{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:XXOFYYPPRWUQO3IUDS2YHZGCPH","short_pith_number":"pith:XXOFYYPP","schema_version":"1.0","canonical_sha256":"bddc5c61ef8da9076d141cb583e4c279ccc45fbe05d57b98fa4db30e887461e7","source":{"kind":"arxiv","id":"2405.03174","version":2},"attestation_state":"computed","paper":{"title":"Beam energy dependence of transverse momentum distribution and elliptic flow in Au-Au collisions using HYDJET++ model","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"B. K. Singh, Saraswati Pandey, Satya Ranjan Nayak","submitted_at":"2024-05-06T05:51:06Z","abstract_excerpt":"In this work, we present the particle ratios, transverse momentum spectra, and elliptic flow ($v_2$) of $\\pi^\\pm,k^\\pm,$ $p$, and $\\bar{p}$ in Au-Au collisions at $\\sqrt{s_{NN}}=$ 62.4, 39.0, 27.0, 19.6 and 11.5 GeV using HYDJET++ model. The particle ratios match the experimental data that validates the Cleymans-Reidlich parameterization of freeze-out parameters at lower beam energies under the HYDJET++ framework. The lower collision energies produce a system of high baryon chemical potential ($\\mu_B$) and have a lower inelastic cross section. The interplay between these effects affects the ov"},"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":"2405.03174","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-05-06T05:51:06Z","cross_cats_sorted":[],"title_canon_sha256":"c5413aa363d6fe51a956fe9595cd7c0b7d922671b3915d02478bbeb43dbb0405","abstract_canon_sha256":"d4e988e28dbf48a7253e302c83dcfe5f2b2d8ca79e27f6c3b07720bf8cb35830"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:02:10.795853Z","signature_b64":"mcPGdhWtJoA0v0Odwo2BGzyEDuXa+TastWoKtZBRPjTmc+3frOnEed+nM8skxNWMUvlwegrGZmXvpJx+lKArBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bddc5c61ef8da9076d141cb583e4c279ccc45fbe05d57b98fa4db30e887461e7","last_reissued_at":"2026-07-05T11:02:10.795401Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:02:10.795401Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Beam energy dependence of transverse momentum distribution and elliptic flow in Au-Au collisions using HYDJET++ model","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"B. K. Singh, Saraswati Pandey, Satya Ranjan Nayak","submitted_at":"2024-05-06T05:51:06Z","abstract_excerpt":"In this work, we present the particle ratios, transverse momentum spectra, and elliptic flow ($v_2$) of $\\pi^\\pm,k^\\pm,$ $p$, and $\\bar{p}$ in Au-Au collisions at $\\sqrt{s_{NN}}=$ 62.4, 39.0, 27.0, 19.6 and 11.5 GeV using HYDJET++ model. The particle ratios match the experimental data that validates the Cleymans-Reidlich parameterization of freeze-out parameters at lower beam energies under the HYDJET++ framework. The lower collision energies produce a system of high baryon chemical potential ($\\mu_B$) and have a lower inelastic cross section. The interplay between these effects affects the ov"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.03174","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2405.03174/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":"2405.03174","created_at":"2026-07-05T11:02:10.795459+00:00"},{"alias_kind":"arxiv_version","alias_value":"2405.03174v2","created_at":"2026-07-05T11:02:10.795459+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.03174","created_at":"2026-07-05T11:02:10.795459+00:00"},{"alias_kind":"pith_short_12","alias_value":"XXOFYYPPRWUQ","created_at":"2026-07-05T11:02:10.795459+00:00"},{"alias_kind":"pith_short_16","alias_value":"XXOFYYPPRWUQO3IU","created_at":"2026-07-05T11:02:10.795459+00:00"},{"alias_kind":"pith_short_8","alias_value":"XXOFYYPP","created_at":"2026-07-05T11:02:10.795459+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/XXOFYYPPRWUQO3IUDS2YHZGCPH","json":"https://pith.science/pith/XXOFYYPPRWUQO3IUDS2YHZGCPH.json","graph_json":"https://pith.science/api/pith-number/XXOFYYPPRWUQO3IUDS2YHZGCPH/graph.json","events_json":"https://pith.science/api/pith-number/XXOFYYPPRWUQO3IUDS2YHZGCPH/events.json","paper":"https://pith.science/paper/XXOFYYPP"},"agent_actions":{"view_html":"https://pith.science/pith/XXOFYYPPRWUQO3IUDS2YHZGCPH","download_json":"https://pith.science/pith/XXOFYYPPRWUQO3IUDS2YHZGCPH.json","view_paper":"https://pith.science/paper/XXOFYYPP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2405.03174&json=true","fetch_graph":"https://pith.science/api/pith-number/XXOFYYPPRWUQO3IUDS2YHZGCPH/graph.json","fetch_events":"https://pith.science/api/pith-number/XXOFYYPPRWUQO3IUDS2YHZGCPH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XXOFYYPPRWUQO3IUDS2YHZGCPH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XXOFYYPPRWUQO3IUDS2YHZGCPH/action/storage_attestation","attest_author":"https://pith.science/pith/XXOFYYPPRWUQO3IUDS2YHZGCPH/action/author_attestation","sign_citation":"https://pith.science/pith/XXOFYYPPRWUQO3IUDS2YHZGCPH/action/citation_signature","submit_replication":"https://pith.science/pith/XXOFYYPPRWUQO3IUDS2YHZGCPH/action/replication_record"}},"created_at":"2026-07-05T11:02:10.795459+00:00","updated_at":"2026-07-05T11:02:10.795459+00:00"}