{"as_of":"2026-08-18T15:39:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:d0da7176c09d138f305f73f3499df9ebca37ed3048bd3b5c419b8a456cb6939e","coverage":[{"denominator":35,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":35,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-03T00:19:17.051549Z","state":"measured"},{"denominator":40,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":40,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-18T06:34:40.430872+00:00","state":"measured"},{"denominator":5,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":5,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-03T10:58:56.199625Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-07-01T13:55:46.068948Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2602.11263","snapshot_observed_at":"2026-08-03T10:58:56.199625Z","title":null,"venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2601.08567","last_updated":"2026-07-03T12:04:07Z","snapshot_observed_at":"2026-08-13T17:31:09.756527Z","submitted_at":"2026-01-13T13:51:40Z","title":"Where to find $X(17)$?","version":5},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-03T10:58:56.199625Z"},"links":{"cited_paper":"/paper/2602.11263","citing_paper":"/paper/2601.08567"},"observation_digest":"sha256:6fb8e35c909567d3c06cf3affb2dfcbb04f1c6e224e490a933be11842210d095","observation_id":"48957735-05fa-4c2c-85c5-7fd41a57e0a8","resolution":{"observed_at":"2026-08-03T10:58:56.199625Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"cited_work":{"arxiv_id":"2602.11263","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2602.11263","snapshot_observed_at":"2026-07-17T01:20:44.793893Z","title":"The X17 with Chiral Couplings","venue":null,"work_id":"b13b65b5-91f7-477c-ae2f-0851c24c3ac8","year":2026},"citing_paper":{"arxiv_id":"2604.22278","last_updated":"2026-07-28T10:08:14Z","snapshot_observed_at":"2026-08-16T05:27:56.118876Z","submitted_at":"2026-04-24T06:45:43Z","title":"Flavor specific chiral $U(1)_X$ framework for explaining the ATOMKI anomaly","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-05-08T11:15:23.262005Z"},"links":{"cited_paper":"/paper/2602.11263","citing_paper":"/paper/2604.22278"},"observation_digest":"sha256:6861dd7724b8dd27c69c5c9548438d9bbeb4bc3b20e9c2830eadc3222f519a59","observation_id":"14bdcadb-03d4-4e2d-862b-d7f15ee35bc5","resolution":{"observed_at":"2026-07-17T01:20:44.793893Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2602.11263","snapshot_observed_at":"2026-08-02T15:45:11.267922Z","title":"The X17 with Chiral Couplings,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2604.22278","last_updated":"2026-07-28T10:08:14Z","snapshot_observed_at":"2026-08-16T05:27:56.118876Z","submitted_at":"2026-04-24T06:45:43Z","title":"Flavor specific chiral $U(1)_X$ framework for explaining the ATOMKI anomaly","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-02T15:45:11.267922Z"},"links":{"cited_paper":"/paper/2602.11263","citing_paper":"/paper/2604.22278"},"observation_digest":"sha256:47aacebe9e15356252765172fb454ee0af85dc15145ef1b2b4a5975e885336c1","observation_id":"17cf483c-c4ef-49d8-9073-3cc3689944fd","resolution":{"observed_at":"2026-08-02T15:45:11.267922Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"cited_work":{"arxiv_id":"2602.11263","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2602.11263","snapshot_observed_at":"2026-07-17T01:20:44.793893Z","title":"The X17 with Chiral Couplings","venue":null,"work_id":"b13b65b5-91f7-477c-ae2f-0851c24c3ac8","year":2026},"citing_paper":{"arxiv_id":"2605.10689","last_updated":"2026-05-27T16:18:49Z","snapshot_observed_at":"2026-08-14T06:04:05.163981Z","submitted_at":"2026-05-11T15:02:49Z","title":"The X17 Existence Hinted at by Nuclear Reactor Neutrinos","version":2},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-06-30T22:31:24.528489Z"},"links":{"cited_paper":"/paper/2602.11263","citing_paper":"/paper/2605.10689"},"observation_digest":"sha256:ebd8d045db90b7d307e2e764602f2b3166aaf9c0fa548722bc17308801fc1613","observation_id":"56961b41-1578-4571-b26f-29cc2d9de201","resolution":{"observed_at":"2026-07-17T01:20:44.793893Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"cited_work":{"arxiv_id":"2602.11263","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2602.11263","snapshot_observed_at":"2026-07-17T01:20:44.793893Z","title":"The