{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:LORGOQLT5XOHNADBAS7BR4I6PJ","short_pith_number":"pith:LORGOQLT","schema_version":"1.0","canonical_sha256":"5ba2674173eddc76806104be18f11e7a446e58cd36ed014aaadced125d3884b2","source":{"kind":"arxiv","id":"1812.05041","version":3},"attestation_state":"computed","paper":{"title":"Identified particle production in Xe+Xe collisions at $\\sqrt{s_{\\rm{NN}}}$ = 5.44 TeV using a multiphase transport model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Mohammed Younus, Raghunath Sahoo, Rutuparna Rath, Sudipan De, Sushanta Tripathy","submitted_at":"2018-12-12T17:25:36Z","abstract_excerpt":"Xe+Xe collisions at relativistic energies provide us with an opportunity to study a possible system with deconfined quarks and gluons, whose size is in between those produced by p+p and Pb+Pb collisions. In the present work, we have used AMPT transport model with nuclear deformation to study the identified particle production such as ($\\pi^{+}+\\pi^{-}$), (K$^{+}$+K$^{-}$), $\\rm{K}_{s}^0$, (p+$\\bar{\\rm{p}}$), $\\phi$ and ($\\Lambda + \\bar{\\Lambda}$) in Xe+Xe collisions at $\\sqrt{s_{\\rm NN}}$=5.44 TeV. We study the $p\\rm{_T}$-spectra, integrated yield, $p\\rm{_T}$-differential and $p\\rm{_T}$-integr"},"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":"1812.05041","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-12-12T17:25:36Z","cross_cats_sorted":["hep-ex","nucl-ex","nucl-th"],"title_canon_sha256":"2d7d9a10999206b8469631454d7d405f7fb2c67d34553321024c530b4ac3161d","abstract_canon_sha256":"107bc714d7ed87abd5654d28e14e9c799bf1048ad7586fd4e460b06c4c0bc1d0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:43:09.225981Z","signature_b64":"Yx1rGZRUgb+yPxrkToX8Ms5Chgc9zh6rqqDsZllgSJRLAWhfUp0M5znL34PuKkiw3kQm4QaG7GwntdnAcR0EAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5ba2674173eddc76806104be18f11e7a446e58cd36ed014aaadced125d3884b2","last_reissued_at":"2026-05-17T23:43:09.225451Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:43:09.225451Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Identified particle production in Xe+Xe collisions at $\\sqrt{s_{\\rm{NN}}}$ = 5.44 TeV using a multiphase transport model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Mohammed Younus, Raghunath Sahoo, Rutuparna Rath, Sudipan De, Sushanta Tripathy","submitted_at":"2018-12-12T17:25:36Z","abstract_excerpt":"Xe+Xe collisions at relativistic energies provide us with an opportunity to study a possible system with deconfined quarks and gluons, whose size is in between those produced by p+p and Pb+Pb collisions. In the present work, we have used AMPT transport model with nuclear deformation to study the identified particle production such as ($\\pi^{+}+\\pi^{-}$), (K$^{+}$+K$^{-}$), $\\rm{K}_{s}^0$, (p+$\\bar{\\rm{p}}$), $\\phi$ and ($\\Lambda + \\bar{\\Lambda}$) in Xe+Xe collisions at $\\sqrt{s_{\\rm NN}}$=5.44 TeV. We study the $p\\rm{_T}$-spectra, integrated yield, $p\\rm{_T}$-differential and $p\\rm{_T}$-integr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.05041","kind":"arxiv","version":3},"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":"1812.05041","created_at":"2026-05-17T23:43:09.225545+00:00"},{"alias_kind":"arxiv_version","alias_value":"1812.05041v3","created_at":"2026-05-17T23:43:09.225545+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.05041","created_at":"2026-05-17T23:43:09.225545+00:00"},{"alias_kind":"pith_short_12","alias_value":"LORGOQLT5XOH","created_at":"2026-05-18T12:32:37.024351+00:00"},{"alias_kind":"pith_short_16","alias_value":"LORGOQLT5XOHNADB","created_at":"2026-05-18T12:32:37.024351+00:00"},{"alias_kind":"pith_short_8","alias_value":"LORGOQLT","created_at":"2026-05-18T12:32:37.024351+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/LORGOQLT5XOHNADBAS7BR4I6PJ","json":"https://pith.science/pith/LORGOQLT5XOHNADBAS7BR4I6PJ.json","graph_json":"https://pith.science/api/pith-number/LORGOQLT5XOHNADBAS7BR4I6PJ/graph.json","events_json":"https://pith.science/api/pith-number/LORGOQLT5XOHNADBAS7BR4I6PJ/events.json","paper":"https://pith.science/paper/LORGOQLT"},"agent_actions":{"view_html":"https://pith.science/pith/LORGOQLT5XOHNADBAS7BR4I6PJ","download_json":"https://pith.science/pith/LORGOQLT5XOHNADBAS7BR4I6PJ.json","view_paper":"https://pith.science/paper/LORGOQLT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1812.05041&json=true","fetch_graph":"https://pith.science/api/pith-number/LORGOQLT5XOHNADBAS7BR4I6PJ/graph.json","fetch_events":"https://pith.science/api/pith-number/LORGOQLT5XOHNADBAS7BR4I6PJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LORGOQLT5XOHNADBAS7BR4I6PJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LORGOQLT5XOHNADBAS7BR4I6PJ/action/storage_attestation","attest_author":"https://pith.science/pith/LORGOQLT5XOHNADBAS7BR4I6PJ/action/author_attestation","sign_citation":"https://pith.science/pith/LORGOQLT5XOHNADBAS7BR4I6PJ/action/citation_signature","submit_replication":"https://pith.science/pith/LORGOQLT5XOHNADBAS7BR4I6PJ/action/replication_record"}},"created_at":"2026-05-17T23:43:09.225545+00:00","updated_at":"2026-05-17T23:43:09.225545+00:00"}