{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:3LG2L6XVHFXVW2WEE4L7VYYN3Y","short_pith_number":"pith:3LG2L6XV","schema_version":"1.0","canonical_sha256":"dacda5faf5396f5b6ac42717fae30dde0af05edd4c1ca351f8be025fcbbc5e1f","source":{"kind":"arxiv","id":"2210.15617","version":2},"attestation_state":"computed","paper":{"title":"Light nuclei production in pp and pA collisions in the Baryon Canonical Ensemble","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Krzysztof Redlich, Lokesh Kumar, Natasha Sharma, Pok Man Lo","submitted_at":"2022-10-27T17:04:36Z","abstract_excerpt":"The increase in yields of light nuclei with charged particle multiplicity, as reported by the ALICE collaboration at CERN in p-p and p-Pb collisions at the LHC energy is investigated in the thermal hadron resonance gas model. The model is extended to account for exact baryon number conservation. The focus is on the production of protons, deuterons, $^3$He, and $^3_\\Lambda$H. A very good description of proton and deuteron yields is obtained as a function of charged particle multiplicity in the mid-rapidity region using the same fixed temperature as in central Pb-Pb collisions. The yields of lig"},"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":"2210.15617","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"nucl-th","submitted_at":"2022-10-27T17:04:36Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"8fdfcbca4ecd859c2554df6fedd3c397a5a378807ddeb97269b46d14e1a24072","abstract_canon_sha256":"1f6609bc4118c7faa48be6bc4370ae6da0e37460d73eda85252b7162eb8499b4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:08:52.356924Z","signature_b64":"R54YpYNvTecS7m45M/qSgBx89aTIDDBEIVFj9/m1GJ9cOZUlAXTkcVaElLat+yMx/Wr/E4ciSboGp9UxJw87BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dacda5faf5396f5b6ac42717fae30dde0af05edd4c1ca351f8be025fcbbc5e1f","last_reissued_at":"2026-07-05T06:08:52.356516Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:08:52.356516Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Light nuclei production in pp and pA collisions in the Baryon Canonical Ensemble","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Krzysztof Redlich, Lokesh Kumar, Natasha Sharma, Pok Man Lo","submitted_at":"2022-10-27T17:04:36Z","abstract_excerpt":"The increase in yields of light nuclei with charged particle multiplicity, as reported by the ALICE collaboration at CERN in p-p and p-Pb collisions at the LHC energy is investigated in the thermal hadron resonance gas model. The model is extended to account for exact baryon number conservation. The focus is on the production of protons, deuterons, $^3$He, and $^3_\\Lambda$H. A very good description of proton and deuteron yields is obtained as a function of charged particle multiplicity in the mid-rapidity region using the same fixed temperature as in central Pb-Pb collisions. The yields of lig"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2210.15617","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/2210.15617/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":"2210.15617","created_at":"2026-07-05T06:08:52.356573+00:00"},{"alias_kind":"arxiv_version","alias_value":"2210.15617v2","created_at":"2026-07-05T06:08:52.356573+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2210.15617","created_at":"2026-07-05T06:08:52.356573+00:00"},{"alias_kind":"pith_short_12","alias_value":"3LG2L6XVHFXV","created_at":"2026-07-05T06:08:52.356573+00:00"},{"alias_kind":"pith_short_16","alias_value":"3LG2L6XVHFXVW2WE","created_at":"2026-07-05T06:08:52.356573+00:00"},{"alias_kind":"pith_short_8","alias_value":"3LG2L6XV","created_at":"2026-07-05T06:08:52.356573+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.07949","citing_title":"Wave-Function Femtometry: Hypertriton - The Ultimate Halo Nucleus","ref_index":52,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3LG2L6XVHFXVW2WEE4L7VYYN3Y","json":"https://pith.science/pith/3LG2L6XVHFXVW2WEE4L7VYYN3Y.json","graph_json":"https://pith.science/api/pith-number/3LG2L6XVHFXVW2WEE4L7VYYN3Y/graph.json","events_json":"https://pith.science/api/pith-number/3LG2L6XVHFXVW2WEE4L7VYYN3Y/events.json","paper":"https://pith.science/paper/3LG2L6XV"},"agent_actions":{"view_html":"https://pith.science/pith/3LG2L6XVHFXVW2WEE4L7VYYN3Y","download_json":"https://pith.science/pith/3LG2L6XVHFXVW2WEE4L7VYYN3Y.json","view_paper":"https://pith.science/paper/3LG2L6XV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2210.15617&json=true","fetch_graph":"https://pith.science/api/pith-number/3LG2L6XVHFXVW2WEE4L7VYYN3Y/graph.json","fetch_events":"https://pith.science/api/pith-number/3LG2L6XVHFXVW2WEE4L7VYYN3Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3LG2L6XVHFXVW2WEE4L7VYYN3Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3LG2L6XVHFXVW2WEE4L7VYYN3Y/action/storage_attestation","attest_author":"https://pith.science/pith/3LG2L6XVHFXVW2WEE4L7VYYN3Y/action/author_attestation","sign_citation":"https://pith.science/pith/3LG2L6XVHFXVW2WEE4L7VYYN3Y/action/citation_signature","submit_replication":"https://pith.science/pith/3LG2L6XVHFXVW2WEE4L7VYYN3Y/action/replication_record"}},"created_at":"2026-07-05T06:08:52.356573+00:00","updated_at":"2026-07-05T06:08:52.356573+00:00"}