{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:73CQWYKDUGTDDXB53GDXY7FCQZ","short_pith_number":"pith:73CQWYKD","schema_version":"1.0","canonical_sha256":"fec50b6143a1a631dc3dd9877c7ca2867e6b567b47f3e358662ee4b82caa08e7","source":{"kind":"arxiv","id":"2508.21477","version":1},"attestation_state":"computed","paper":{"title":"SMASH: Results from hadronic transport for heavy-ion collisions at high densities","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"Hannah Elfner, Renan G\\'oes-Hirayama","submitted_at":"2025-08-29T10:01:42Z","abstract_excerpt":"This mini-review summarizes the general setup and some highlight results from the hadronic transport approach SMASH (Simulating Many Accelerated Strongly-interacting Hadrons). We start by laying out the software development structures as well as the particle properties and how they are determined by elementary collisions. The different ways to produce light clusters in SMASH, either by coalescence or dynamic multi-particle reactions, are explained. The constraints on nuclear mean fields and the corresponding equation of state from collective flow observables are discussed. In addition, we show"},"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":"2508.21477","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2025-08-29T10:01:42Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"f098e75a649da45a45e71fcc25d76467afaa53c1e7b9302735764916e2aa2221","abstract_canon_sha256":"ca10e6ccbaa9d038d185fac7b9a1d64e6a068b7321e80f8d2a46efc9ab28a12b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T12:01:35.481571Z","signature_b64":"L70VEpiSAMf6RItRiYD+YhpJuC+If+3yQKm8Fd2wxR9Isb+JUsWtSM/dD5oYIA6fw/YIUEtX91/TiEb8wEY8AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fec50b6143a1a631dc3dd9877c7ca2867e6b567b47f3e358662ee4b82caa08e7","last_reissued_at":"2026-07-05T12:01:35.481045Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T12:01:35.481045Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"SMASH: Results from hadronic transport for heavy-ion collisions at high densities","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"Hannah Elfner, Renan G\\'oes-Hirayama","submitted_at":"2025-08-29T10:01:42Z","abstract_excerpt":"This mini-review summarizes the general setup and some highlight results from the hadronic transport approach SMASH (Simulating Many Accelerated Strongly-interacting Hadrons). We start by laying out the software development structures as well as the particle properties and how they are determined by elementary collisions. The different ways to produce light clusters in SMASH, either by coalescence or dynamic multi-particle reactions, are explained. The constraints on nuclear mean fields and the corresponding equation of state from collective flow observables are discussed. In addition, we show"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2508.21477","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/2508.21477/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":"2508.21477","created_at":"2026-07-05T12:01:35.481100+00:00"},{"alias_kind":"arxiv_version","alias_value":"2508.21477v1","created_at":"2026-07-05T12:01:35.481100+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2508.21477","created_at":"2026-07-05T12:01:35.481100+00:00"},{"alias_kind":"pith_short_12","alias_value":"73CQWYKDUGTD","created_at":"2026-07-05T12:01:35.481100+00:00"},{"alias_kind":"pith_short_16","alias_value":"73CQWYKDUGTDDXB5","created_at":"2026-07-05T12:01:35.481100+00:00"},{"alias_kind":"pith_short_8","alias_value":"73CQWYKD","created_at":"2026-07-05T12:01:35.481100+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.26326","citing_title":"Studying the QCD Matter produced in Heavy-Ion Collisions using the MUSES Calculation Engine","ref_index":282,"is_internal_anchor":false},{"citing_arxiv_id":"2605.16914","citing_title":"3D Initial-State Dynamics across scales: A Comparative Study of saturation and string-based descriptions","ref_index":18,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/73CQWYKDUGTDDXB53GDXY7FCQZ","json":"https://pith.science/pith/73CQWYKDUGTDDXB53GDXY7FCQZ.json","graph_json":"https://pith.science/api/pith-number/73CQWYKDUGTDDXB53GDXY7FCQZ/graph.json","events_json":"https://pith.science/api/pith-number/73CQWYKDUGTDDXB53GDXY7FCQZ/events.json","paper":"https://pith.science/paper/73CQWYKD"},"agent_actions":{"view_html":"https://pith.science/pith/73CQWYKDUGTDDXB53GDXY7FCQZ","download_json":"https://pith.science/pith/73CQWYKDUGTDDXB53GDXY7FCQZ.json","view_paper":"https://pith.science/paper/73CQWYKD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2508.21477&json=true","fetch_graph":"https://pith.science/api/pith-number/73CQWYKDUGTDDXB53GDXY7FCQZ/graph.json","fetch_events":"https://pith.science/api/pith-number/73CQWYKDUGTDDXB53GDXY7FCQZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/73CQWYKDUGTDDXB53GDXY7FCQZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/73CQWYKDUGTDDXB53GDXY7FCQZ/action/storage_attestation","attest_author":"https://pith.science/pith/73CQWYKDUGTDDXB53GDXY7FCQZ/action/author_attestation","sign_citation":"https://pith.science/pith/73CQWYKDUGTDDXB53GDXY7FCQZ/action/citation_signature","submit_replication":"https://pith.science/pith/73CQWYKDUGTDDXB53GDXY7FCQZ/action/replication_record"}},"created_at":"2026-07-05T12:01:35.481100+00:00","updated_at":"2026-07-05T12:01:35.481100+00:00"}