{"as_of":"2026-08-11T22:04:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:2c0538f3c1bbf191e33760e33fe3dfad3dbf9cdfcfaccd5ef530357a730ee04c","coverage":[{"denominator":149,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":100,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-11T13:31:31.600923Z","state":"measured"},{"denominator":101,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":101,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-11T06:34:44.6726+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":"2026-07-11T18:50:30.278593Z","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":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.13150","snapshot_observed_at":"2026-07-11T18:50:30.278593Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.04481","last_updated":"2026-07-05T20:06:41Z","snapshot_observed_at":"2026-08-03T20:56:37.566883Z","submitted_at":"2026-07-05T20:06:41Z","title":"Implications of exclusive photon leptoproduction measurements for the proton charge-radius puzzle","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-07-11T18:50:30.278593Z"},"links":{"cited_paper":"/paper/2412.13150","citing_paper":"/paper/2607.04481"},"observation_digest":"sha256:63945a45eea6ed792f6f300d548f584df75cc579aca0e17fb65388cc3c03abdc","observation_id":"8bcaa687-227a-4922-82a7-39776493127c","resolution":{"observed_at":"2026-07-11T18:50:30.278593Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2412.13150/citation-record","integrity":"/paper/2412.13150/integrity","json":"/paper/2412.13150/citation-record.json","paper":"/paper/2412.13150"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:31:31.147994Z","title":"(2.4) The identities are a direct consequence of definitions (2.2) and (2.3), and they are obtained automatically when the parameterization is carried out using FT N(t)","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.147994Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:0c9a2c86c0f000a601ac0096015b7979c849ed0a297e91dabd3b9b575055e6f3","observation_id":"a4f6e1dd-8824-4d89-8a2b-993341573c1e","resolution":{"observed_at":"2026-08-11T13:31:31.147994Z","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":"2026-08-11T13:31:31.154065Z","title":"Taking into account additional suppression of amplitudes, generated by spin flip of quarks [8], QCR’s take the form of Eqs","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.154065Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:0e7ff3cc2019c0c4594009cad0df82ed4686f9a538e0015da6c4235dcce12b4d","observation_id":"a0811468-7521-4949-a631-8571146393e9","resolution":{"observed_at":"2026-08-11T13:31:31.154065Z","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":"2026-08-11T13:31:31.158998Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.158998Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:c9150c91ed35041317f853ccce2d0aae46c9243492abe0838335f660fd3c95d6","observation_id":"24c08713-6614-4739-927d-6fc45e72c134","resolution":{"observed_at":"2026-08-11T13:31:31.158998Z","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":"2026-08-11T13:31:31.163521Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.163521Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:83233588242444064caae00bcca957cf5dd3966ed881b1f822444f211d4dc480","observation_id":"3b0f104f-aa0e-4211-aa81-524feda15e7a","resolution":{"observed_at":"2026-08-11T13:31:31.163521Z","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":"2026-08-11T13:31:31.168770Z","title":"Form factors are functions with the established analytical properties","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.168770Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:f3c5254cbca3fcbd2324db5dc0c06d3ba94c0b079343a2034348572672fb7419","observation_id":"af964c39-3737-4b2e-af56-7ff0cd259726","resolution":{"observed_at":"2026-08-11T13:31:31.168770Z","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":"2026-08-11T13:31:31.173209Z","title":"bootstrap","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.173209Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:76bcd56bacc9b13ae1eedea2e983be3807a066d48995fd6ba8821bf873d38b16","observation_id":"1f4d1a3f-123f-461a-a810-a897190644bf","resolution":{"observed_at":"2026-08-11T13:31:31.173209Z","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":"2026-08-11T13:31:31.213063Z","title":null,"venue":null,"work_id":null,"year":1975},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.213063Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:e9b2774947b8e22a0f492b9f4542ed73e70c6ca7b609406410c779b34c87b0ee","observation_id":"c0e43e57-a249-4b05-bc75-05d2a9832a7b","resolution":{"observed_at":"2026-08-11T13:31:31.213063Z","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":"2026-08-11T13:31:31.184265Z","title":null,"venue":null,"work_id":null,"year":1959},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.184265Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:8237004b75cf484b230a7faf42287cb49a2c79f9dcc9fef11fd900391ed7610d","observation_id":"d4b52bb0-3d8e-4577-85f9-0ffcf6236f1e","resolution":{"observed_at":"2026-08-11T13:31:31.184265Z","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":"2026-08-11T13:31:31.188598Z","title":null,"venue":null,"work_id":null,"year":1960},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.188598Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:09347a8d314862dce1a56c2e63c5f1d19ac8d33d2a1fada60e90c2512bf7a3f3","observation_id":"c2415c88-7d87-4c48-b593-f87f7f9d3e4f","resolution":{"observed_at":"2026-08-11T13:31:31.188598Z","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":"2026-08-11T13:31:31.179471Z","title":"This group of data sets mostly includes the proton form factor mea- sured in the spacelike region","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.179471Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:21c7bd8c7fab0bddb6a813aa24030e726efc4e78ac215f65198656f3e3f6b8e4","observation_id":"4ff28887-a2ed-4e25-9176-3414782fe7e4","resolution":{"observed_at":"2026-08-11T13:31:31.179471Z","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":"2026-08-11T13:31:31.193150Z","title":null,"venue":null,"work_id":null,"year":1960},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.193150Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:37042814b8c10708a916e309a2934319306f8ec5d979e7e34cdd530d03d01f0b","observation_id":"ab6a68c9-07cf-49e4-bd6e-2593f772d336","resolution":{"observed_at":"2026-08-11T13:31:31.193150Z","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":"2026-08-11T13:31:31.197822Z","title":"Gounaris and J","venue":null,"work_id":null,"year":1968},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.197822Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:2f22a0eb7b5d480fffaeee18a59796899983a3a99be69adaa95ea7f23bb9187d","observation_id":"136b4716-4d82-4d1e-9120-6af6fa366b93","resolution":{"observed_at":"2026-08-11T13:31:31.197822Z","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":"2026-08-11T13:31:31.202840Z","title":null,"venue":null,"work_id":null,"year":1973},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.202840Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:32e4c1a20a3f6929853e9457911c4abf9ddd44318afce5db0f6586be28db0669","observation_id":"8a210667-f26a-4f98-b09a-a188677faf61","resolution":{"observed_at":"2026-08-11T13:31:31.202840Z","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":"2026-08-11T13:31:31.208881Z","title":null,"venue":null,"work_id":null,"year":1973},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.208881Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:7ac8ce99b2548d6e9f60c6e0181195b33dfaee4512b1f17fd50abc6e9cdfc78f","observation_id":"e4105856-6d6d-46ef-a17b-0d6c2e070454","resolution":{"observed_at":"2026-08-11T13:31:31.208881Z","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":"2026-08-11T13:31:31.217678Z","title":null,"venue":null,"work_id":null,"year":1978},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.217678Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:e368e63409a2babf1fab2d54401bd09c04e9075e42b112d4713b57a184c38c6c","observation_id":"e75ce1ec-7185-4dd2-86cc-b464e9077f18","resolution":{"observed_at":"2026