{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:KNDIHUAHTMLOKI7OLYH73GGFII","short_pith_number":"pith:KNDIHUAH","schema_version":"1.0","canonical_sha256":"534683d0079b16e523ee5e0ffd98c542272d592caf7c65f6f3594574015b0991","source":{"kind":"arxiv","id":"2406.14409","version":2},"attestation_state":"computed","paper":{"title":"Measurement of the polarizations of prompt and non-prompt J/$\\psi$ and $\\psi$(2S) mesons produced in pp collisions at $\\sqrt{s}$ = 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2024-06-20T15:31:31Z","abstract_excerpt":"The polarizations of prompt and non-prompt J$/\\psi$ and $\\psi$(2S) mesons are measured in proton-proton collisions at $\\sqrt{s}$ = 13 TeV, using data samples collected by the CMS experiment in 2017 and 2018, corresponding to a total integrated luminosity of 103.3 fb$^{-1}$. Based on the analysis of the dimuon decay angular distributions in the helicity frame, the polar anisotropy, $\\lambda_\\theta$, is measured as a function of the transverse momentum, $p_\\mathrm{T}$, of the charmonium states, in the 25-120 and 20-100 GeV ranges for the J$/\\psi$ and $\\psi$(2S), respectively. The non-prompt pola"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2406.14409","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2024-06-20T15:31:31Z","cross_cats_sorted":[],"title_canon_sha256":"42afd2b02651e784a0f64d9d142e105ebf998210eaf54d9b3cd4593fd0bb8455","abstract_canon_sha256":"d89f9038665797607fc76bfc7d08f8972dcf6b0e35896709f874797352f30d13"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:16:50.342177Z","signature_b64":"RU7UdYQR/QAVH7jEKe4SgHlffYIcipexzJwfiyFQ4c/Pf7+7xlLaCk++X4wLwno/g+scHmVGULcDLxIrfREfCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"534683d0079b16e523ee5e0ffd98c542272d592caf7c65f6f3594574015b0991","last_reissued_at":"2026-07-05T09:16:50.341684Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:16:50.341684Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of the polarizations of prompt and non-prompt J/$\\psi$ and $\\psi$(2S) mesons produced in pp collisions at $\\sqrt{s}$ = 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2024-06-20T15:31:31Z","abstract_excerpt":"The polarizations of prompt and non-prompt J$/\\psi$ and $\\psi$(2S) mesons are measured in proton-proton collisions at $\\sqrt{s}$ = 13 TeV, using data samples collected by the CMS experiment in 2017 and 2018, corresponding to a total integrated luminosity of 103.3 fb$^{-1}$. Based on the analysis of the dimuon decay angular distributions in the helicity frame, the polar anisotropy, $\\lambda_\\theta$, is measured as a function of the transverse momentum, $p_\\mathrm{T}$, of the charmonium states, in the 25-120 and 20-100 GeV ranges for the J$/\\psi$ and $\\psi$(2S), respectively. The non-prompt pola"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.14409","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2406.14409/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2406.14409","created_at":"2026-07-05T09:16:50.341742+00:00"},{"alias_kind":"arxiv_version","alias_value":"2406.14409v2","created_at":"2026-07-05T09:16:50.341742+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.14409","created_at":"2026-07-05T09:16:50.341742+00:00"},{"alias_kind":"pith_short_12","alias_value":"KNDIHUAHTMLO","created_at":"2026-07-05T09:16:50.341742+00:00"},{"alias_kind":"pith_short_16","alias_value":"KNDIHUAHTMLOKI7O","created_at":"2026-07-05T09:16:50.341742+00:00"},{"alias_kind":"pith_short_8","alias_value":"KNDIHUAH","created_at":"2026-07-05T09:16:50.341742+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.16384","citing_title":"How well does nonrelativistic QCD factorization work at next-to-leading order?","ref_index":52,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KNDIHUAHTMLOKI7OLYH73GGFII","json":"https://pith.science/pith/KNDIHUAHTMLOKI7OLYH73GGFII.json","graph_json":"https://pith.science/api/pith-number/KNDIHUAHTMLOKI7OLYH73GGFII/graph.json","events_json":"https://pith.science/api/pith-number/KNDIHUAHTMLOKI7OLYH73GGFII/events.json","paper":"https://pith.science/paper/KNDIHUAH"},"agent_actions":{"view_html":"https://pith.science/pith/KNDIHUAHTMLOKI7OLYH73GGFII","download_json":"https://pith.science/pith/KNDIHUAHTMLOKI7OLYH73GGFII.json","view_paper":"https://pith.science/paper/KNDIHUAH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2406.14409&json=true","fetch_graph":"https://pith.science/api/pith-number/KNDIHUAHTMLOKI7OLYH73GGFII/graph.json","fetch_events":"https://pith.science/api/pith-number/KNDIHUAHTMLOKI7OLYH73GGFII/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KNDIHUAHTMLOKI7OLYH73GGFII/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KNDIHUAHTMLOKI7OLYH73GGFII/action/storage_attestation","attest_author":"https://pith.science/pith/KNDIHUAHTMLOKI7OLYH73GGFII/action/author_attestation","sign_citation":"https://pith.science/pith/KNDIHUAHTMLOKI7OLYH73GGFII/action/citation_signature","submit_replication":"https://pith.science/pith/KNDIHUAHTMLOKI7OLYH73GGFII/action/replication_record"}},"created_at":"2026-07-05T09:16:50.341742+00:00","updated_at":"2026-07-05T09:16:50.341742+00:00"}