X17 with Chiral Couplings","venue":null,"work_id":"b13b65b5-91f7-477c-ae2f-0851c24c3ac8","year":2026},"citing_paper":{"arxiv_id":"2605.27513","last_updated":"2026-05-26T18:00:04Z","snapshot_observed_at":"2026-08-13T08:27:19.166756Z","submitted_at":"2026-05-26T18:00:04Z","title":"Constraints on a Light Leptophilic Scalar from Dark-Sector Couplings","version":1},"reference_index":102,"source":"pdf_text","source_observed_at":"2026-06-29T16:46:41.892216Z"},"links":{"cited_paper":"/paper/2602.11263","citing_paper":"/paper/2605.27513"},"observation_digest":"sha256:980751530b3e0edfc73de48d84ce7a987f9d8c99625c473ef0484b0176e5c187","observation_id":"f8e5460c-b8a3-4a1b-98bb-4aad000d5885","resolution":{"observed_at":"2026-07-17T01:20:44.793893Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2602.11263/citation-record","integrity":"/paper/2602.11263/integrity","json":"/paper/2602.11263/citation-record.json","paper":"/paper/2602.11263"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-03T00:19:12.876755Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:12.876755Z"},"links":{"citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:afc38fa1881a31e4a280ac19a252ffc7788097dc7e99089e9c1483ce96110a20","observation_id":"aacaa0c4-5379-47e7-9480-1790f4a5ccb6","resolution":{"observed_at":"2026-08-03T00:19:12.876755Z","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":"2026-08-03T00:19:13.056035Z","title":"A parity even 4He(20.21) state withJ P = 0 + and a parity odd 4He(21.01) withJ P = 0 −","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:13.056035Z"},"links":{"citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:9ab29f3204bf975ca32c139e31fcc69f9b6517949dd94bd103fa7e6501a19fe3","observation_id":"187665eb-8ea7-4497-9e63-f64de0cd2a15","resolution":{"observed_at":"2026-08-03T00:19:13.056035Z","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":"2026-08-03T00:19:13.200767Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:13.200767Z"},"links":{"citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:30fbd65dc7c38673e32f49820117fc077503edbbe7ebe04e98007546a7df185c","observation_id":"e947caa2-6310-4119-b0cc-27ae48fb8f65","resolution":{"observed_at":"2026-08-03T00:19:13.200767Z","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":"2026-08-03T00:19:13.301796Z","title":"The am- plitude for the decay of the excited state then reads M=M V +MA =C Be V Λ−1ϵµναβ p∗ µϵ∗ νpαϵX β +C Be A Λϵ∗ µϵX µ","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:13.301796Z"},"links":{"citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:78d6febc64264336c11ce4762363c58b7a3d8992bfe0e338568a6f1b28892e88","observation_id":"bd150d43-18b9-4491-a8af-70a9e2a2c149","resolution":{"observed_at":"2026-08-03T00:19:13.301796Z","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":"2026-08-03T00:19:13.454455Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:13.454455Z"},"links":{"citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:95d7e1c2ea2995517bb4c2bd075cedee43713841a89f360c1286075cb27e2b72","observation_id":"ec2a76d3-46d8-4987-acd0-f8b7c51a4968","resolution":{"observed_at":"2026-08-03T00:19:13.454455Z","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":"2026-08-03T00:19:13.574999Z","title":"Due to the isospin mixing and breaking of the phys- ical excited nuclear state of beryllium, care must be taken when matching the nucleus EFT to the nucleon EFT","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:13.574999Z"},"links":{"citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:00c3d52ab657ee1422e6251d1bfa4dde079277c2a11c1303069802d2405e007f","observation_id":"995a2c40-4512-448e-af2a-95d0db058004","resolution":{"observed_at":"2026-08-03T00:19:13.574999Z","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":"2026-08-03T00:19:13.694893Z","title":"The experiment was run at an intermediate energy, such that both excited states would be produced","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:13.694893Z"},"links":{"citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:c9a9762890aecb3c3921af361e49832a47903741a3e044b09d81cc9275c842a9","observation_id":"0bca6fc7-7620-40ef-8280-28762dcb1f1f","resolution":{"observed_at":"2026-08-03T00:19:13.694893Z","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":"2026-08-03T00:19:13.823566Z","title":"The