-08-11T13:31:31.217678Z","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":"2026-08-11T13:31:31.221645Z","title":"Santini, M","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.221645Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:6d36345d4241e4b3d45dd1f8047afc94978d2d9e328aa57b48622de0118d58ef","observation_id":"6acc8fe0-388f-4443-97fc-431e42d4a3db","resolution":{"observed_at":"2026-08-11T13:31:31.221645Z","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":"2026-08-11T13:31:31.225831Z","title":null,"venue":null,"work_id":null,"year":1972},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.225831Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:cbe3ea63f88d1a112d320e16ec0d4ccfc76d407f61b8ec1d41cc41f0a52cd7d2","observation_id":"03332b7b-bda7-40e3-a82e-ffc10a62f227","resolution":{"observed_at":"2026-08-11T13:31:31.225831Z","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":"2026-08-11T13:31:31.230100Z","title":null,"venue":null,"work_id":null,"year":1977},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.230100Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:d8fcf042e379765e2f4318515d2bcd39f6308cc97f1bd9ffdeaf49e35e88b1b4","observation_id":"37777980-6142-440a-865d-3e18bb1e5067","resolution":{"observed_at":"2026-08-11T13:31:31.230100Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/9904024","last_updated":"1999-11-22T16:18:50Z","snapshot_observed_at":"2026-07-07T06:41:51.118586Z","submitted_at":"1999-04-10T17:28:35Z","title":"Dilepton Spectra from Decays of Light Unflavored Mesons","version":2},"cited_work":{"arxiv_id":"nucl-th/9904024","doi":null,"metadata_source":"pith","pith_arxiv_id":"nucl-th/9904024","snapshot_observed_at":"2026-08-11T13:31:33.590585Z","title":"Dilepton Spectra from Decays of Light Unflavored Mesons","venue":"nucl-th","work_id":"e87f7079-6fb9-4309-a668-2de1f0e04743","year":1999},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.233986Z"},"links":{"cited_paper":"/paper/nucl-th/9904024","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:7b43f9e24f41727df06c9c47f0ddaf6f483c020bd4712f7dc8e07e44ff4b5841","observation_id":"e07837b3-e40d-4a73-9057-2b4b8d8395a3","resolution":{"observed_at":"2026-08-11T13:31:33.595781Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/0010056","last_updated":"2003-02-14T16:55:56Z","snapshot_observed_at":"2026-07-07T06:29:54.419123Z","submitted_at":"2000-10-18T10:38:16Z","title":"Dilepton production in proton-proton collisions at BEVALAC energies","version":2},"cited_work":{"arxiv_id":"nucl-th/0010056","doi":null,"metadata_source":"pith","pith_arxiv_id":"nucl-th/0010056","snapshot_observed_at":"2026-08-11T13:31:33.573445Z","title":"Dilepton production in proton-proton collisions at BEVALAC energies","venue":"nucl-th","work_id":"0bd4e4a0-6b3d-413c-9b8a-1ad9a30e69c1","year":2000},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.238528Z"},"links":{"cited_paper":"/paper/nucl-th/0010056","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:adc39c77d923498400c59a75f5912d3a9c251e78468c874b4dbc81ba05774c43","observation_id":"aacd14a4-063a-484c-9971-896079c66c5b","resolution":{"observed_at":"2026-08-11T13:31:33.577996Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0910.5589","last_updated":"2009-10-29T09:22:17Z","snapshot_observed_at":"2026-07-06T01:58:46.665986Z","submitted_at":"2009-10-29T09:22:17Z","title":"Once more on electromagnetic form factors of nucleons in extended vector meson dominance model","version":1},"cited_work":{"arxiv_id":"0910.5589","doi":null,"metadata_source":"pith","pith_arxiv_id":"0910.5589","snapshot_observed_at":"2026-08-11T13:31:33.555512Z","title":"Once more on electromagnetic form factors of nucleons in extended vector meson dominance model","venue":"hep-ph","work_id":"43f29c2b-903f-46d9-8907-79acdea0f634","year":2009},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.242954Z"},"links":{"cited_paper":"/paper/0910.5589","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:abcb4cd18bf2dd0691db3c9c6faf3f957e2b06ab86c0aae840b71c060dafaa8d","observation_id":"0da24635-ed0d-4e2d-b880-0c8ce9f385f2","resolution":{"observed_at":"2026-08-11T13:31:33.560148Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/0110066","last_updated":"2001-11-14T10:45:05Z","snapshot_observed_at":"2026-07-07T06:31:02.520551Z","submitted_at":"2001-10-25T12:23:23Z","title":"Electromagnetic transition form factors and dilepton decay rates of nucleon resonances","version":2},"cited_work":{"arxiv_id":"nucl-th/0110066","doi":null,"metadata_source":"pith","pith_arxiv_id":"nucl-th/0110066","snapshot_observed_at":"2026-08-11T13:31:33.534304Z","title":"Electromagnetic transition form factors and dilepton decay rates of nucleon resonances","venue":"nucl-th","work_id":"581574ab-bc4c-4434-9580-1c3411ca6d02","year":2001},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.247332Z"},"links":{"cited_paper":"/paper/nucl-th/0110066","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:c4a8c0f27f0648ba67983277d241ae3e538b49c153767668fb6f48d6f8c5a56a","observation_id":"0357c2a1-ba7f-4f86-a0e8-6d1ce51f88b2","resolution":{"observed_at":"2026-08-11T13:31:33.539498Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2109.12961","last_updated":"2021-09-27T11:35:11Z","snapshot_observed_at":"2026-08-11T20:02:36.433207Z","submitted_at":"2021-09-27T11:35:11Z","title":"New insights into the nucleon's electromagnetic structure","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2109.12961","snapshot_observed_at":"2026-08-11T13:31:31.251794Z","title":"Lin, H.-W","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.251794Z"},"links":{"cited_paper":"/paper/2109.12961","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:c7eda88be1befa1e20be18bc5d438a64b058d0e6e80b6f8a4f947b8f0709c1f6","observation_id":"f8fdd019-83ec-470a-840a-d53242ec7ffe","resolution":{"observed_at":"2026-08-11T13:31:31.251794Z","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":"2026-08-11T13:31:31.255795Z","title":null,"venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.255795Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:d1e0d876eda673aae82c3d59d8df3b62f087379f80ce454217bf1e7dbef716a7","observation_id":"0a64ec62-d1da-4a20-9ae3-f3b3e674c616","resolution":{"observed_at":"2026-08-11T13:31:31.255795Z","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":"2026-08-11T13:31:31.259481Z","title":"Galster et al., Elastic electron–deuteron scattering and the electric neutron form factor at four-momentum transfers 5 fm−2 < q2 < 14 fm−2, Nucl","venue":null,"work_id":null,"year":1971},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.259481Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:2077e64c427d44dbd8cdf6e29f4287ed5f918d6674074e9a4cf9623d4791eacd","observation_id":"a2ed3edc-30c3-4147-ace7-08e3801aa532","resolution":{"observed_at":"2026-08-11T13:31:31.259481Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ex/0602017","last_updated":"2006-05-19T19:29:58Z","snapshot_observed_at":"2026-07-07T03:37:41.579992Z","submitted_at":"2006-02-07T20:11:04Z","title":"A new parameterization of the nucleon elastic form factors","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ex/0602017","snapshot_observed_at":"2026-08-11T13:31:31.263296Z","title":null,"venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.263296Z"},"links":{"cited_paper":"/paper/hep-ex/0602017","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:459f78a4cb7600a2b091fe5fdecbce08f3f409a574e6c3ffbce72ef6fd781305","observation_id":"06c7afcb-90d6-48d5-8fbb-685ba71397a5","resolution":{"observed_at":"2026-08-11T13:31:31.263296Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0708.1946","last_updated":"2007-11-22T00:54:35Z","snapshot_observed_at":"2026-07-06T01:29:46.696333Z","submitted_at":"2007-08-14T18:58:54Z","title":"Vector and Axial Nucleon Form Factors:A Duality Constrained Parameterization","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0708.1946","snapshot_observed_at":"2026-08-11T13:31:31.267910Z","title":"Bodek, S","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.267910Z"},"links":{"cited_paper":"/paper/0708.1946","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:56d039c073f98ff4d43e085fe97aa199babb3f61e2a71b13e623f4eb07945511","observation_id":"3476367a-f77f-41b6-a63d-de151316cbc5","resolution":{"observed_at":"2026-08-11T13:31:31.267910Z","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":"2026-08-11T13:31:31.272064Z","title":"Castellano