{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:VE3HLEFXIUZKNMQGKI2PV3UQ7I","short_pith_number":"pith:VE3HLEFX","schema_version":"1.0","canonical_sha256":"a9367590b74532a6b2065234faee90fa075ac4158729883702be8d167ba6a268","source":{"kind":"arxiv","id":"2606.10441","version":1},"attestation_state":"computed","paper":{"title":"Sequential Clusterization of Light Nuclei and Hypernuclei in Heavy-Ion Collisions within a Wigner Function Coalescence Framework","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Jiaxing Zhao, Junyi Han, Norbert Hermann, Yaping Wang, Yingjie Zhou, Yue-Hang Leung","submitted_at":"2026-06-09T05:37:33Z","abstract_excerpt":"We investigate the formation of light nuclei and hypernuclei in Au+Au collisions at $\\sqrt{s_{NN}}=3~\\mathrm{GeV}$ within a coalescence framework embedded in the microscopic N-body Parton-Hadron-Quantum-Molecular Dynamics (PHQMD) transport model. The Wigner phase-space distributions employed in the coalescence calculation are constructed from realistic $N$-body wave functions obtained by solving the Schr\\\"odinger equation in the hyperspherical harmonics formalism, providing a solid and parameter-free description of nuclear clusters and hypernuclei. By comparing calculated rapidity distribution"},"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":"2606.10441","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2026-06-09T05:37:33Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"2b1e1fcf99c08ed26ef5f2c67c400bccbc353770e2b01db7e85c077aaceed13a","abstract_canon_sha256":"118650d75addf59cd9ebaecb81deaf3edb706686a11b04f2d01a5aa47fd7240f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-10T01:10:19.230776Z","signature_b64":"YLH24Cn4FEPbbKj626Auoy9Alhgsc5iSyFRCdIoVKl2zuFh1kKtF+Z7LmnA1dX0qUiUFtG7CvpNrej6lJeNaAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a9367590b74532a6b2065234faee90fa075ac4158729883702be8d167ba6a268","last_reissued_at":"2026-06-10T01:10:19.229883Z","signature_status":"signed_v1","first_computed_at":"2026-06-10T01:10:19.229883Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Sequential Clusterization of Light Nuclei and Hypernuclei in Heavy-Ion Collisions within a Wigner Function Coalescence Framework","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Jiaxing Zhao, Junyi Han, Norbert Hermann, Yaping Wang, Yingjie Zhou, Yue-Hang Leung","submitted_at":"2026-06-09T05:37:33Z","abstract_excerpt":"We investigate the formation of light nuclei and hypernuclei in Au+Au collisions at $\\sqrt{s_{NN}}=3~\\mathrm{GeV}$ within a coalescence framework embedded in the microscopic N-body Parton-Hadron-Quantum-Molecular Dynamics (PHQMD) transport model. The Wigner phase-space distributions employed in the coalescence calculation are constructed from realistic $N$-body wave functions obtained by solving the Schr\\\"odinger equation in the hyperspherical harmonics formalism, providing a solid and parameter-free description of nuclear clusters and hypernuclei. By comparing calculated rapidity distribution"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.10441","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2606.10441/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":"2606.10441","created_at":"2026-06-10T01:10:19.230046+00:00"},{"alias_kind":"arxiv_version","alias_value":"2606.10441v1","created_at":"2026-06-10T01:10:19.230046+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.10441","created_at":"2026-06-10T01:10:19.230046+00:00"},{"alias_kind":"pith_short_12","alias_value":"VE3HLEFXIUZK","created_at":"2026-06-10T01:10:19.230046+00:00"},{"alias_kind":"pith_short_16","alias_value":"VE3HLEFXIUZKNMQG","created_at":"2026-06-10T01:10:19.230046+00:00"},{"alias_kind":"pith_short_8","alias_value":"VE3HLEFX","created_at":"2026-06-10T01:10:19.230046+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VE3HLEFXIUZKNMQGKI2PV3UQ7I","json":"https://pith.science/pith/VE3HLEFXIUZKNMQGKI2PV3UQ7I.json","graph_json":"https://pith.science/api/pith-number/VE3HLEFXIUZKNMQGKI2PV3UQ7I/graph.json","events_json":"https://pith.science/api/pith-number/VE3HLEFXIUZKNMQGKI2PV3UQ7I/events.json","paper":"https://pith.science/paper/VE3HLEFX"},"agent_actions":{"view_html":"https://pith.science/pith/VE3HLEFXIUZKNMQGKI2PV3UQ7I","download_json":"https://pith.science/pith/VE3HLEFXIUZKNMQGKI2PV3UQ7I.json","view_paper":"https://pith.science/paper/VE3HLEFX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2606.10441&json=true","fetch_graph":"https://pith.science/api/pith-number/VE3HLEFXIUZKNMQGKI2PV3UQ7I/graph.json","fetch_events":"https://pith.science/api/pith-number/VE3HLEFXIUZKNMQGKI2PV3UQ7I/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VE3HLEFXIUZKNMQGKI2PV3UQ7I/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VE3HLEFXIUZKNMQGKI2PV3UQ7I/action/storage_attestation","attest_author":"https://pith.science/pith/VE3HLEFXIUZKNMQGKI2PV3UQ7I/action/author_attestation","sign_citation":"https://pith.science/pith/VE3HLEFXIUZKNMQGKI2PV3UQ7I/action/citation_signature","submit_replication":"https://pith.science/pith/VE3HLEFXIUZKNMQGKI2PV3UQ7I/action/replication_record"}},"created_at":"2026-06-10T01:10:19.230046+00:00","updated_at":"2026-06-10T01:10:19.230046+00:00"}