{"as_of":"2026-08-13T23:41:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:5cfd9eca188e0d10cb810a9bbd371120e1abce5fd8d8a6cc79727e1be4749f56","coverage":[{"denominator":0,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":5,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":5,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-13T06:32:02.005865+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":"2026-08-12T22:01:49.587433Z","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":"2026-05-12T10:56:30.327707Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2103.01290","last_updated":"2021-09-11T00:15:19Z","snapshot_observed_at":"2026-08-13T17:41:51.446100Z","submitted_at":"2021-03-01T20:23:13Z","title":"Search for top squark production in fully-hadronic final states in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2103.01290","snapshot_observed_at":"2026-08-12T22:01:49.587433Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2411.08112","last_updated":"2025-07-22T10:43:58Z","snapshot_observed_at":"2026-08-13T14:17:43.844061Z","submitted_at":"2024-11-12T19:00:03Z","title":"Markov Chain Monte Carlo analysis to probe trilinear $R$-parity violating SUSY scenarios and possible LHC signatures","version":2},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-12T22:01:49.587433Z"},"links":{"cited_paper":"/paper/2103.01290","citing_paper":"/paper/2411.08112"},"observation_digest":"sha256:bf8cfde101b29692e31db27b297f3f341d64089fc98bc500086f3faffca4f029","observation_id":"73a74d4b-207c-4241-a5dc-9c6ddbc5fcda","resolution":{"observed_at":"2026-08-12T22:01:49.587433Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2103.01290","last_updated":"2021-09-11T00:15:19Z","snapshot_observed_at":"2026-08-13T17:41:51.446100Z","submitted_at":"2021-03-01T20:23:13Z","title":"Search for top squark production in fully-hadronic final states in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2103.01290","snapshot_observed_at":"2026-08-12T16:24:27.424471Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2411.13541","last_updated":"2024-11-20T18:51:54Z","snapshot_observed_at":"2026-08-13T13:24:10.719090Z","submitted_at":"2024-11-20T18:51:54Z","title":"Living dangerously with decoupled first/second generation scalars: SUSY prospects at the LHC","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-12T16:24:27.424471Z"},"links":{"cited_paper":"/paper/2103.01290","citing_paper":"/paper/2411.13541"},"observation_digest":"sha256:320829206a83a4db3fa2df18aee800824d06d88c8f2e64f9b6be24eb51b11e1e","observation_id":"91a063d3-341e-4767-954a-fe5a68472d81","resolution":{"observed_at":"2026-08-12T16:24:27.424471Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2103.01290","last_updated":"2021-09-11T00:15:19Z","snapshot_observed_at":"2026-08-13T17:41:51.446100Z","submitted_at":"2021-03-01T20:23:13Z","title":"Search for top squark production in fully-hadronic final states in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2103.01290","snapshot_observed_at":"2026-08-11T11:38:24.725386Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2412.15356","last_updated":"2025-03-18T19:45:22Z","snapshot_observed_at":"2026-08-11T11:27:57.274691Z","submitted_at":"2024-12-19T19:40:41Z","title":"Implications of Higgs mass for hidden sector SUSY breaking","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-11T11:38:24.725386Z"},"links":{"cited_paper":"/paper/2103.01290","citing_paper":"/paper/2412.15356"},"observation_digest":"sha256:a42e5b87fec8f82a190c2fc59c6a6029fab649ea8f0e30f31d01f093f05c067f","observation_id":"f4c193a2-2a94-4c9f-8d8f-b795eb9b65ff","resolution":{"observed_at":"2026-08-11T11:38:24.725386Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2103.01290","last_updated":"2021-09-11T00:15:19Z","snapshot_observed_at":"2026-08-13T17:41:51.446100Z","submitted_at":"2021-03-01T20:23:13Z","title":"Search for top squark production in fully-hadronic final states in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2103.01290","snapshot_observed_at":"2026-08-03T22:32:25.962726Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2511.10490","last_updated":"2026-07-21T18:16:19Z","snapshot_observed_at":"2026-08-12T21:45:42.625681Z","submitted_at":"2025-11-13T16:58:01Z","title":"Toward a Comprehensive Exploration of Flavored Dark Matter Models","version":2},"reference_index":105,"source":"pdf_text","source_observed_at":"2026-08-03T22:32:25.962726Z"},"links":{"cited_paper":"/paper/2103.01290","citing_paper":"/paper/2511.10490"},"observation_digest":"sha256:bdff2cb8b6efda3b60ca85ce27cc92956bbdeb973bf9e843926ca5bb52696d34","observation_id":"c8e75a19-813c-42e3-a2be-dc22e7ca77e4","resolution":{"observed_at":"2026-08-03T22:32:25.962726Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2103.01290","last_updated":"2021-09-11T00:15:19Z","snapshot_observed_at":"2026-08-13T17:41:51.446100Z","submitted_at":"2021-03-01T20:23:13Z","title":"Search for top squark production in fully-hadronic final states in proton-proton collisions at $\\sqrt{s} =$ 13 TeV","version":2},"cited_work":{"arxiv_id":"2103.01290","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2103.01290","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":null,"venue":null,"work_id":"25eeec1e-14ef-4ebe-bab1-b7666dcd2ad0","year":2021},"citing_paper":{"arxiv_id":"2605.03427","last_updated":"2026-05-05T07:03:21Z","snapshot_observed_at":"2026-08-09T09:24:31.106734Z","submitted_at":"2026-05-05T07:03:21Z","title":"Search for Long-Lived Dark Photons from Dark Radiation at the LHC","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-05-07T16:04:41.839531Z"},"links":{"cited_paper":"/paper/2103.01290","citing_paper":"/paper/2605.03427"},"observation_digest":"sha256:352248ae0a9f2dcba7eb0a38834efa69be1b0339e265794475b21404c849c041","observation_id":"c14f437a-1d81-406e-a266-e5674f11b3a9","resolution":{"observed_at":"2026-05-12T10:56:30.330039Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2103.01290/citation-record","integrity":"/paper/2103.01290/integrity","json":"/paper/2103.01290/citation-record.json","paper":"/paper/2103.01290"},"outbound":[],"paper":{"arxiv_id":"2103.01290","last_updated":"2021-09-11T00:15:19Z","latest_version":2,"primary_category":"hep-ex","snapshot_observed_at":"2026-08-13T17:41:51.446100Z","submitted_at":"2021-03-01T20:23:13Z","title":"Search for top squark production in fully-hadronic final states in proton-proton collisions at $\\sqrt{s} =$ 13 TeV"},"reference_resolution":{"displayed":0,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":0,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":0},"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":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"thesis":"As of 13 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 5 inbound Pith citation observations for arXiv:2103.01290."}