et al., The reaction e+e−→ pp at a total energy of 2.1 GeV, Il Nuovo Cim","venue":null,"work_id":null,"year":1973},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.272064Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:608b327627339b7da964029f9a26931ae9e004aec30792fd5bb5bb7a34b1a2ac","observation_id":"4ac5ae2c-5c4a-4829-92b8-d2ad794b3130","resolution":{"observed_at":"2026-08-11T13:31:31.272064Z","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":"2026-08-11T13:31:31.276038Z","title":"Voci (on behalf of FENICE Collaboration), The first measurement of the neutron electromagnetic form fac- tors in the time-like region, Nucl","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.276038Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:bf53ecc478058402c8d1725392740e050f0be04ec8ca42d6b51e3eebac1d9826","observation_id":"0a235af5-ce3b-4f2a-b40d-c68a547ace02","resolution":{"observed_at":"2026-08-11T13:31:31.276038Z","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":"2026-08-11T13:31:31.279972Z","title":"Bassompierre (Mulhouse–Strasbourg–Turin Collabo- ration), First determination of the proton electromagne- tic form factors at the threshold of the time-like region, Phys","venue":null,"work_id":null,"year":1977},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.279972Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:a2f7a4e89a6e5239c0bc686c6d9c3013f131d1db92c21f56e0a14ad2a173d72c","observation_id":"4318f821-77c0-4578-afa2-764607b752ad","resolution":{"observed_at":"2026-08-11T13:31:31.279972Z","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":"2026-08-11T13:31:31.283876Z","title":"Conversi, T","venue":null,"work_id":null,"year":1965},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.283876Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:54e5bfe46b3704a422352a7d6e9b6dfef030e5d49778d5aa08023850e7d2d5d1","observation_id":"3e29f717-78ee-4601-bc11-6f00578b5534","resolution":{"observed_at":"2026-08-11T13:31:31.283876Z","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":"2026-08-11T13:31:31.287818Z","title":null,"venue":null,"work_id":null,"year":1969},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.287818Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:d2a9a2da8504611f2576d5911a519942d6a9b95981152dfa08197a36e462298c","observation_id":"049ed7e7-345d-448a-93fe-e47a7d8354ea","resolution":{"observed_at":"2026-08-11T13:31:31.287818Z","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":"2026-08-11T13:31:31.291861Z","title":"Bisello et al., A measurement of e+e−→ pp for (1975 ⩽ √s ⩽ 2250) MeV, Nucl","venue":null,"work_id":null,"year":1983},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.291861Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:cda4f3aa59e6c7e2bdb286747e69fb5a21a47177ef83e527dce9d87a05774b70","observation_id":"5aae849c-8ba9-42cb-9500-79fa2f37cf7c","resolution":{"observed_at":"2026-08-11T13:31:31.291861Z","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":"2026-08-11T13:31:31.296461Z","title":"Delcourt et al., Study of the reaction e+e− → pp in the total energy range 1925 − 2180 MeV, Phys","venue":null,"work_id":null,"year":1979},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.296461Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:26626fb88d0e6a3e91f13b7dc8aa4f2fcc9900bdc3cd1e168e52a51937ee50ca","observation_id":"48631678-53b3-4a60-857c-aa88763c7154","resolution":{"observed_at":"2026-08-11T13:31:31.296461Z","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":"2026-08-11T13:31:31.300581Z","title":"Antonelli et al., First measurement of the neu- tron electromagnetic form factor in the time-like region, Phys","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.300581Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:38af9e528aa4f91436dbd17073db163c02a92b4fc8e9774117c9a99cdfdf9a05","observation_id":"cd6cf986-0568-459f-9965-709ef2cebaa4","resolution":{"observed_at":"2026-08-11T13:31:31.300581Z","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":"2026-08-11T13:31:31.305221Z","title":"Antonelli et al., Measurement of the electromagnetic form factor of the proton in the time-like region, Phys","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.305221Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:4fac3c9fa4ba6d74312de60a2dd976e8d2911981f78a4af6347b6ce26f7c4b8e","observation_id":"a4b91457-d7ef-4cf1-9c6c-91f57570ff62","resolution":{"observed_at":"2026-08-11T13:31:31.305221Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1503.01452","last_updated":"2015-06-01T15:57:55Z","snapshot_observed_at":"2026-08-10T10:31:15.871853Z","submitted_at":"2015-03-04T20:43:20Z","title":"The Structure of the Nucleon: Elastic Electromagnetic Form Factors","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1503.01452","snapshot_observed_at":"2026-08-11T13:31:31.310270Z","title":"Punjabi et al., The structure of the nucleon: Elastic electromagnetic form factors, Eur","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.310270Z"},"links":{"cited_paper":"/paper/1503.01452","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:a518381598617e6a4b07cc103b9a83c284ca4925e685df9a16e6db16e2b38595","observation_id":"0be229a1-cd9a-46fc-bf43-b266b064780e","resolution":{"observed_at":"2026-08-11T13:31:31.310270Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1210.4689","last_updated":"2012-10-17T10:55:38Z","snapshot_observed_at":"2026-08-11T20:01:02.983504Z","submitted_at":"2012-10-17T10:55:38Z","title":"Nucleon Electromagnetic Form Factors in the Timelike Region","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1210.4689","snapshot_observed_at":"2026-08-11T13:31:31.315053Z","title":"Denig and G","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.315053Z"},"links":{"cited_paper":"/paper/1210.4689","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:554076d38384bba5b287f0e1f435769d6f6c02608cb5641a4b7d88f2bd8dace2","observation_id":"443247f3-02fc-49d2-9dc9-c796911b1e82","resolution":{"observed_at":"2026-08-11T13:31:31.315053Z","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":"2026-08-11T13:31:31.320188Z","title":"Pacetti, R","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.320188Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:3d5b3d0597b48d3ea3c31bdd9bd43032f7113a97463ccc29fa43a110bceaa811","observation_id":"b2aa9abb-1c97-4740-84da-155772c2d5b3","resolution":{"observed_at":"2026-08-11T13:31:31.320188Z","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":"2026-08-11T13:31:31.325680Z","title":null,"venue":null,"work_id":null,"year":1964},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.325680Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:9879923a7ff337de42416a8f22dd25542ec0a1a38b3014463872dcbbb16dbe20","observation_id":"47f35535-1cfe-4aa0-8a17-2463eb0a6525","resolution":{"observed_at":"2026-08-11T13:31:31.325680Z","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":"2026-08-11T13:31:31.330299Z","title":null,"venue":null,"work_id":null,"year":1989},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.330299Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:ba4445590fc64030ee2e3435946da4b924c4a97674f2d2ac5d1530baa5a85b94","observation_id":"ab9bfa20-b617-4032-b085-365611e8ca38","resolution":{"observed_at":"2026-08-11T13:31:31.330299Z","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":"2026-08-11T13:31:31.334592Z","title":"Ablikim et al.