{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:6RCC2MDYG3IAXQ7H5VSJVIJB3B","short_pith_number":"pith:6RCC2MDY","schema_version":"1.0","canonical_sha256":"f4442d307836d00bc3e7ed649aa121d87add9efd7a19cf432ef5ee43febbdab6","source":{"kind":"arxiv","id":"1604.05666","version":2},"attestation_state":"computed","paper":{"title":"Propagation of heavy baryons in heavy-ion collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"Francesco Scardina, Juan M. Torres-Rincon, Laura Tolos, Santosh K. Das, Vincenzo Greco, Vincenzo Minissale","submitted_at":"2016-04-19T17:39:44Z","abstract_excerpt":"The drag and diffusion coefficients of heavy baryons ($\\Lambda_c$ and $\\Lambda_b$) in the hadronic phase created in the latter stage of the heavy-ion collisions at RHIC and LHC energies have been evaluated recently. In this work we compute some experimental observables, such as the nuclear suppression factor $R_{AA}$ and the elliptic flow $v_2$ of heavy baryons at RHIC and LHC energies, highlighting the role of the hadronic phase contribution to these observables, which are going to be measured at Run 3 of LHC. For the time evolution of the heavy quarks in the QGP and heavy baryons in the hadr"},"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":"1604.05666","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-04-19T17:39:44Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"9bae949fdd40370be1c374df8f2a367ef06f9a0ddfd0a0288185bfbe22e9af1d","abstract_canon_sha256":"43cae9047ff8c49fadf482d5b2fcebd4a7c1fc19f0c2272c79828db6314aeaa8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:53:08.319293Z","signature_b64":"eA9Y7n6iBmDvb0Ie69OXnNPD3eowTt8Xic+J0oztUu9w52gx7UaMQw87KLNySuCgHg+lysEaxeMz6iYEowgDAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f4442d307836d00bc3e7ed649aa121d87add9efd7a19cf432ef5ee43febbdab6","last_reissued_at":"2026-05-18T00:53:08.318901Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:53:08.318901Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Propagation of heavy baryons in heavy-ion collisions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"Francesco Scardina, Juan M. Torres-Rincon, Laura Tolos, Santosh K. Das, Vincenzo Greco, Vincenzo Minissale","submitted_at":"2016-04-19T17:39:44Z","abstract_excerpt":"The drag and diffusion coefficients of heavy baryons ($\\Lambda_c$ and $\\Lambda_b$) in the hadronic phase created in the latter stage of the heavy-ion collisions at RHIC and LHC energies have been evaluated recently. In this work we compute some experimental observables, such as the nuclear suppression factor $R_{AA}$ and the elliptic flow $v_2$ of heavy baryons at RHIC and LHC energies, highlighting the role of the hadronic phase contribution to these observables, which are going to be measured at Run 3 of LHC. For the time evolution of the heavy quarks in the QGP and heavy baryons in the hadr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.05666","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":"1604.05666","created_at":"2026-05-18T00:53:08.318959+00:00"},{"alias_kind":"arxiv_version","alias_value":"1604.05666v2","created_at":"2026-05-18T00:53:08.318959+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.05666","created_at":"2026-05-18T00:53:08.318959+00:00"},{"alias_kind":"pith_short_12","alias_value":"6RCC2MDYG3IA","created_at":"2026-05-18T12:30:01.593930+00:00"},{"alias_kind":"pith_short_16","alias_value":"6RCC2MDYG3IAXQ7H","created_at":"2026-05-18T12:30:01.593930+00:00"},{"alias_kind":"pith_short_8","alias_value":"6RCC2MDY","created_at":"2026-05-18T12:30:01.593930+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2605.21222","citing_title":"System-size dependence of the $D^0$--$D_s^+$ flow splitting from early $D_s^+$ formation at $\\sqrt{s_{NN}} = 5.36$~TeV","ref_index":28,"is_internal_anchor":true},{"citing_arxiv_id":"2512.07169","citing_title":"Bayesian Inference of Heavy-Quark Dissipation and Jet Transport Parameters from D-Meson observables in heavy-ion collisions at the LHC energies","ref_index":24,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6RCC2MDYG3IAXQ7H5VSJVIJB3B","json":"https://pith.science/pith/6RCC2MDYG3IAXQ7H5VSJVIJB3B.json","graph_json":"https://pith.science/api/pith-number/6RCC2MDYG3IAXQ7H5VSJVIJB3B/graph.json","events_json":"https://pith.science/api/pith-number/6RCC2MDYG3IAXQ7H5VSJVIJB3B/events.json","paper":"https://pith.science/paper/6RCC2MDY"},"agent_actions":{"view_html":"https://pith.science/pith/6RCC2MDYG3IAXQ7H5VSJVIJB3B","download_json":"https://pith.science/pith/6RCC2MDYG3IAXQ7H5VSJVIJB3B.json","view_paper":"https://pith.science/paper/6RCC2MDY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1604.05666&json=true","fetch_graph":"https://pith.science/api/pith-number/6RCC2MDYG3IAXQ7H5VSJVIJB3B/graph.json","fetch_events":"https://pith.science/api/pith-number/6RCC2MDYG3IAXQ7H5VSJVIJB3B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6RCC2MDYG3IAXQ7H5VSJVIJB3B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6RCC2MDYG3IAXQ7H5VSJVIJB3B/action/storage_attestation","attest_author":"https://pith.science/pith/6RCC2MDYG3IAXQ7H5VSJVIJB3B/action/author_attestation","sign_citation":"https://pith.science/pith/6RCC2MDYG3IAXQ7H5VSJVIJB3B/action/citation_signature","submit_replication":"https://pith.science/pith/6RCC2MDYG3IAXQ7H5VSJVIJB3B/action/replication_record"}},"created_at":"2026-05-18T00:53:08.318959+00:00","updated_at":"2026-05-18T00:53:08.318959+00:00"}