{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:MGJLYG5R6Z7PD22PUFKJQ4RCRZ","short_pith_number":"pith:MGJLYG5R","schema_version":"1.0","canonical_sha256":"6192bc1bb1f67ef1eb4fa1549872228e44b1b1b76dc61f30585718113dba4b66","source":{"kind":"arxiv","id":"1708.03497","version":2},"attestation_state":"computed","paper":{"title":"Measurement of prompt D$^0$ meson azimuthal anisotropy in PbPb collisions at $\\sqrt{s_\\mathrm{NN}} = $5.02 TeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"CMS Collaboration","submitted_at":"2017-08-11T10:07:22Z","abstract_excerpt":"The prompt D$^0$ meson azimuthal anisotropy coefficients, $v_2$ and $v_3$, are measured at midrapidity ($|y| < 1.0$) in PbPb collisions at a center-of-mass energy $\\sqrt{s_\\mathrm{NN}} = $5.02 TeV per nucleon pair with data collected by the CMS experiment. The measurement is performed in the transverse momentum ($p_\\mathrm{T}$) range of 1 to 40 GeV/c, for central and midcentral collisions. The $v_2$ coefficient is found to be positive throughout the $p_\\mathrm{T}$ range studied. The first measurement of the prompt D$^0$ meson $v_3$ coefficient is performed, and values up to 0.07 are observed f"},"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":"1708.03497","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2017-08-11T10:07:22Z","cross_cats_sorted":[],"title_canon_sha256":"2d0a297a85985e363ddf15d3f9c8942002433cb0c1cf2782dd8a086798977a62","abstract_canon_sha256":"43e333e4515a07506a6d632cb7474c2dea40cb91bbf033d934ecdf10354cd9e5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:14:47.411173Z","signature_b64":"AhfSX3kucZxdLovRUeidsgTjti5ZvFZ0W0m+AuU+WWrvl+G9iEHMrJcRlM+UNup4V0CV5AphANsfdxXKXU9WAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6192bc1bb1f67ef1eb4fa1549872228e44b1b1b76dc61f30585718113dba4b66","last_reissued_at":"2026-05-18T00:14:47.410735Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:14:47.410735Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of prompt D$^0$ meson azimuthal anisotropy in PbPb collisions at $\\sqrt{s_\\mathrm{NN}} = $5.02 TeV","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"CMS Collaboration","submitted_at":"2017-08-11T10:07:22Z","abstract_excerpt":"The prompt D$^0$ meson azimuthal anisotropy coefficients, $v_2$ and $v_3$, are measured at midrapidity ($|y| < 1.0$) in PbPb collisions at a center-of-mass energy $\\sqrt{s_\\mathrm{NN}} = $5.02 TeV per nucleon pair with data collected by the CMS experiment. The measurement is performed in the transverse momentum ($p_\\mathrm{T}$) range of 1 to 40 GeV/c, for central and midcentral collisions. The $v_2$ coefficient is found to be positive throughout the $p_\\mathrm{T}$ range studied. The first measurement of the prompt D$^0$ meson $v_3$ coefficient is performed, and values up to 0.07 are observed f"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.03497","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":""},"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":"1708.03497","created_at":"2026-05-18T00:14:47.410800+00:00"},{"alias_kind":"arxiv_version","alias_value":"1708.03497v2","created_at":"2026-05-18T00:14:47.410800+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.03497","created_at":"2026-05-18T00:14:47.410800+00:00"},{"alias_kind":"pith_short_12","alias_value":"MGJLYG5R6Z7P","created_at":"2026-05-18T12:31:31.346846+00:00"},{"alias_kind":"pith_short_16","alias_value":"MGJLYG5R6Z7PD22P","created_at":"2026-05-18T12:31:31.346846+00:00"},{"alias_kind":"pith_short_8","alias_value":"MGJLYG5R","created_at":"2026-05-18T12:31:31.346846+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.11017","citing_title":"Exploring the origin of D$^0$ meson elliptic flow in PbPb collisions at $\\sqrt{s_\\mathrm{NN}}$ = 5.02 TeV using event shape engineering","ref_index":17,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MGJLYG5R6Z7PD22PUFKJQ4RCRZ","json":"https://pith.science/pith/MGJLYG5R6Z7PD22PUFKJQ4RCRZ.json","graph_json":"https://pith.science/api/pith-number/MGJLYG5R6Z7PD22PUFKJQ4RCRZ/graph.json","events_json":"https://pith.science/api/pith-number/MGJLYG5R6Z7PD22PUFKJQ4RCRZ/events.json","paper":"https://pith.science/paper/MGJLYG5R"},"agent_actions":{"view_html":"https://pith.science/pith/MGJLYG5R6Z7PD22PUFKJQ4RCRZ","download_json":"https://pith.science/pith/MGJLYG5R6Z7PD22PUFKJQ4RCRZ.json","view_paper":"https://pith.science/paper/MGJLYG5R","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1708.03497&json=true","fetch_graph":"https://pith.science/api/pith-number/MGJLYG5R6Z7PD22PUFKJQ4RCRZ/graph.json","fetch_events":"https://pith.science/api/pith-number/MGJLYG5R6Z7PD22PUFKJQ4RCRZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MGJLYG5R6Z7PD22PUFKJQ4RCRZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MGJLYG5R6Z7PD22PUFKJQ4RCRZ/action/storage_attestation","attest_author":"https://pith.science/pith/MGJLYG5R6Z7PD22PUFKJQ4RCRZ/action/author_attestation","sign_citation":"https://pith.science/pith/MGJLYG5R6Z7PD22PUFKJQ4RCRZ/action/citation_signature","submit_replication":"https://pith.science/pith/MGJLYG5R6Z7PD22PUFKJQ4RCRZ/action/replication_record"}},"created_at":"2026-05-18T00:14:47.410800+00:00","updated_at":"2026-05-18T00:14:47.410800+00:00"}