(BESIII Collaboration), Measurement of proton electromagnetic form factors in the time-like region using initial state radiation at BESIII, Phys","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.334592Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:e4c4ea7b0cd94a865411e233c9b9b0bb069f061241d81d5dcc5964718a235143","observation_id":"7410af00-e2cf-47b8-a309-5a05b431eb7f","resolution":{"observed_at":"2026-08-11T13:31:31.334592Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.05241","last_updated":"2023-09-11T05:26:17Z","snapshot_observed_at":"2026-08-11T20:01:47.859993Z","submitted_at":"2023-09-11T05:26:17Z","title":"Measurement of the neutron timelike electromagnetic form factor with the SND detector","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.05241","snapshot_observed_at":"2026-08-11T13:31:31.339108Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.339108Z"},"links":{"cited_paper":"/paper/2309.05241","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:3010618ea35d77aaf0e8e42dbdf3a511bec897041db1d9a2ac825854315115de","observation_id":"fbe2e6df-1989-4b52-a7ac-391a59ef7b22","resolution":{"observed_at":"2026-08-11T13:31:31.339108Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2206.13047","last_updated":"2022-06-27T05:17:36Z","snapshot_observed_at":"2026-08-11T20:02:44.916088Z","submitted_at":"2022-06-27T05:17:36Z","title":"Experimental study of the $e^+e^-\\to n\\bar n$ process at the VEPP-2000 $e^+e^-$ collider with the SND detector","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2206.13047","snapshot_observed_at":"2026-08-11T13:31:31.343987Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.343987Z"},"links":{"cited_paper":"/paper/2206.13047","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:ffd964a63371910608bbbeab2db8be0d54ee10bd0d80bc7485b1cffc3d817f9c","observation_id":"ee497652-164e-4cf6-87fe-6ad098233038","resolution":{"observed_at":"2026-08-11T13:31:31.343987Z","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":"2026-08-11T13:31:31.348400Z","title":null,"venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.348400Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:6e6495c3581c264fac58e1ff61b08f56c4d08b84f72482b4db478d01cf4d0a9f","observation_id":"d80fb439-045b-40ae-a27b-b211945cf177","resolution":{"observed_at":"2026-08-11T13:31:31.348400Z","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":"2026-08-11T13:31:31.352555Z","title":null,"venue":null,"work_id":null,"year":1969},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.352555Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:cc1ddea1646faa04a3a133cdbb0366e96c9c50cb83f33e6bad1908fc19a425fb","observation_id":"eaac9bcc-f2ff-4500-ab8f-2a6c43bd35cf","resolution":{"observed_at":"2026-08-11T13:31:31.352555Z","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":"2026-08-11T13:31:31.356805Z","title":"H¨ ohler,Pion–nucleon scattering (Springer, Landolt- B¨ ornstein, Switzerland, 1983)","venue":null,"work_id":null,"year":1983},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.356805Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:5cf263ab17c5b615c6701857efedc028d398e04abe24cb7d6a55ff63e39d2be2","observation_id":"c6b76d79-c9bb-4a26-8be3-2425975c0ded","resolution":{"observed_at":"2026-08-11T13:31:31.356805Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2106.06357","last_updated":"2021-06-11T12:56:12Z","snapshot_observed_at":"2026-08-11T20:02:20.449319Z","submitted_at":"2021-06-11T12:56:12Z","title":"Dispersion-theoretical analysis of the electromagnetic form factors of the nucleon: Past, present and future","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2106.06357","snapshot_observed_at":"2026-08-11T13:31:31.360622Z","title":"Lin, H.-W","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.360622Z"},"links":{"cited_paper":"/paper/2106.06357","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:b986eb5f1220436076fc6559479b21005f258bca9cede408cf4bb0257d9ce387","observation_id":"0959e3c9-2aff-42b4-9344-70cb6b600c7e","resolution":{"observed_at":"2026-08-11T13:31:31.360622Z","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":"2026-08-11T13:31:31.365151Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.365151Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:51f7e5641a8c30a15aae1b142e35191de0c43f3550e975fb8ec8ffc8617890a3","observation_id":"48226dfd-e05c-4fa5-86b3-021a08b9c5c1","resolution":{"observed_at":"2026-08-11T13:31:31.365151Z","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":"2026-08-11T13:31:31.369140Z","title":null,"venue":null,"work_id":null,"year":1972},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.369140Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:71d67c0463a44be088db0068f1a423dd8d8a32b04ab22990528dc355ad1bec41","observation_id":"28f6228b-a4c1-42f1-8598-7c6e31121fc2","resolution":{"observed_at":"2026-08-11T13:31:31.369140Z","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":"2026-08-11T13:31:31.373346Z","title":"H¨ ohleret al., Analysis of electromagnetic nucleon form factors, Nucl","venue":null,"work_id":null,"year":1976},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.373346Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:f499e2c8503f22ef076a7e25fe81968f048e91313a6a032d8bb132cba51a5093","observation_id":"914f90c0-b4c7-4ff1-ae21-5e8f222d7e7c","resolution":{"observed_at":"2026-08-11T13:31:31.373346Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0608337","last_updated":"2006-08-31T11:08:48Z","snapshot_observed_at":"2026-07-07T04:12:07.006377Z","submitted_at":"2006-08-31T11:08:48Z","title":"Dispersion analysis of the nucleon form factors including meson continua","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0608337","snapshot_observed_at":"2026-08-11T13:31:31.377528Z","title":null,"venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.377528Z"},"links":{"cited_paper":"/paper/hep-ph/0608337","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:fe9335dc65362248c24edff400c2fec3772e4df04bc335925bc16c7a530be458","observation_id":"9977d1ee-b87d-416f-8b65-bd1264a888d3","resolution":{"observed_at":"2026-08-11T13:31:31.377528Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2301.00976","last_updated":"2023-01-06T01:30:12Z","snapshot_observed_at":"2026-08-11T20:01:56.014323Z","submitted_at":"2023-01-03T07:13:46Z","title":"The $\\Sigma$ and $\\Xi$ electromagnetic form factors in the extended vector meson dominance model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2301.00976","snapshot_observed_at":"2026-08-11T13:31:31.381519Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.381519Z"},"links":{"cited_paper":"/paper/2301.00976","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:9a275eae20c1f2a955b2b481c1ec25d94543bfb83d41464fd96a128950e0d762","observation_id":"73ba5864-17d1-4e30-9b15-2b19422348f5","resolution":{"observed_at":"2026-08-11T13:31:31.381519Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1707.09063","last_updated":"2017-12-11T01:03:15Z","snapshot_observed_at":"2026-08-08T05:10:27.414805Z","submitted_at":"2017-07-27T22:31:54Z","title":"Proton and neutron electromagnetic form factors and uncertainties","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1707.09063","snapshot_observed_at":"2026-08-11T13:31:31.385308Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.385308Z"},"links":{"cited_paper":"/paper/1707.09063","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:8e580f4c98971f399c6f0db4d0a22a735f54b88730d4bb4ecca0c02cae8be045","observation_id":"7967972c-761a-40a1-8719-d3a3808f7cf5","resolution":{"observed_at":"2026-08-11T13:31:31.385308Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/0208022","last_updated":"2002-12-20T09:38:02Z","snapshot_observed_at":"2026-07-07T06:31:55.900836Z","submitted_at":"2002-08-13T12:55:26Z","title":"Off-shell omega production in proton-proton collisions near threshold","version":2},"cited_work":{"arxiv_id":"nucl-th/0208022","doi":null,"metadata_source":"pith","pith_arxiv_id":"nucl-th/0208022","snapshot_observed_at":"2026-08-11T13:31:33.182924Z","title":"Off-shell omega production in proton-proton collisions near threshold","venue":"nucl-th","work_id":"5e8e0440-ffcb-4143-8ef4-5769e25a00b5","year":2002},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.390148Z"},"links":{"cited_paper":"/paper/nucl-th/0208022","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:714e8b86d8c35f87b6d0c642ac79238841c2d644978ab9a726327d5475984655","observation_id":"15b3fcb9-9004-45ab-b01c-9e0062f85d81","resolution":{"observed_at":"2026-08-11T13:31:33.188302Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:31:31.394640Z","title":"Gell-Mann, D","venue":null,"work_id":null,"year":1962},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.394640Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:f692cdf818335b780c978f3cdec0925ab445bb666ada932c06b34b1420508ddc","observation_id":"98a82e06-040d-4b17-92ef-622b549545ea","resolution":{"observed_at":"2026-08-11T13:31:31.394640Z","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":"2026-08-11T13:31:31.398565Z","title":"Navas et al.