leading operator for anXwith (axial-)vector transition is of dimension (5) 3","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:13.823566Z"},"links":{"citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:1f3624a1d2023777abf454e48800dcb4f7bda9718b77dca932b0e639d7b398c1","observation_id":"820e53a7-7a32-4b78-a138-935159c3ca5f","resolution":{"observed_at":"2026-08-03T00:19:13.823566Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1504.01527","last_updated":"2015-04-07T09:24:21Z","snapshot_observed_at":"2026-08-14T22:53:26.124777Z","submitted_at":"2015-04-07T09:24:21Z","title":"Observation of Anomalous Internal Pair Creation in $^8$Be: A Possible Signature of a Light, Neutral Boson","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1504.01527","snapshot_observed_at":"2026-08-03T00:19:13.966605Z","title":"Observation of Anomalous Internal Pair Creation in Be8 : A Possible Indication of a Light, Neutral Boson,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:13.966605Z"},"links":{"cited_paper":"/paper/1504.01527","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:15fce416100a74d704c683bca971ad20b88956d49c654372d1302cb73121cb9a","observation_id":"6dbbbc82-e13e-4ed9-812d-21e2f7be1fc2","resolution":{"observed_at":"2026-08-03T00:19:13.966605Z","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":"2026-08-03T00:19:14.109812Z","title":"New results on the Be-8 anomaly,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:14.109812Z"},"links":{"citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:e44ba67974575bd67faecf718dc4caf488ca63026b4c1de88c320283d2e10551","observation_id":"cf1335ef-864d-4810-8f0c-fe266839591f","resolution":{"observed_at":"2026-08-03T00:19:14.109812Z","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":"2026-08-03T00:19:14.228857Z","title":"New results on the 8Be anomaly,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:14.228857Z"},"links":{"citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:cb1e180c32a1881513af57f317a5c45f7bb2e118f4068c29cd277c5f6bb16b65","observation_id":"52918fcd-4c8b-4466-acad-26f7c0bf1835","resolution":{"observed_at":"2026-08-03T00:19:14.228857Z","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":"2026-08-03T00:19:14.324874Z","title":"On the creation of the 17 MeV X boson in the 17.6 MeV M1 transition of 8Be,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:14.324874Z"},"links":{"citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:6837c699cd646bdb0562dc214290bc125df8436a2f725405f1b83a0d9e5e48e7","observation_id":"ab8aec8d-369f-4ff1-b528-742abe44e45a","resolution":{"observed_at":"2026-08-03T00:19:14.324874Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2209.10795","last_updated":"2022-11-01T15:20:20Z","snapshot_observed_at":"2026-08-16T16:30:43.320089Z","submitted_at":"2022-09-22T05:44:27Z","title":"New anomaly observed in $^{12}$C supports the existence and the vector character of the hypothetical X17 boson","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2209.10795","snapshot_observed_at":"2026-08-03T00:19:14.466803Z","title":"New anomaly observed in C12 supports the existence and the vector character of the hypothetical X17 boson,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:14.466803Z"},"links":{"cited_paper":"/paper/2209.10795","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:3dc9d430be9014bf624313ccabb147dd6f687c64b206262afe40506cb117237f","observation_id":"1f1e376d-c5b8-4610-af88-0d0b7ba4ef9c","resolution":{"observed_at":"2026-08-03T00:19:14.466803Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.10459","last_updated":"2019-10-23T11:06:55Z","snapshot_observed_at":"2026-08-16T12:24:03.253422Z","submitted_at":"2019-10-23T11:06:55Z","title":"New evidence supporting the existence of the hypothetic X17 particle","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.10459","snapshot_observed_at":"2026-08-03T00:19:14.593242Z","title":"New evidence supporting the existence of the hypothetic X17 