{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:OG5FP5L2EC4242MKQDFDQ4AVK7","short_pith_number":"pith:OG5FP5L2","schema_version":"1.0","canonical_sha256":"71ba57f57a20b9ae698a80ca38701557e7907fbc8bad04ddeaef20cf8679d4c6","source":{"kind":"arxiv","id":"1311.7508","version":1},"attestation_state":"computed","paper":{"title":"Thermal Description of Particle Production in Au-Au Collisions at STAR Energies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"A. Tawfik (Egyptian Ctr. Theor. Phys., Cairo, Cairo), E. Abbas (Egyptian Ctr. Theor. Phys., WLCAPP","submitted_at":"2013-11-29T10:02:42Z","abstract_excerpt":"The hadron ratios measured in central Au-Au collisions are analysed by means of Hadron Resonance Gas (HRG) model over a wide range of nucleon-nucleon center-of-mass energies ranging from 7.7 to 200 GeV as offered by the STAR Beam Energy Scan I (BES-I). We restrict the discussion on STAR BES-I, because of large statistics and over all homogeneity of STAR measurements (one detector) against previous experiments. Over the last three decades, various heavy-ion experiments utilizing different detectors (different certainties) have been carried out. Regularities in produced particles at different en"},"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":"1311.7508","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-11-29T10:02:42Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"865a3cabd7859b7f0692dd2aa35ad9971a952e13a274663fd696ea8ba3b17bfb","abstract_canon_sha256":"c9f24ca1bbf37cd446b4e5acfedf9a33aa00426bbe4db6ddc3726f96575a9e22"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:05:56.007947Z","signature_b64":"LRQ1yH678GoccL/OUwg+5sZL32vq45JyIfWF4DtK9PMYYuExWKq/P9bM9QgJULEKcD+H43WRanHupvdcQT/cAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"71ba57f57a20b9ae698a80ca38701557e7907fbc8bad04ddeaef20cf8679d4c6","last_reissued_at":"2026-05-18T03:05:56.007290Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:05:56.007290Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermal Description of Particle Production in Au-Au Collisions at STAR Energies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"A. Tawfik (Egyptian Ctr. Theor. Phys., Cairo, Cairo), E. Abbas (Egyptian Ctr. Theor. Phys., WLCAPP","submitted_at":"2013-11-29T10:02:42Z","abstract_excerpt":"The hadron ratios measured in central Au-Au collisions are analysed by means of Hadron Resonance Gas (HRG) model over a wide range of nucleon-nucleon center-of-mass energies ranging from 7.7 to 200 GeV as offered by the STAR Beam Energy Scan I (BES-I). We restrict the discussion on STAR BES-I, because of large statistics and over all homogeneity of STAR measurements (one detector) against previous experiments. Over the last three decades, various heavy-ion experiments utilizing different detectors (different certainties) have been carried out. Regularities in produced particles at different en"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.7508","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":"1311.7508","created_at":"2026-05-18T03:05:56.007378+00:00"},{"alias_kind":"arxiv_version","alias_value":"1311.7508v1","created_at":"2026-05-18T03:05:56.007378+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.7508","created_at":"2026-05-18T03:05:56.007378+00:00"},{"alias_kind":"pith_short_12","alias_value":"OG5FP5L2EC42","created_at":"2026-05-18T12:27:54.935989+00:00"},{"alias_kind":"pith_short_16","alias_value":"OG5FP5L2EC4242MK","created_at":"2026-05-18T12:27:54.935989+00:00"},{"alias_kind":"pith_short_8","alias_value":"OG5FP5L2","created_at":"2026-05-18T12:27:54.935989+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/OG5FP5L2EC4242MKQDFDQ4AVK7","json":"https://pith.science/pith/OG5FP5L2EC4242MKQDFDQ4AVK7.json","graph_json":"https://pith.science/api/pith-number/OG5FP5L2EC4242MKQDFDQ4AVK7/graph.json","events_json":"https://pith.science/api/pith-number/OG5FP5L2EC4242MKQDFDQ4AVK7/events.json","paper":"https://pith.science/paper/OG5FP5L2"},"agent_actions":{"view_html":"https://pith.science/pith/OG5FP5L2EC4242MKQDFDQ4AVK7","download_json":"https://pith.science/pith/OG5FP5L2EC4242MKQDFDQ4AVK7.json","view_paper":"https://pith.science/paper/OG5FP5L2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1311.7508&json=true","fetch_graph":"https://pith.science/api/pith-number/OG5FP5L2EC4242MKQDFDQ4AVK7/graph.json","fetch_events":"https://pith.science/api/pith-number/OG5FP5L2EC4242MKQDFDQ4AVK7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OG5FP5L2EC4242MKQDFDQ4AVK7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OG5FP5L2EC4242MKQDFDQ4AVK7/action/storage_attestation","attest_author":"https://pith.science/pith/OG5FP5L2EC4242MKQDFDQ4AVK7/action/author_attestation","sign_citation":"https://pith.science/pith/OG5FP5L2EC4242MKQDFDQ4AVK7/action/citation_signature","submit_replication":"https://pith.science/pith/OG5FP5L2EC4242MKQDFDQ4AVK7/action/replication_record"}},"created_at":"2026-05-18T03:05:56.007378+00:00","updated_at":"2026-05-18T03:05:56.007378+00:00"}