(Particle Data Group), Review of particle physics, Phys","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.398565Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:c3e11fbca8865cfb6ecdbcd044dbcd51294a691deb51a6271faf7d2b1e0d1c6a","observation_id":"25521aa7-4170-49e0-a536-1c5ec6dcf654","resolution":{"observed_at":"2026-08-11T13:31:31.398565Z","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":"2026-08-11T13:31:31.402493Z","title":"Frenkiel et al., ωπ resonances and ππ s-wave struc- tures as observed in pp annihilations at rest, Nucl","venue":null,"work_id":null,"year":1972},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.402493Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:7f83e5367d53003669cebf680bb454184cbe994ad3359f80166625514f2f9df1","observation_id":"6799f864-8fe7-4a3d-8612-ccf3a2a147a7","resolution":{"observed_at":"2026-08-11T13:31:31.402493Z","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":"2026-08-11T13:31:31.407236Z","title":"Bartalucci et al., Experimental confirmation of the 1100 structure and first observation of the leptonic de- cay of the ρ′(1250), Nuovo Cim","venue":null,"work_id":null,"year":1979},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.407236Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:461bf87f66b24b1406a5c4bbc1fdd5cc80db1d2ae8ebad8b76091264da99a0c7","observation_id":"5cf146bb-a4c7-463f-8ecf-2dcef0777b44","resolution":{"observed_at":"2026-08-11T13:31:31.407236Z","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":"2026-08-11T13:31:31.411215Z","title":null,"venue":null,"work_id":null,"year":1980},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.411215Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:5117d5dea31aab0cb24010323c18351918e50bccaa2e64c6f323ad65cdae5453","observation_id":"9bd9e158-56ad-49e6-abc4-3d4a8f9f5810","resolution":{"observed_at":"2026-08-11T13:31:31.411215Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.06317","last_updated":"2020-09-14T10:32:05Z","snapshot_observed_at":"2026-08-11T20:02:18.063193Z","submitted_at":"2020-09-14T10:32:05Z","title":"Strong evidence of $\\rho(1250)$ from a unitary multichannel reanalysis of elastic scattering data with crossing-symmetry constraints","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2009.06317","snapshot_observed_at":"2026-08-11T13:31:31.415400Z","title":"Hammoud, R","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.415400Z"},"links":{"cited_paper":"/paper/2009.06317","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:59bd532edfcc75cc1d9d67d869d8c45828addba7b2864406bb571e2c50d0eda0","observation_id":"a8d46a75-320e-4e7c-9189-a54938622b43","resolution":{"observed_at":"2026-08-11T13:31:31.415400Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-ex/0401030","last_updated":"2004-05-26T03:54:18Z","snapshot_observed_at":"2026-07-07T06:24:42.977085Z","submitted_at":"2004-01-23T17:45:18Z","title":"Measurements of electron-proton elastic cross sections for $0.4 < Q^2 < 5.5 (GeV/c)^2$","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-ex/0401030","snapshot_observed_at":"2026-08-11T13:31:31.420174Z","title":null,"venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.420174Z"},"links":{"cited_paper":"/paper/nucl-ex/0401030","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:e2729265265c72d80f2441e55baeeec676093dd8676c8be471491203de67478b","observation_id":"8a339ec6-c923-499a-98de-0749fc2b84c2","resolution":{"observed_at":"2026-08-11T13:31:31.420174Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-ex/0410010","last_updated":"2004-10-08T18:26:14Z","snapshot_observed_at":"2026-07-07T06:25:06.427399Z","submitted_at":"2004-10-08T18:26:14Z","title":"Precision Rosenbluth measurement of the proton elastic form factors","version":1},"cited_work":{"arxiv_id":"nucl-ex/0410010","doi":null,"metadata_source":"pith","pith_arxiv_id":"nucl-ex/0410010","snapshot_observed_at":"2026-08-11T13:31:33.135787Z","title":"Precision Rosenbluth measurement of the proton elastic form factors","venue":"nucl-ex","work_id":"88ccd634-e103-4b90-ac57-95feeb9137cb","year":2004},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.425399Z"},"links":{"cited_paper":"/paper/nucl-ex/0410010","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:05d598b25a3fedbd5a37e8ae5db171e1130b2050f3af87ad6bce61fa5a6003e2","observation_id":"359ed4a0-1c8f-44a9-ae2f-397ece372514","resolution":{"observed_at":"2026-08-11T13:31:33.140865Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-ex/0308021","last_updated":"2004-02-02T23:58:47Z","snapshot_observed_at":"2026-07-07T06:24:37.137245Z","submitted_at":"2003-08-20T15:18:21Z","title":"Measurement of the Electric Form Factor of the Neutron at Q^2=0.5 and 1.0 (GeV/c)^2","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-ex/0308021","snapshot_observed_at":"2026-08-11T13:31:31.430086Z","title":"Warren et al.(Jefferson Lab E93-026 Collaboration), Measurement of the electric form factor of the neutron at Q2 = 0 .5 and 1 .0 GeV 2/c2, Phys","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.430086Z"},"links":{"cited_paper":"/paper/nucl-ex/0308021","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:fd08580070e4570108ba2141d933b4d3103d936685f50dcba7b4f90e71e050f4","observation_id":"2bd14d0b-0be0-4c56-9ff8-ffbc40a7827e","resolution":{"observed_at":"2026-08-11T13:31:31.430086Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-ex/0501018","last_updated":"2005-01-20T21:07:31Z","snapshot_observed_at":"2026-07-07T06:25:12.815075Z","submitted_at":"2005-01-20T21:07:31Z","title":"Proton elastic form factor ratios to $Q^2$ = 3.5 GeV$^2$ by polarization transfer","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-ex/0501018","snapshot_observed_at":"2026-08-11T13:31:31.434400Z","title":"Punjabi et al., Proton elastic form factor ratios to Q2 = 3.5 GeV 2 by polarization transfer, Phys","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.434400Z"},"links":{"cited_paper":"/paper/nucl-ex/0501018","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:175d97ad75fc239b1d6e486c63394183d0164705ce287d10e7a9b25e381b8635","observation_id":"3115fe6c-dc58-4f8b-a19d-70d99e14991a","resolution":{"observed_at":"2026-08-11T13:31:31.434400Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-ex/0601025","last_updated":"2006-05-19T16:39:02Z","snapshot_observed_at":"2026-07-07T06:25:42.359248Z","submitted_at":"2006-01-19T00:33:36Z","title":"Polarization transfer in the d(epol,e' ppol)n reaction up to Q^2=1.61 (GeV/c)^2","version":2},"cited_work":{"arxiv_id":"nucl-ex/0601025","doi":null,"metadata_source":"pith","pith_arxiv_id":"nucl-ex/0601025","snapshot_observed_at":"2026-08-11T13:31:33.085257Z","title":"Polarization transfer in the d(epol,e' ppol)n reaction up to Q^2=1.61 (GeV/c)^2","venue":"nucl-ex","work_id":"91e7f364-7583-443d-891c-c9546d6ef8ea","year":2006},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.438551Z"},"links":{"cited_paper":"/paper/nucl-ex/0601025","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:3ab7fdb7c45c4544d2fac47515e33bdbfaf4a39d8d62d016f3b8314dffa1f9f5","observation_id":"ecfe7331-4b62-4d57-b9a2-f7ca74be5150","resolution":{"observed_at":"2026-08-11T13:31:33.089666Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-ex/0606015","last_updated":"2006-09-08T18:55:04Z","snapshot_observed_at":"2026-08-10T22:31:31.062596Z","submitted_at":"2006-06-07T16:12:52Z","title":"Proton G_E/G_M from beam-target asymmetry","version":2},"cited_work":{"arxiv_id":"nucl-ex/0606015","doi":null,"metadata_source":"pith","pith_arxiv_id":"nucl-ex/0606015","snapshot_observed_at":"2026-08-11T13:31:33.065871Z","title":"Proton G_E/G_M from beam-target