{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:4TOECFMKKGNKKZKBU5ZI6ZUC5Z","short_pith_number":"pith:4TOECFMK","schema_version":"1.0","canonical_sha256":"e4dc41158a519aa56541a7728f6682ee780b1ddbc840b8ae058fc7d43d719ecf","source":{"kind":"arxiv","id":"1804.10557","version":1},"attestation_state":"computed","paper":{"title":"Net baryon diffusion in fluid dynamic simulations of relativistic 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":"Akihiko Monnai, Bj\\\"orn Schenke, Charles Gale, Chun Shen, Gabriel S. Denicol, Sangyong Jeon","submitted_at":"2018-04-27T15:23:42Z","abstract_excerpt":"A hybrid (hydrodynamics + hadronic transport) theoretical framework is assembled to model the bulk dynamics of relativistic heavy-ion collisions at energies accessible in the Beam Energy Scan (BES) program at the Relativistic Heavy-Ion Collider (RHIC) and the NA61/SHINE experiment at CERN. The system's energy-momentum tensor and net baryon current are evolved according to relativistic hydrodynamics with finite shear viscosity and non-zero net baryon diffusion. Our hydrodynamic description is matched to a hadronic transport model in the dilute region. With this fully integrated theoretical fram"},"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":"1804.10557","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2018-04-27T15:23:42Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"48c07cfd0920e2e369045c14526784201a3b0256048bcdd12738b5b469361e7a","abstract_canon_sha256":"7b28c7fabd5fdf9cf68fb8a3bb6bff5c74c257ec0b2654b345b2771529bbd9f8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:39:37.200838Z","signature_b64":"AIcotR4jL0WMVnUpgGpCusDqInxAO0ON4+8DWfHJt2WoIwVmb/jsMPKlm6owsr6eXXflmsHeEKXh/SJT4OulCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e4dc41158a519aa56541a7728f6682ee780b1ddbc840b8ae058fc7d43d719ecf","last_reissued_at":"2026-05-17T23:39:37.200169Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:39:37.200169Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Net baryon diffusion in fluid dynamic simulations of relativistic 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":"Akihiko Monnai, Bj\\\"orn Schenke, Charles Gale, Chun Shen, Gabriel S. Denicol, Sangyong Jeon","submitted_at":"2018-04-27T15:23:42Z","abstract_excerpt":"A hybrid (hydrodynamics + hadronic transport) theoretical framework is assembled to model the bulk dynamics of relativistic heavy-ion collisions at energies accessible in the Beam Energy Scan (BES) program at the Relativistic Heavy-Ion Collider (RHIC) and the NA61/SHINE experiment at CERN. The system's energy-momentum tensor and net baryon current are evolved according to relativistic hydrodynamics with finite shear viscosity and non-zero net baryon diffusion. Our hydrodynamic description is matched to a hadronic transport model in the dilute region. With this fully integrated theoretical fram"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1804.10557","kind":"arxiv","version":1},"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":"1804.10557","created_at":"2026-05-17T23:39:37.200271+00:00"},{"alias_kind":"arxiv_version","alias_value":"1804.10557v1","created_at":"2026-05-17T23:39:37.200271+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1804.10557","created_at":"2026-05-17T23:39:37.200271+00:00"},{"alias_kind":"pith_short_12","alias_value":"4TOECFMKKGNK","created_at":"2026-05-18T12:32:05.422762+00:00"},{"alias_kind":"pith_short_16","alias_value":"4TOECFMKKGNKKZKB","created_at":"2026-05-18T12:32:05.422762+00:00"},{"alias_kind":"pith_short_8","alias_value":"4TOECFMK","created_at":"2026-05-18T12:32:05.422762+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2512.08007","citing_title":"(3+1)D event-by-event pre-equilibrium dynamics in heavy-ion collisions","ref_index":70,"is_internal_anchor":true},{"citing_arxiv_id":"2602.16369","citing_title":"Rapidity dependence of mean transverse momentum fluctuation and decorrelation in baryon-dense medium","ref_index":89,"is_internal_anchor":true},{"citing_arxiv_id":"2604.22352","citing_title":"Four-dimensional QCD equation of state from a quasi-parton model with physics-informed neural networks","ref_index":11,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4TOECFMKKGNKKZKBU5ZI6ZUC5Z","json":"https://pith.science/pith/4TOECFMKKGNKKZKBU5ZI6ZUC5Z.json","graph_json":"https://pith.science/api/pith-number/4TOECFMKKGNKKZKBU5ZI6ZUC5Z/graph.json","events_json":"https://pith.science/api/pith-number/4TOECFMKKGNKKZKBU5ZI6ZUC5Z/events.json","paper":"https://pith.science/paper/4TOECFMK"},"agent_actions":{"view_html":"https://pith.science/pith/4TOECFMKKGNKKZKBU5ZI6ZUC5Z","download_json":"https://pith.science/pith/4TOECFMKKGNKKZKBU5ZI6ZUC5Z.json","view_paper":"https://pith.science/paper/4TOECFMK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1804.10557&json=true","fetch_graph":"https://pith.science/api/pith-number/4TOECFMKKGNKKZKBU5ZI6ZUC5Z/graph.json","fetch_events":"https://pith.science/api/pith-number/4TOECFMKKGNKKZKBU5ZI6ZUC5Z/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4TOECFMKKGNKKZKBU5ZI6ZUC5Z/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4TOECFMKKGNKKZKBU5ZI6ZUC5Z/action/storage_attestation","attest_author":"https://pith.science/pith/4TOECFMKKGNKKZKBU5ZI6ZUC5Z/action/author_attestation","sign_citation":"https://pith.science/pith/4TOECFMKKGNKKZKBU5ZI6ZUC5Z/action/citation_signature","submit_replication":"https://pith.science/pith/4TOECFMKKGNKKZKBU5ZI6ZUC5Z/action/replication_record"}},"created_at":"2026-05-17T23:39:37.200271+00:00","updated_at":"2026-05-17T23:39:37.200271+00:00"}