particle,","venue":null,"work_id":null,"year":1910},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:14.593242Z"},"links":{"cited_paper":"/paper/1910.10459","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:7b435c28fc0af4e448325c3d50927071c662a1f79966756cc242c57a93da0da6","observation_id":"25d6a6ad-9ce8-4770-9928-d82b8447f8f0","resolution":{"observed_at":"2026-08-03T00:19:14.593242Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.11676","last_updated":"2024-03-19T11:09:00Z","snapshot_observed_at":"2026-08-17T03:01:49.229824Z","submitted_at":"2024-01-22T03:32:56Z","title":"Checking the $^8$Be anomaly with a two-arm electron positron pair spectrometer","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.11676","snapshot_observed_at":"2026-08-03T00:19:14.727745Z","title":"Checking the 8Be Anomaly with a Two-Arm Electron Positron Pair Spectrometer,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:14.727745Z"},"links":{"cited_paper":"/paper/2401.11676","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:29c7b3faa146ca47f49f25f4baa3ecfabe5b75d1df8294f6150783c12a57b9a5","observation_id":"8f28f277-73b8-4bff-9712-2904177790a6","resolution":{"observed_at":"2026-08-03T00:19:14.727745Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2504.11439","last_updated":"2026-04-14T11:24:42Z","snapshot_observed_at":"2026-08-14T11:36:51.419976Z","submitted_at":"2025-04-15T17:53:40Z","title":"Combined Evidence for the $X_{17}$ Boson After PADME Results on Resonant Production in Positron Annihilation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2504.11439","snapshot_observed_at":"2026-08-03T00:19:14.875795Z","title":"Combined Evidence for theX 17 Boson After PADME Results on Resonant Production in Positron Annihilation,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:14.875795Z"},"links":{"cited_paper":"/paper/2504.11439","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:6e25d679275b5d20a08e5bcaea73f2913bc410b49453ebc50e5a6116b812cb0d","observation_id":"32b10473-207c-434f-8168-d36c8cced56a","resolution":{"observed_at":"2026-08-03T00:19:14.875795Z","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":"2026-08-03T00:19:15.007448Z","title":"Hunting the elusiveX17 in CEνNS at the ESS,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:15.007448Z"},"links":{"citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:44ee2a805f96f81cd4a3c00c8a0413a6144daa02a9d40605dfe9049492586b97","observation_id":"7b4e0cb0-5ac4-4a1c-a1a4-97194dcc58a9","resolution":{"observed_at":"2026-08-03T00:19:15.007448Z","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":"2026-08-03T00:19:15.153717Z","title":"Search for a new 17 MeV resonance via e+e− annihilation with the PADME Experiment,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:15.153717Z"},"links":{"citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:cd2f8c87454473ec32d1ecae4ebf775131008e22b69868fb19bc4ee719c4574c","observation_id":"f26960b0-7e0b-4d30-ba61-15cf78606a74","resolution":{"observed_at":"2026-08-03T00:19:15.153717Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1604.07411","last_updated":"2016-08-15T06:16:03Z","snapshot_observed_at":"2026-08-16T10:16:49.301988Z","submitted_at":"2016-04-25T20:00:03Z","title":"Protophobic Fifth Force Interpretation of the Observed Anomaly in $^8$Be Nuclear Transitions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1604.07411","snapshot_observed_at":"2026-08-03T00:19:15.282584Z","title":"Protophobic Fifth-Force Interpretation of the Observed Anomaly in 8Be Nuclear Transitions,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:15.282584Z"},"links":{"cited_paper":"/paper/1604.07411","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:f58b9bfa9f195293fef69e75f3732d843c14205a0a9830436fd16278a52fe0d4","observation_id":"cea9531a-dda2-40b5-845d-20b2c3e715c8","resolution":{"observed_at":"2026-08-03T00:19:15.282584Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1612.01525","last_updated":"2017-07-05T17:11:58Z","snapshot_observed_at":"2026-08-16T02:13:49.564813Z","submitted_at":"2016-12-05T21:00:00Z","title":"Light Axial Vectors, Nuclear Transitions, and the $^8$Be Anomaly","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1612.01525","snapshot_observed_at":"2026-08-03T00:19:15.367335Z","title":"Light axial vector bosons, nuclear transitions, and the 8Be