asymmetry","venue":"nucl-ex","work_id":"84771d94-30ce-4cc3-b093-f3d4566e01f3","year":2006},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.442819Z"},"links":{"cited_paper":"/paper/nucl-ex/0606015","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:15e88b639c5230d4b29d7cf86decb550a5ac7e331c51b3398e1e4d33cac6813c","observation_id":"e02927c5-5276-4761-81df-edd1aeba8ee0","resolution":{"observed_at":"2026-08-11T13:31:33.070213Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-ex/0308007","last_updated":"2003-08-08T00:33:58Z","snapshot_observed_at":"2026-07-07T06:24:37.137245Z","submitted_at":"2003-08-08T00:33:58Z","title":"Measurements of GEn/GMn from the ^2H(vec{e},e'vec{n})^1H Reaction to Q^2=1.45 (GeV/c)^2","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-ex/0308007","snapshot_observed_at":"2026-08-11T13:31:31.447600Z","title":"Madey et al","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.447600Z"},"links":{"cited_paper":"/paper/nucl-ex/0308007","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:b5419bcdfaefed843319535afcefea8c267f752e7b3d1c7c556ae8d36ecece04","observation_id":"841598e4-56c4-44b4-a554-6f57cede623e","resolution":{"observed_at":"2026-08-11T13:31:31.447600Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-ex/0511025","last_updated":"2005-11-13T02:25:05Z","snapshot_observed_at":"2026-07-07T06:25:36.493348Z","submitted_at":"2005-11-13T02:25:05Z","title":"Measurements of the neutron electric to magnetic form factor ratio GEn/GMn via the ^2H(\\vec{e},e'\\vec{n})^1H reaction to Q^2 = 1.45 (GeV/c)^2","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-ex/0511025","snapshot_observed_at":"2026-08-11T13:31:31.452065Z","title":"Plaster et al","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.452065Z"},"links":{"cited_paper":"/paper/nucl-ex/0511025","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:64ed909fdb48b3122703ed049acf548c3748883e1695bb43fdb5f6926de50624","observation_id":"ec0d0e1d-70af-4065-bea7-fc9ea94c9e33","resolution":{"observed_at":"2026-08-11T13:31:31.452065Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-ex/0605006","last_updated":"2006-11-20T21:53:21Z","snapshot_observed_at":"2026-07-07T06:25:54.609256Z","submitted_at":"2006-05-09T21:29:16Z","title":"Extraction of the Neutron Magnetic Form Factor from Quasi-Elastic 3He(pol)(e(pol),e') at Q^2 = 0.1 - 0.6 (GeV/c)^2","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-ex/0605006","snapshot_observed_at":"2026-08-11T13:31:31.459158Z","title":"Anderson et al","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.459158Z"},"links":{"cited_paper":"/paper/nucl-ex/0605006","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:fbf4d5708b81799a8e9777eaf633919d340ad4b509a5aca87b78bf87833eb6c3","observation_id":"e45bcbe4-b5da-4c7d-80b4-0a0e3b483879","resolution":{"observed_at":"2026-08-11T13:31:31.459158Z","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":"2026-08-11T13:31:31.464668Z","title":"MacLachlan et al., The ratio of proton electro- magnetic form factors via recoil polarimetry at Q2 = 1.13 (GeV/c)2, Nucl","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.464668Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:9ece7fb282576c5195ec58efa627632b956aa040000a3b9d61a8b8248f585733","observation_id":"aff43726-9e9d-4dcc-bc62-5dc581cd45e5","resolution":{"observed_at":"2026-08-11T13:31:31.464668Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1008.1738","last_updated":"2010-11-02T19:21:34Z","snapshot_observed_at":"2026-07-06T02:14:01.798204Z","submitted_at":"2010-08-10T15:33:23Z","title":"Measurements of the Electric Form Factor of the Neutron up to Q2=3.4 GeV2 using the Reaction He3(e,e'n)pp","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1008.1738","snapshot_observed_at":"2026-08-11T13:31:31.469228Z","title":"Riordan et al., Measurements of the electric form factor of the neutron up to Q2 = 3 .4 GeV2 using the reaction 3 ⃗He (⃗ e, e′n) pp, Phys","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.469228Z"},"links":{"cited_paper":"/paper/1008.1738","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:f1fc97743788371aed365d0219add3eb964b1a49a26d2ef6d68dd9555fb61e93","observation_id":"63065e2b-ad0b-4726-9a85-a171be874b53","resolution":{"observed_at":"2026-08-11T13:31:31.469228Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1012.0339","last_updated":"2011-02-28T19:59:33Z","snapshot_observed_at":"2026-07-06T02:20:03.344744Z","submitted_at":"2010-12-01T22:22:59Z","title":"Search for effects beyond the Born approximation in polarization transfer observables in $\\vec{e}p$ elastic scattering","version":2},"cited_work":{"arxiv_id":"1012.0339","doi":null,"metadata_source":"pith","pith_arxiv_id":"1012.0339","snapshot_observed_at":"2026-08-11T13:31:32.986679Z","title":"Search for effects beyond the Born approximation in polarization transfer observables in $\\vec{e}p$ elastic scattering","venue":"nucl-ex","work_id":"702ac14f-8d10-4503-b58d-bc283c8f376e","year":2010},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.473684Z"},"links":{"cited_paper":"/paper/1012.0339","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:8c3ac9c4362feffd08f5e7a14881005991d1d1e79c0b72101030b87d2aebdcdd","observation_id":"aaebfe28-c5bd-45f2-889f-e6653cd6c215","resolution":{"observed_at":"2026-08-11T13:31:32.991658Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1005.3419","last_updated":"2010-05-28T17:41:52Z","snapshot_observed_at":"2026-07-06T02:10:41.427013Z","submitted_at":"2010-05-19T12:14:24Z","title":"Recoil Polarization Measurements of the Proton Electromagnetic Form Factor Ratio to Q^2 = 8.5 GeV^2","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1005.3419","snapshot_observed_at":"2026-08-11T13:31:31.478312Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.478312Z"},"links":{"cited_paper":"/paper/1005.3419","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:0e5975f060569785f80c459d08470671c9cbb66cef14546643ff0b92b5bffbbe","observation_id":"f28def3f-91a3-4215-8180-0adccaf35249","resolution":{"observed_at":"2026-08-11T13:31:31.478312Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1002.2188","last_updated":"2010-08-23T14:41:32Z","snapshot_observed_at":"2026-07-06T02:03:42.854332Z","submitted_at":"2010-02-10T20:45:26Z","title":"Polarization Transfer in the 4He(e,e'p)3H Reaction at Q^2 = 0.8 and 1.3 (GeV/c)^2","version":8},"cited_work":{"arxiv_id":"1002.2188","doi":null,"metadata_source":"pith","pith_arxiv_id":"1002.2188","snapshot_observed_at":"2026-08-11T13:31:32.954201Z","title":"Polarization Transfer in the 4He(e,e'p)3H Reaction at Q^2 = 0.8 and 1.3 (GeV/c)^2","venue":"nucl-ex","work_id":"1e3d4b29-f821-4d95-b061-1a7d9b1cc3b8","year":2010},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.482479Z"},"links":{"cited_paper":"/paper/1002.2188","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:164f7a1eb3f6807b46e0c4bac876e80264e241ec34149d25b3c81f81071bd052","observation_id":"83702045-751d-46f6-84b0-ed3ec8e2d2c2","resolution":{"observed_at":"2026-08-11T13:31:32.958940Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1102.0318","last_updated":"2011-08-31T19:39:18Z","snapshot_observed_at":"2026-07-06T02:22:52.841674Z","submitted_at":"2011-02-01T23:09:16Z","title":"High Precision Measurement of the Proton Elastic Form Factor Ratio $\\mu_pG_E/G_M$ at low $Q^2$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1102.0318","snapshot_observed_at":"2026-08-11T13:31:31.487720Z","title":"Zhan et al., High precision measurement of the pro- ton elastic form factor ratio µpGE/GM at low Q2, Phys","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.487720Z"},"links":{"cited_paper":"/paper/1102.0318","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:0f1d3011679f7dca7812793c3fd0c51c56f12cae31a6b94129949ba05259673e","observation_id":"94824ae8-81c9-44c2-807f-78d219d04f12","resolution":{"observed_at":"2026-08-11T13:31:31.487720Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1103.5784","last_updated":"2011-08-30T21:03:52Z","snapshot_observed_at":"2026-08-03T14:58:05.424231Z","submitted_at":"2011-03-29T22:27:47Z","title":"Low Q^2 measurements of the proton form factor ratio $mu_p G_E / G_M$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1103.5784","snapshot_observed_at":"2026-08-11T13:31:31.492133Z","title":"Ron et