{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:JNIY4QJK7M2EFERJCCXF6LRICB","short_pith_number":"pith:JNIY4QJK","schema_version":"1.0","canonical_sha256":"4b518e412afb3442922910ae5f2e2810644608819310b11c49a280888cb8eca9","source":{"kind":"arxiv","id":"1607.02267","version":2},"attestation_state":"computed","paper":{"title":"Production of light nuclei in the thermal and coalescence models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"Stanislaw Mrowczynski","submitted_at":"2016-07-08T08:21:46Z","abstract_excerpt":"The thermal model properly describes the production yields of light nuclei in relativistic heavy-ion collisions even so the loosely bound sizable nuclei cannot exist in the dense and hot hadron gas at a chemical freeze-out. Within the coalescence model, light nuclei are formed at the latest stage of nuclear collisions - a kinetic freeze-out - due to final state interactions. After discussing the models, we derive simple analytic formulas and, using model parameters directly inferred from experimental data, we show that the thermal and coalescence model predictions are quantitatively close to e"},"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":"1607.02267","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-07-08T08:21:46Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"13f521c5ed1a45e21680817039ea5a464db1ea292997c3b3e85da07b3fc1441c","abstract_canon_sha256":"6afb7189f170e763abfaa9739e04ab3659046740f4208fc51b57af3011b15a91"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:43:02.612790Z","signature_b64":"UWka+1/Nd6gEoI2C0mlB3rU6dXSpUTgM1Y9GluIZKmwAq4fdqqurJP77aqcgyn4ex11yI4xRCV91Y1MYv7xhBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4b518e412afb3442922910ae5f2e2810644608819310b11c49a280888cb8eca9","last_reissued_at":"2026-05-18T00:43:02.612096Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:43:02.612096Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Production of light nuclei in the thermal and coalescence models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"Stanislaw Mrowczynski","submitted_at":"2016-07-08T08:21:46Z","abstract_excerpt":"The thermal model properly describes the production yields of light nuclei in relativistic heavy-ion collisions even so the loosely bound sizable nuclei cannot exist in the dense and hot hadron gas at a chemical freeze-out. Within the coalescence model, light nuclei are formed at the latest stage of nuclear collisions - a kinetic freeze-out - due to final state interactions. After discussing the models, we derive simple analytic formulas and, using model parameters directly inferred from experimental data, we show that the thermal and coalescence model predictions are quantitatively close to e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.02267","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":"1607.02267","created_at":"2026-05-18T00:43:02.612213+00:00"},{"alias_kind":"arxiv_version","alias_value":"1607.02267v2","created_at":"2026-05-18T00:43:02.612213+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.02267","created_at":"2026-05-18T00:43:02.612213+00:00"},{"alias_kind":"pith_short_12","alias_value":"JNIY4QJK7M2E","created_at":"2026-05-18T12:30:25.849896+00:00"},{"alias_kind":"pith_short_16","alias_value":"JNIY4QJK7M2EFERJ","created_at":"2026-05-18T12:30:25.849896+00:00"},{"alias_kind":"pith_short_8","alias_value":"JNIY4QJK","created_at":"2026-05-18T12:30:25.849896+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1907.06868","citing_title":"Testing production scenarios for (anti-)(hyper-)nuclei with multiplicity-dependent measurements at the LHC","ref_index":13,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JNIY4QJK7M2EFERJCCXF6LRICB","json":"https://pith.science/pith/JNIY4QJK7M2EFERJCCXF6LRICB.json","graph_json":"https://pith.science/api/pith-number/JNIY4QJK7M2EFERJCCXF6LRICB/graph.json","events_json":"https://pith.science/api/pith-number/JNIY4QJK7M2EFERJCCXF6LRICB/events.json","paper":"https://pith.science/paper/JNIY4QJK"},"agent_actions":{"view_html":"https://pith.science/pith/JNIY4QJK7M2EFERJCCXF6LRICB","download_json":"https://pith.science/pith/JNIY4QJK7M2EFERJCCXF6LRICB.json","view_paper":"https://pith.science/paper/JNIY4QJK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1607.02267&json=true","fetch_graph":"https://pith.science/api/pith-number/JNIY4QJK7M2EFERJCCXF6LRICB/graph.json","fetch_events":"https://pith.science/api/pith-number/JNIY4QJK7M2EFERJCCXF6LRICB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JNIY4QJK7M2EFERJCCXF6LRICB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JNIY4QJK7M2EFERJCCXF6LRICB/action/storage_attestation","attest_author":"https://pith.science/pith/JNIY4QJK7M2EFERJCCXF6LRICB/action/author_attestation","sign_citation":"https://pith.science/pith/JNIY4QJK7M2EFERJCCXF6LRICB/action/citation_signature","submit_replication":"https://pith.science/pith/JNIY4QJK7M2EFERJCCXF6LRICB/action/replication_record"}},"created_at":"2026-05-18T00:43:02.612213+00:00","updated_at":"2026-05-18T00:43:02.612213+00:00"}