anomaly,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:15.367335Z"},"links":{"cited_paper":"/paper/1612.01525","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:e2ce1d6daf8352b05840642c31ebfb0c5228847dfcb52e7e6942305bb4b8f996","observation_id":"dcab68b9-f2d9-4eaa-871c-f1d9b1916488","resolution":{"observed_at":"2026-08-03T00:19:15.367335Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1608.03591","last_updated":"2017-01-18T19:17:49Z","snapshot_observed_at":"2026-08-16T02:13:46.860734Z","submitted_at":"2016-08-11T20:00:01Z","title":"Particle Physics Models for the 17 MeV Anomaly in Beryllium Nuclear Decays","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1608.03591","snapshot_observed_at":"2026-08-03T00:19:15.445280Z","title":"Particle physics models for the 17 MeV anomaly in beryllium nuclear decays,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:15.445280Z"},"links":{"cited_paper":"/paper/1608.03591","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:a7903e574e8894c77907ee00e258cdbb56231c127a171896cc4c2a233f348d0d","observation_id":"96b91b43-8cfb-4c11-a988-b1d42faa165c","resolution":{"observed_at":"2026-08-03T00:19:15.445280Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2006.01151","last_updated":"2020-08-18T16:50:04Z","snapshot_observed_at":"2026-08-14T20:04:17.206619Z","submitted_at":"2020-06-01T18:00:03Z","title":"Dynamical Evidence For a Fifth Force Explanation of the ATOMKI Nuclear Anomalies","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.01151","snapshot_observed_at":"2026-08-03T00:19:15.526422Z","title":"Dynamical Evidence For a Fifth Force Explanation of the ATOMKI Nuclear Anomalies,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:15.526422Z"},"links":{"cited_paper":"/paper/2006.01151","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:d454615177ba7933826f8c06c0efff91ac895c23459f336f7beda7ea9cf19e43","observation_id":"b1d1702e-99cc-4c39-a9af-0f6867d3f765","resolution":{"observed_at":"2026-08-03T00:19:15.526422Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.06453","last_updated":"2023-08-16T09:06:06Z","snapshot_observed_at":"2026-08-16T16:09:04.045868Z","submitted_at":"2022-12-13T09:48:16Z","title":"An updated view on the ATOMKI nuclear anomalies","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.06453","snapshot_observed_at":"2026-08-03T00:19:15.585329Z","title":"An updated view on the ATOMKI nuclear anomalies,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:15.585329Z"},"links":{"cited_paper":"/paper/2212.06453","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:ebebeac3e2a99708f38afe12869b53772d4e61a95049fc87c44b1bf4442b6a50","observation_id":"cefdd267-87d1-4c8e-9924-ee89182d6b0c","resolution":{"observed_at":"2026-08-03T00:19:15.585329Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2406.08143","last_updated":"2024-06-12T12:34:44Z","snapshot_observed_at":"2026-08-16T13:43:47.189186Z","submitted_at":"2024-06-12T12:34:44Z","title":"Constraining the axial-vector X17 interpretation with ${}^{12}$C data","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.08143","snapshot_observed_at":"2026-08-03T00:19:15.652451Z","title":"Constraining the axial-vector X17 interpretation with 12C data,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:15.652451Z"},"links":{"cited_paper":"/paper/2406.08143","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:4778a873aad3553a1ea0f9296ff62d3eb18e7e69cb7ed4e63f1f735a6caa9a04","observation_id":"850491a4-8c64-4212-a974-8aad9e1e9ba1","resolution":{"observed_at":"2026-08-03T00:19:15.652451Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1609.09072","last_updated":"2016-10-21T17:56:54Z","snapshot_observed_at":"2026-08-14T21:37:40.515445Z","submitted_at":"2016-09-28T20:00:01Z","title":"Light Weakly Coupled Axial Forces: Models, Constraints, and Projections","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1609.09072","snapshot_observed_at":"2026-08-03T00:19:15.733446Z","title":"Light Weakly Coupled Axial Forces: Models, Constraints, and