al","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.492133Z"},"links":{"cited_paper":"/paper/1103.5784","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:d8b6f3615079fda7d03b05c55cb1b7f06439694a3ea680fec426da511fb4b004","observation_id":"11c47eef-81a5-4332-ab28-93133012a6da","resolution":{"observed_at":"2026-08-11T13:31:31.492133Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1707.08587","last_updated":"2018-08-10T18:07:21Z","snapshot_observed_at":"2026-08-07T14:46:02.789820Z","submitted_at":"2017-07-26T18:01:27Z","title":"Polarization Transfer Observables in Elastic Electron Proton Scattering at $Q^2 = $2.5, 5.2, 6.8, and 8.5 GeV$^2$","version":3},"cited_work":{"arxiv_id":"1707.08587","doi":null,"metadata_source":"pith","pith_arxiv_id":"1707.08587","snapshot_observed_at":"2026-08-11T13:31:32.906799Z","title":"Polarization Transfer Observables in Elastic Electron Proton Scattering at $Q^2 = $2.5, 5.2, 6.8, and 8.5 GeV$^2$","venue":"nucl-ex","work_id":"33ba38d7-4560-424d-836a-0a6eaa3dbc59","year":2017},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.496657Z"},"links":{"cited_paper":"/paper/1707.08587","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:9d2b8984c88d5e6334ce7fb1dc665a30160bfb6889b21f0962683422d47097de","observation_id":"05b71c2a-146e-42e9-86aa-4b47c1c9a821","resolution":{"observed_at":"2026-08-11T13:31:32.912029Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1704.06253","last_updated":"2017-11-28T11:45:32Z","snapshot_observed_at":"2026-08-11T20:02:33.804766Z","submitted_at":"2017-04-20T17:56:15Z","title":"Extraction of the Neutron Electric Form Factor from Measurements of Inclusive Double Spin Asymmetries","version":2},"cited_work":{"arxiv_id":"1704.06253","doi":null,"metadata_source":"pith","pith_arxiv_id":"1704.06253","snapshot_observed_at":"2026-08-11T13:31:32.887775Z","title":"Extraction of the Neutron Electric Form Factor from Measurements of Inclusive Double Spin Asymmetries","venue":"nucl-ex","work_id":"c6cddfb8-75c3-49a3-8725-bc3471cb5d0d","year":2017},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.501377Z"},"links":{"cited_paper":"/paper/1704.06253","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:46e3de525057cfe01bb7df796e65a91372d92edfbdd5babe735fbd14b093c08a","observation_id":"491ac16d-b1aa-464f-996c-fe192244b653","resolution":{"observed_at":"2026-08-11T13:31:32.892152Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1806.11156","last_updated":"2018-08-06T18:22:20Z","snapshot_observed_at":"2026-07-06T06:47:25.889567Z","submitted_at":"2018-06-28T19:39:46Z","title":"Proton Form Factor Ratio, $\\mu_p G_E^p/G_M^p$ from Double Spin Asymmetry","version":2},"cited_work":{"arxiv_id":"1806.11156","doi":null,"metadata_source":"pith","pith_arxiv_id":"1806.11156","snapshot_observed_at":"2026-08-11T13:31:32.869566Z","title":"Proton Form Factor Ratio, $\\mu_p G_E^p/G_M^p$ from Double Spin Asymmetry","venue":"nucl-ex","work_id":"83ae4aee-bdc3-439b-8593-70ef52d7080d","year":2018},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.506726Z"},"links":{"cited_paper":"/paper/1806.11156","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:86dd682b2662256275f63178ebb71066f7a6e937c77b09500612682a39f17506","observation_id":"091ac8bb-af21-4bbf-bd1e-a798651b5048","resolution":{"observed_at":"2026-08-11T13:31:32.873895Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2103.01842","last_updated":"2022-03-21T20:04:26Z","snapshot_observed_at":"2026-08-11T02:10:56.884466Z","submitted_at":"2021-03-02T16:26:17Z","title":"Form Factors and Two-Photon Exchange in High-Energy Elastic Electron-Proton Scattering","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2103.01842","snapshot_observed_at":"2026-08-11T13:31:31.511134Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.511134Z"},"links":{"cited_paper":"/paper/2103.01842","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:dc15f583e490ca9b8a11d2f654aefd408335199c39088b8dc400e53c09b754a2","observation_id":"ae77514a-0f25-4d9c-b181-d9eb15cd96f5","resolution":{"observed_at":"2026-08-11T13:31:31.511134Z","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":"ex/9910005","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:31:32.831056Z","title":null,"venue":null,"work_id":"2322354c-469f-4c04-a5f4-baa7eea93c3c","year":2000},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.516535Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:68afc34bd08d2615a277a184e9cefe63ba517dbbedf847b675c6a99c86a01021","observation_id":"24f7b80c-6dfe-41ea-87fa-2d8f002971b3","resolution":{"observed_at":"2026-08-11T13:31:32.839321Z","resolver_source":"raw_fallback","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:31:31.520812Z","title":"Janssens, R","venue":null,"work_id":null,"year":1966},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.520812Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:f8d8fec28dd999497917726678d365be68c5af35522e041c99bbcec6a6aeac62","observation_id":"a14d5e2a-1ba8-4668-bd36-1b1442735d05","resolution":{"observed_at":"2026-08-11T13:31:31.520812Z","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":"2026-08-11T13:31:31.527286Z","title":"Litt et al., Measurements of the ratio of the proton form factors, GE/GM at high momentum transfers and the question of scaling, Phys","venue":null,"work_id":null,"year":1970},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.527286Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:97ac39703ad7bb028a99c563f8016c869516ed8a9d8ca767bcef599773cc939c","observation_id":"63388b62-ebf3-497a-871e-ae10326f6746","resolution":{"observed_at":"2026-08-11T13:31:31.527286Z","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":"2026-08-11T13:31:31.531673Z","title":null,"venue":null,"work_id":null,"year":1989},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.531673Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:557c3ae45fdb567c33ee7e529603cb84596b26d754a760b000bb5a810e9783ea","observation_id":"27d32e56-0578-4960-969f-f3356c4a9409","resolution":{"observed_at":"2026-08-11T13:31:31.531673Z","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":"2026-08-11T13:31:31.536120Z","title":null,"venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.536120Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:da694fe4f13293727792ef6f9ee08683d0856e410cbacd14c50e996758f8a43c","observation_id":"f60c31ed-4a03-4e70-bf65-73b82cdadc06","resolution":{"observed_at":"2026-08-11T13:31:31.536120Z","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":"2026-08-11T13:31:31.540483Z","title":"Lung et al., Measurements of the electric and mag- netic form factors of the neutron from Q2 = 1 .75 to 4.00 (GeV/c)2, Phys","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.540483Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:2e96632ab832d2711b6001be1709d6bdcc505dcb7b1ec5c92127f02c108bb7c3","observation_id":"053f8b90-a4be-4382-861a-22c0491c4e34","resolution":{"observed_at":"2026-08-11T13:31:31.540483Z","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":"2026-08-11T13:31:31.544730Z","title":"Andivahis et al., Measurements of the electric and magnetic form factors of the proton from Q2 = 1.75 to 8.83 (GeV/c)2, Phys","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.544730Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:cb029818b33dcda7f15dd7eb3bbcf66bf5d779bec09d764ec0fe70492b7a1477","observation_id":"6ba6fe32-d58c-4273-a699-04a42484d846","resolution":{"observed_at":"2026-08-11T13:31:31.544730Z","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":"2026-08-11T13:31:31.550614Z","title":"Andreotti et al., Measurements of the magnetic form factor of the proton for timelike momentum transfers, Phys","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.550614Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:fd97289e4222c68d49ceb686722c4193f6eb24513be25f5c49898ff0a44d31e6","observation_id":"c2302b7b-e665-4209-b49a-e1f77f637968","resolution":{"observed_at":"2026-08-11T13:31:31.550614Z","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":"2026-08-11T13:31:31.555336Z","title":null,"venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.555336Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:e02b56de48a56e664f8a98ca3da7669f2e79eee1848efdc209eb64a8e4396c3d","observation_id":"5f054594-b9c1-4f1f-93a4-bab11bef42d8","resolution":{"observed_at":"2026-08-11T13:31:31.555336Z","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":"2026-08-11T13:31:31.559979Z","title":"Ambrogiani