{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:YCWPAOC3WLHVO6TXI7WEW7ANRH","short_pith_number":"pith:YCWPAOC3","schema_version":"1.0","canonical_sha256":"c0acf0385bb2cf577a7747ec4b7c0d89ee5f9a5c4b1c34217f9fb51e107ac6de","source":{"kind":"arxiv","id":"2201.08096","version":2},"attestation_state":"computed","paper":{"title":"Fluidity of the system produced in relativistic pp and heavy-ion collisions: Hadron resonance gas model approach","license":"http://creativecommons.org/licenses/by-sa/4.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Captain R. Singh, Dushmanta Sahu, Jan-e Alam, Raghunath Sahoo, Ronald Scaria","submitted_at":"2022-01-20T09:56:54Z","abstract_excerpt":"We have estimated the dimensionless parameters such as Reynolds number ($Re$), Knudsen number ($Kn$) and Mach number ($Ma$) for a multi-hadron system by using the excluded volume hadron resonance gas (EVHRG) model along with Hagedorn mass spectrum to include higher resonances in the system. The size dependence of these parameters indicate that the system formed in proton+proton collisions may achieve thermal equilibrium making it unsuitable as a benchmark to analyze the properties of the system produced in heavy ion collisions at similar energies. While the magnitude of $Kn$ can be used to stu"},"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":"2201.08096","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"hep-ph","submitted_at":"2022-01-20T09:56:54Z","cross_cats_sorted":["hep-ex","nucl-ex","nucl-th"],"title_canon_sha256":"82fea33b3b1a1f9a8d0f0e718d76049da17a36eddb6973d8ec7eab70fda30c43","abstract_canon_sha256":"b6e9f74e64fe9c7063414321c61f6955dfa8135996ae647571b7d59f3310f03c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:24:23.079245Z","signature_b64":"S9epNVZUyW2BLfrbLM4pYm8Me+3h5Ch1M7P69zpBF4fKsoBpfVrdFa2lKFx/GXFhjIcG98/7k6j8t5Wu45lXBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c0acf0385bb2cf577a7747ec4b7c0d89ee5f9a5c4b1c34217f9fb51e107ac6de","last_reissued_at":"2026-07-05T06:24:23.078886Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:24:23.078886Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Fluidity of the system produced in relativistic pp and heavy-ion collisions: Hadron resonance gas model approach","license":"http://creativecommons.org/licenses/by-sa/4.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Captain R. Singh, Dushmanta Sahu, Jan-e Alam, Raghunath Sahoo, Ronald Scaria","submitted_at":"2022-01-20T09:56:54Z","abstract_excerpt":"We have estimated the dimensionless parameters such as Reynolds number ($Re$), Knudsen number ($Kn$) and Mach number ($Ma$) for a multi-hadron system by using the excluded volume hadron resonance gas (EVHRG) model along with Hagedorn mass spectrum to include higher resonances in the system. The size dependence of these parameters indicate that the system formed in proton+proton collisions may achieve thermal equilibrium making it unsuitable as a benchmark to analyze the properties of the system produced in heavy ion collisions at similar energies. While the magnitude of $Kn$ can be used to stu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2201.08096","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/2201.08096/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":"2201.08096","created_at":"2026-07-05T06:24:23.078943+00:00"},{"alias_kind":"arxiv_version","alias_value":"2201.08096v2","created_at":"2026-07-05T06:24:23.078943+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2201.08096","created_at":"2026-07-05T06:24:23.078943+00:00"},{"alias_kind":"pith_short_12","alias_value":"YCWPAOC3WLHV","created_at":"2026-07-05T06:24:23.078943+00:00"},{"alias_kind":"pith_short_16","alias_value":"YCWPAOC3WLHVO6TX","created_at":"2026-07-05T06:24:23.078943+00:00"},{"alias_kind":"pith_short_8","alias_value":"YCWPAOC3","created_at":"2026-07-05T06:24:23.078943+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/YCWPAOC3WLHVO6TXI7WEW7ANRH","json":"https://pith.science/pith/YCWPAOC3WLHVO6TXI7WEW7ANRH.json","graph_json":"https://pith.science/api/pith-number/YCWPAOC3WLHVO6TXI7WEW7ANRH/graph.json","events_json":"https://pith.science/api/pith-number/YCWPAOC3WLHVO6TXI7WEW7ANRH/events.json","paper":"https://pith.science/paper/YCWPAOC3"},"agent_actions":{"view_html":"https://pith.science/pith/YCWPAOC3WLHVO6TXI7WEW7ANRH","download_json":"https://pith.science/pith/YCWPAOC3WLHVO6TXI7WEW7ANRH.json","view_paper":"https://pith.science/paper/YCWPAOC3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2201.08096&json=true","fetch_graph":"https://pith.science/api/pith-number/YCWPAOC3WLHVO6TXI7WEW7ANRH/graph.json","fetch_events":"https://pith.science/api/pith-number/YCWPAOC3WLHVO6TXI7WEW7ANRH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YCWPAOC3WLHVO6TXI7WEW7ANRH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YCWPAOC3WLHVO6TXI7WEW7ANRH/action/storage_attestation","attest_author":"https://pith.science/pith/YCWPAOC3WLHVO6TXI7WEW7ANRH/action/author_attestation","sign_citation":"https://pith.science/pith/YCWPAOC3WLHVO6TXI7WEW7ANRH/action/citation_signature","submit_replication":"https://pith.science/pith/YCWPAOC3WLHVO6TXI7WEW7ANRH/action/replication_record"}},"created_at":"2026-07-05T06:24:23.078943+00:00","updated_at":"2026-07-05T06:24:23.078943+00:00"}