Projections,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:15.733446Z"},"links":{"cited_paper":"/paper/1609.09072","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:f34c69881c2dc66b24817b1afcc5ce6c0ae5a9016ca3f433631162ba305d936a","observation_id":"160765ad-9a36-48f9-a5d3-646ee141dc66","resolution":{"observed_at":"2026-08-03T00:19:15.733446Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.15077","last_updated":"2023-09-11T16:18:56Z","snapshot_observed_at":"2026-08-16T15:20:56.188464Z","submitted_at":"2023-06-26T21:25:16Z","title":"Pion decay constraints on exotic 17 MeV vector bosons","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.15077","snapshot_observed_at":"2026-08-03T00:19:15.875940Z","title":"Pion decay constraints on exotic 17 MeV vector bosons,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:15.875940Z"},"links":{"cited_paper":"/paper/2306.15077","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:bad1043ed849ca056bf6eff0c1f02f74e98a5c6fe6264e93711517caf8d19a60","observation_id":"2e835e83-3747-4f8b-aea2-15f385573270","resolution":{"observed_at":"2026-08-03T00:19:15.875940Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1509.00740","last_updated":"2015-10-19T14:48:28Z","snapshot_observed_at":"2026-08-17T21:01:54.506050Z","submitted_at":"2015-09-02T15:24:44Z","title":"Limit on the production of a low-mass vector boson in $\\mathrm{e}^{+}\\mathrm{e}^{-} \\to \\mathrm{U}\\gamma$, $\\mathrm{U} \\to \\mathrm{e}^{+}\\mathrm{e}^{-}$ with the KLOE experiment","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1509.00740","snapshot_observed_at":"2026-08-03T00:19:16.010375Z","title":"Limit on the production of a low-mass vector boson in e +e− →Uγ, U→e +e− with the KLOE experiment,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:16.010375Z"},"links":{"cited_paper":"/paper/1509.00740","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:c32862f790ba1c69f53041ce18b3bb9601a8a9d685be1819d8e257954f1395da","observation_id":"455eeb53-75c1-416d-8cc3-ffc0af2753bd","resolution":{"observed_at":"2026-08-03T00:19:16.010375Z","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":"2026-08-03T00:19:16.125272Z","title":"Four-body calculation for excited states of He-4,","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:16.125272Z"},"links":{"citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:eabb2012cce59528add60e4221735ad69caeb280514c02a6841be3bbe41a83f0","observation_id":"152f8bc2-13ad-4bd7-b0bb-7c1b3c852db4","resolution":{"observed_at":"2026-08-03T00:19:16.125272Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2409.16300","last_updated":"2024-09-10T06:23:00Z","snapshot_observed_at":"2026-08-16T13:19:53.099910Z","submitted_at":"2024-09-10T06:23:00Z","title":"An Update on the Hypothetical X17 Particle","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2409.16300","snapshot_observed_at":"2026-08-03T00:19:16.248474Z","title":"An Update of the Hypothetical X17 Particle,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:16.248474Z"},"links":{"cited_paper":"/paper/2409.16300","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:0f1b178df226d0cae320655a25241c3acbf55cfce41b2fcc79b11ead9f0aa699","observation_id":"f1fed39b-e72b-47a0-9d23-4fdfd61ea786","resolution":{"observed_at":"2026-08-03T00:19:16.248474Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2308.06473","last_updated":"2023-08-12T05:49:05Z","snapshot_observed_at":"2026-08-16T15:08:58.566128Z","submitted_at":"2023-08-12T05:49:05Z","title":"Observation of the X17 anomaly in the decay of the Giant Dipole Resonance of $^8$Be","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2308.06473","snapshot_observed_at":"2026-08-03T00:19:16.432129Z","title":"Observation of the X17 anomaly in the decay of the Giant Dipole Resonance of 8Be,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:16.432129Z"},"links":{"cited_paper":"/paper/2308.06473","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:a6962d963f42ffb2b1c4c85b78ac560636efe9a259073784f1eacc13a0819dbf","observation_id":"357cc921-aa5f-44bf-8192-b888483e6f8e","resolution":{"observed_at":"2026-08-03T00:19:16.432129Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1504.00607","last_updated":"2015-04-30T16:19:56Z","snapshot_observed_at":"2026-08-14T22:53:51.770626Z","submitted_at":"2015-04-02T16:21:03Z","title":"Search for the dark photon in $\\pi^0$ decays","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1504.00607","snapshot_observed_at":"2026-08-03T00:19:16.562015Z","title":"The SINDRUM-I