at":"2026-08-02T02:39:58.793577Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:39:58.940759Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-02T02:39:58.940759Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:af785eb366ae2d5567ca0e9ed41d9ac98d468d9b039556fdaa2faf9b5b9ce3e7","observation_id":"37371323-8ae3-4786-9369-09627c03be3d","resolution":{"observed_at":"2026-08-02T02:39:58.940759Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:39:59.180613Z","title":"clusters","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-02T02:39:59.180613Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:e59994e63d382ae8395be0cf04e3d66cba01391868ee5c3a183bf3253201e64d","observation_id":"3944e99c-63ff-405b-9e46-1bb6c61488ee","resolution":{"observed_at":"2026-08-02T02:39:59.180613Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:39:59.354231Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-02T02:39:59.354231Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:0eff93410a23e3c7dfc562dc7f23394bcff839b672a2260c9032efd28c3d2be6","observation_id":"f5214dd7-2215-435d-9321-37ac68f54dd0","resolution":{"observed_at":"2026-08-02T02:39:59.354231Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:39:59.561370Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-02T02:39:59.561370Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:8e5188edf6bfd87c4d1c1e296b405442fa264e754c8079d1dfc791bad77a430b","observation_id":"5440e46d-3bbf-41ce-925c-42d5897ad8c6","resolution":{"observed_at":"2026-08-02T02:39:59.561370Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:39:59.728506Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-02T02:39:59.728506Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:be6e15648f1d2e78496863e6ecf08b99d415e32834a5c357bc3cb89d03fc9501","observation_id":"bc38af62-0a4f-4c24-985f-6bebbf87547e","resolution":{"observed_at":"2026-08-02T02:39:59.728506Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:39:59.901664Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-02T02:39:59.901664Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:29d5d99fbe5719ad0110e24b3efc27ccbc4362851b8e5274595c568c083e091d","observation_id":"72fd186e-a502-450f-b084-bb1489a2d18a","resolution":{"observed_at":"2026-08-02T02:39:59.901664Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:40:00.126739Z","title":",2l −1, and all clusters are disjoint","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-02T02:40:00.126739Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:83b55d9ff51cfadd525af34d72db12217c94139af8f73077a42555c9c06edc16","observation_id":"8a9862c5-b6c8-4cca-9998-d9da86b7facf","resolution":{"observed_at":"2026-08-02T02:40:00.126739Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:40:00.301507Z","title":"internal","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-02T02:40:00.301507Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:181f63446ff7ad44ed591d66e13acb4cb114640c788ddc75a124cccbedb7a2b7","observation_id":"a32a81d1-0ef5-4244-8e6d-c096fb87ce57","resolution":{"observed_at":"2026-08-02T02:40:00.301507Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:40:00.474650Z","title":"To handle this neatly we give a theorem that is sufficiently flexible to accommodate all cases of interest here","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-02T02:40:00.474650Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:26d2f392bcd05116029590c5c80877ae2b9a9a302ccab2bcbaa1d52943b925bb","observation_id":"141b6919-4000-4008-8ec6-43e1c5e672fc","resolution":{"observed_at":"2026-08-02T02:40:00.474650Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:40:00.647085Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-02T02:40:00.647085Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:a67a9a0b1a39c9aa64caa65fe00ece64a29b2e71f9870eb0046ab2ad010a18de","observation_id":"0271b721-09ec-4a03-8d6e-8680e2091c8f","resolution":{"observed_at":"2026-08-02T02:40:00.647085Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:40:00.819393Z","title":"We explained how this can be obtained from a block-encodingU K of the real-space dataKdefined earlier, through controlled discrete Fourier transforms","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-02T02:40:00.819393Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:3fe880e0f3432dcdfc82e49fda74a7154d7626e33c65b095fef2dc08d1af7ece","observation_id":"7f3baa34-a42e-4da6-a30f-016fa114ec3c","resolution":{"observed_at":"2026-08-02T02:40:00.819393Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:40:00.906574Z","title":"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]","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-02T02:40:00.906574Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:057e05fb9656123395de2d85a7c466d6e46b691346cfc86efe5e0db126838eac","observation_id":"a7d39144-12b1-4e97-b417-75ce60abee09","resolution":{"observed_at":"2026-08-02T02:40:00.906574Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:40:00.909423Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-02T02:40:00.909423Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:26bad31cb7834657a7db37568d3e1d53c3390d93c49142856195cf34cbfbcbe0","observation_id":"44f8e56a-3930-4b7c-8348-5549e5464fba","resolution":{"observed_at":"2026-08-02T02:40:00.909423Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:40:00.984854Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-02T02:40:00.984854Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:a423233bf72494f774d97dc4429979d17eacb7343324530791af5e364cae3fec","observation_id":"575ec138-e0a2-4734-bc73-3eb28df6c138","resolution":{"observed_at":"2026-08-02T02:40:00.984854Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:40:01.095964Z","title":"Moreover, the initial data (8) satisfies (67) att= 0","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-02T02:40:01.095964Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:55d16965e8aef13b69517542e7e15d04d632fa2d3c9c98eb40f4aa0509f347ed","observation_id":"2caab783-2a64-45a6-b28a-a2fb8388ce42","resolution":{"observed_at":"2026-08-02T02:40:01.095964Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:40:01.260406Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-02T02:40:01.260406Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:2124325d9f574858bf8089e6f2b28dc2cc6f9bcee362d8b376dbebf1378b6451","observation_id":"5f1439ca-7fba-4c2e-91d5-a9b54e43ed9b","resolution":{"observed_at":"2026-08-02T02:40:01.260406Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:40:01.459165Z","title":"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)","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-02T02:40:01.459165Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:be0de37d35ba2e875630978eb36a24ddf199d1a64bf5fde6dead7ca0e85f03e9","observation_id":"b9aba1d2-10bb-454a-8299-fb82ce63f9c8","resolution":{"observed_at":"2026-08-02T02:40:01.459165Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:40:01.631045Z","title":"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","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-02T02:40:01.631045Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:550c8ba6cd2fde1948d8db66fcccdf853fec04a03d0a855aa266bfa9bf72241f","observation_id":"7a5704d7-9d09-48fb-9f68-e4bf6edbf679","resolution":{"observed_at":"2026-08-02T02:40:01.631045Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:40:01.797053Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-02T02:40:01.797053Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:114c8b0cc6798f21349ff902bcdfb92f9464ab30c45e357d98178ce3b3fdc45f","observation_id":"669f1232-2055-4f54-a34e-1ced982d0aa1","resolution":{"observed_at":"2026-08-02T02:40:01.797053Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T02:40:01.978372Z","title":"We must therefore construct a state preparation routine for the normalized state| ¯ℓK,k⟩","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-02T02:40:01.978372Z"},"links":{"citing_paper":"/paper/2607.14308"},"observation_digest":"sha256:db2f4802dec66bc10d8b1aec4378eb4fa7bcaad75525d2659993f0f2f301e5ce","observation_id":"8dfbb960-de95-4107-b1d0-c82a2019cda7","resolution":{"observed_at":"2026-08-02T02:40:01.978372Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2607.14308","last_updated":"2026-07-17T15:40:59Z","latest_version":2,"primary_category":"quant-ph","snapshot_observed_at":"2026-08-09T15:26:51.645684Z","submitted_at":"2026-07-15T19:14:21Z","title":"An end-to-end quantum algorithm for weakly nonlinear plasma physics with superquadratic speedup"},"reference_resolution":{"displayed":31,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":31,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":31},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"thesis":"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."}