et al., Measurements of the magnetic form factor of the proton in the timelike region at large momentum transfer, Phys","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.559979Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:c006101b123d22f9f0f0da2f2a868ba25dc89555df2c9a6fe5939ece4e9f0611","observation_id":"02fc004b-8319-47dc-8ff2-f9e020d846b6","resolution":{"observed_at":"2026-08-11T13:31:31.559979Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1302.0055","last_updated":"2013-02-01T01:58:01Z","snapshot_observed_at":"2026-08-03T16:05:05.555340Z","submitted_at":"2013-02-01T01:58:01Z","title":"Study of e+e- --> p anti-p via initial-state radiation at BABAR","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1302.0055","snapshot_observed_at":"2026-08-11T13:31:31.564137Z","title":null,"venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.564137Z"},"links":{"cited_paper":"/paper/1302.0055","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:b322e0cb76f19eb2317bb5e2f1b7db55bb502df42b485a6bd190332a8c6ac851","observation_id":"92527731-e0f0-4f77-a353-2fad72775fe2","resolution":{"observed_at":"2026-08-11T13:31:31.564137Z","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":"2026-08-11T13:31:31.568327Z","title":"Eden et al., Electric form factor of the neutron from the 2H (⃗ e, e′⃗ n) 1H reaction at Q2 = 0 .255 (GeV/c)2, Phys","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.568327Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:4f6d89c70f041c8765324fa01a98346c485757d5459bc9bb9b6c93e340a69ad5","observation_id":"686d8222-42c3-49e7-9a4c-eaf6666edf91","resolution":{"observed_at":"2026-08-11T13:31:31.568327Z","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":"ex/9712006","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T13:31:32.737469Z","title":null,"venue":null,"work_id":"4f6b47b2-cab6-421d-90be-ff0f1f713846","year":1998},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.572210Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:3e06b2536f99dc18bc3021aa20c6af25081d6ec44b00d77afda6e4cc1de32514","observation_id":"80dced97-ab60-4ceb-a830-47ee6882ec95","resolution":{"observed_at":"2026-08-11T13:31:32.744722Z","resolver_source":"raw_fallback","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-ex/0609007","last_updated":"2006-09-07T22:34:29Z","snapshot_observed_at":"2026-07-07T06:26:01.316897Z","submitted_at":"2006-09-07T22:34:29Z","title":"Measurement of the proton electric to magnetic form factor ratio from \\vec ^1H(\\vec e, e'p)","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-ex/0609007","snapshot_observed_at":"2026-08-11T13:31:31.577222Z","title":null,"venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.577222Z"},"links":{"cited_paper":"/paper/nucl-ex/0609007","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:e28eb5f00117353068acbe3de1e6413044b5b8d817dc7563ad94683c9cc61ef0","observation_id":"ecb6ab52-83a1-4709-996f-dc91fa67e3ec","resolution":{"observed_at":"2026-08-11T13:31:31.577222Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0803.3827","last_updated":"2008-04-08T21:14:57Z","snapshot_observed_at":"2026-07-06T01:37:53.699832Z","submitted_at":"2008-03-26T21:33:28Z","title":"The Charge Form Factor of the Neutron at Low Momentum Transfer from the $^{2}\\vec{\\rm H}(\\vec{\\rm e},{\\rm e}'{\\rm n}){\\rm p}$ Reaction","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0803.3827","snapshot_observed_at":"2026-08-11T13:31:31.581775Z","title":"Geis et al.(BLAST Collaboration), Charge form fac- tor of the neutron at low momentum transfer from the 2 ⃗H (⃗ e, e′n) 1H reaction, Phys","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.581775Z"},"links":{"cited_paper":"/paper/0803.3827","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:f76b34f3b6fb60b834f233fa81b498b73c5617a79826240f06402976e226ec7a","observation_id":"763e5a0b-bbcc-48ca-bdc2-9c7286275e04","resolution":{"observed_at":"2026-08-11T13:31:31.581775Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ex/0510005","last_updated":"2005-12-23T14:09:14Z","snapshot_observed_at":"2026-07-07T03:37:26.654331Z","submitted_at":"2005-10-03T13:30:15Z","title":"Precision Measurements of the Timelike Electromagnetic Form Factors of Pion, Kaon, and Proton","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ex/0510005","snapshot_observed_at":"2026-08-11T13:31:31.586205Z","title":null,"venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.586205Z"},"links":{"cited_paper":"/paper/hep-ex/0510005","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:64b855b794d325c192b1369203c63d8b633e56e6f041685e3d2f37d89b9e1f98","observation_id":"61f32899-0695-4feb-8ad1-a4d55594d9fd","resolution":{"observed_at":"2026-08-11T13:31:31.586205Z","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":"2026-08-11T13:31:31.590339Z","title":"Anklin et al., Precision measurement of the neutron magnetic form factor, Phys","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.590339Z"},"links":{"citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:4042e797a62c2bf4ed0356ab33f57c17c0af63e9fbd1d468e2cbd9b289895ab1","observation_id":"ecc039c2-194b-4ccf-858b-6705d9762d3b","resolution":{"observed_at":"2026-08-11T13:31:31.590339Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-ex/9907012","last_updated":"1999-07-19T16:44:29Z","snapshot_observed_at":"2026-07-07T06:28:59.555865Z","submitted_at":"1999-07-19T16:44:29Z","title":"The Charge Form Factor of the Neutron from the Reaction \\pol{2H}(\\pol{e},e'n)p","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-ex/9907012","snapshot_observed_at":"2026-08-11T13:31:31.594690Z","title":"Passchier et al., Charge form factor of the neutron from the reaction 2 ⃗H (⃗ e, e′n) p, Phys","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.594690Z"},"links":{"cited_paper":"/paper/nucl-ex/9907012","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:938b632285c0347ae9bd0fb2d4831e415039256db4e92948b345769fcb203b55","observation_id":"f060d3c9-4e1f-46ec-acf1-e4b23f51ad74","resolution":{"observed_at":"2026-08-11T13:31:31.594690Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-ex/9908002","last_updated":"1999-08-09T08:03:02Z","snapshot_observed_at":"2026-07-07T06:28:59.555865Z","submitted_at":"1999-08-09T08:03:02Z","title":"The Charge Form Factor of the Neutron from the reaction 2H(pol)(e(pol)e'n)p","version":1},"cited_work":{"arxiv_id":"nucl-ex/9908002","doi":null,"metadata_source":"pith","pith_arxiv_id":"nucl-ex/9908002","snapshot_observed_at":"2026-08-11T13:31:32.594005Z","title":"The Charge Form Factor of the Neutron from the reaction 2H(pol)(e(pol)e'n)p","venue":"nucl-ex","work_id":"30c85f39-0656-4c05-b722-c679caaa0067","year":1999},"citing_paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model","version":2},"reference_index":100,"source":"pdf_text","source_observed_at":"2026-08-11T13:31:31.600923Z"},"links":{"cited_paper":"/paper/nucl-ex/9908002","citing_paper":"/paper/2412.13150"},"observation_digest":"sha256:ced9475711dce552e5b45169da081bd58d609d1911374b12df2ca6f2aa9c337c","observation_id":"bcb649db-8695-464a-ab98-f480e7c9e236","resolution":{"observed_at":"2026-08-11T13:31:32.598943Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-11T06:34:44.6726+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"2412.13150","last_updated":"2025-01-19T13:38:56Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-11T20:00:24.350228Z","submitted_at":"2024-12-17T18:20:31Z","title":"Electromagnetic nucleon form factors in the extended vector meson dominance model"},"reference_resolution":{"displayed":100,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":84,"verified_exact":16,"verified_fuzzy":0},"total_outbound_references":149},"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":"2026-08-11T06:34:44.6726+00:00","source":"crossref"},{"observed_at":"2026-08-11T06:34:36.301508+00:00","source":"retraction_watch"}],"thesis":"As of 11 August 2026, this Paper Citation Record lists 100 of 149 outbound references and 1 inbound Pith citation observation for arXiv:2412.13150."}