Experiment,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:16.562015Z"},"links":{"cited_paper":"/paper/1504.00607","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:0d00d1384fc0cf0faae22535666f5d2bc76513aaeb89bd24ae26a9dc85de05b8","observation_id":"968a4c23-3f8d-4301-b182-6ed5d43c49fc","resolution":{"observed_at":"2026-08-03T00:19:16.562015Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0902.0335","last_updated":"2009-02-02T18:47:32Z","snapshot_observed_at":"2026-08-15T05:56:06.663529Z","submitted_at":"2009-02-02T18:47:32Z","title":"Precision determination of electroweak coupling from atomic parity violation and implications for particle physics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0902.0335","snapshot_observed_at":"2026-08-03T00:19:16.727969Z","title":"Precision determination of electroweak coupling from atomic parity violation and implications for particle physics,","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:16.727969Z"},"links":{"cited_paper":"/paper/0902.0335","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:e04f65cbf46309998cf463907c65b9877653bc2fa54f55b79ac90ed6e433d0ae","observation_id":"6d8270f7-7058-483d-99ec-472c67b1129d","resolution":{"observed_at":"2026-08-03T00:19:16.727969Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1709.10009","last_updated":"2017-12-09T22:21:41Z","snapshot_observed_at":"2026-08-17T03:19:49.535364Z","submitted_at":"2017-09-28T15:08:44Z","title":"Probing low-mass vector bosons with parity nonconservation and nuclear anapole moment measurements in atoms and molecules","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1709.10009","snapshot_observed_at":"2026-08-03T00:19:16.826567Z","title":"Probing low-mass vector bosons with parity nonconservation and nuclear anapole moment measurements in atoms and molecules,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:16.826567Z"},"links":{"cited_paper":"/paper/1709.10009","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:e17eedc62ed0dd81100197a2416550fea624b0c51e0c284b78008ad031b52694","observation_id":"421b5897-7866-4361-9921-d476b490552d","resolution":{"observed_at":"2026-08-03T00:19:16.826567Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1406.2343","last_updated":"2014-06-09T20:21:24Z","snapshot_observed_at":"2026-08-14T23:31:00.089484Z","submitted_at":"2014-06-09T20:21:24Z","title":"Quantum Monte Carlo calculations of electromagnetic transitions in 8Be with meson-exchange currents derived from chiral effective field theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1406.2343","snapshot_observed_at":"2026-08-03T00:19:16.957708Z","title":"Quantum Monte Carlo calculations of electromagnetic transitions in 8Be with meson-exchange 11 currents derived from chiral effective field theory,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:16.957708Z"},"links":{"cited_paper":"/paper/1406.2343","citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:eda154eff14c1daa7e7a976382a14e9d189ce9b2587fb24aa5f76606cc224686","observation_id":"6d8a97a8-cdc5-42b9-9fc1-978e8f2cc399","resolution":{"observed_at":"2026-08-03T00:19:16.957708Z","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":"2026-08-03T00:19:17.051549Z","title":"http://www.nndc.bnl.gov/ensdf","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-03T00:19:17.051549Z"},"links":{"citing_paper":"/paper/2602.11263"},"observation_digest":"sha256:4f8f7bacb07db0a114a6ce8ca20d35f39b529ee79712f8bc405110f93716527f","observation_id":"23506cc2-c35f-4af2-aff5-90aa4d5a5ada","resolution":{"observed_at":"2026-08-03T00:19:17.051549Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2602.11263","last_updated":"2026-02-11T19:00:01Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-14T08:27:36.451020Z","submitted_at":"2026-02-11T19:00:01Z","title":"The X17 with Chiral Couplings"},"reference_resolution":{"displayed":35,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":35,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":35},"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":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"thesis":"As of 18 August 2026, this Paper Citation Record lists 35 of 35 outbound references and 5 inbound Pith citation observations for arXiv:2602.11263."}