{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:35QQEKFMIYYBEEBN267PO7IVFY","short_pith_number":"pith:35QQEKFM","schema_version":"1.0","canonical_sha256":"df610228ac463012102dd7bef77d152e3eea3d5c2865640ada9b05b96a36eb28","source":{"kind":"arxiv","id":"1512.07227","version":2},"attestation_state":"computed","paper":{"title":"Multi-strange baryon production in p-Pb collisions at $\\sqrt{s_\\mathbf{NN}}=5.02$ TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"nucl-ex","authors_text":"ALICE Collaboration","submitted_at":"2015-12-22T20:21:32Z","abstract_excerpt":"The multi-strange baryon yields in Pb--Pb collisions have been shown to exhibit an enhancement relative to pp reactions. In this work, $\\Xi$ and $\\Omega$ production rates have been measured with the ALICE experiment as a function of transverse momentum, ${p_{\\rm T}}$, in p-Pb collisions at a centre-of-mass energy of ${\\sqrt{s_{\\rm NN}}}$ = 5.02 TeV. The results cover the kinematic ranges 0.6 GeV/$c<{p_{\\rm T}} <$7.2 GeV/$c$ and 0.8 GeV/$c<{p_{\\rm T}}<$ 5 GeV/$c$, for $\\Xi$ and $\\Omega$ respectively, in the common rapidity interval -0.5 $<{y_{\\rm CMS}}<$ 0. Multi-strange baryons have been ident"},"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":"1512.07227","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-ex","submitted_at":"2015-12-22T20:21:32Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"3146bbbbe8218cbd40ec2d9ffe6782c906d0efb41d36fa98434d0075b93f2b85","abstract_canon_sha256":"dba80603e6cdc43ca5d973276f7b3442429c73d1d46ee3546f2032626cdd3e55"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:23:02.110287Z","signature_b64":"J09YuHGmi1AzzzN47b9U6AdLttLjy6aMNskpok570+ZNftyb6ujKOGJhP6ISH4zR+GdWoeK+gUxW4NZuoDeKCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"df610228ac463012102dd7bef77d152e3eea3d5c2865640ada9b05b96a36eb28","last_reissued_at":"2026-05-18T01:23:02.109418Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:23:02.109418Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Multi-strange baryon production in p-Pb collisions at $\\sqrt{s_\\mathbf{NN}}=5.02$ TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"nucl-ex","authors_text":"ALICE Collaboration","submitted_at":"2015-12-22T20:21:32Z","abstract_excerpt":"The multi-strange baryon yields in Pb--Pb collisions have been shown to exhibit an enhancement relative to pp reactions. In this work, $\\Xi$ and $\\Omega$ production rates have been measured with the ALICE experiment as a function of transverse momentum, ${p_{\\rm T}}$, in p-Pb collisions at a centre-of-mass energy of ${\\sqrt{s_{\\rm NN}}}$ = 5.02 TeV. The results cover the kinematic ranges 0.6 GeV/$c<{p_{\\rm T}} <$7.2 GeV/$c$ and 0.8 GeV/$c<{p_{\\rm T}}<$ 5 GeV/$c$, for $\\Xi$ and $\\Omega$ respectively, in the common rapidity interval -0.5 $<{y_{\\rm CMS}}<$ 0. Multi-strange baryons have been ident"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1512.07227","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":""},"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":"1512.07227","created_at":"2026-05-18T01:23:02.109561+00:00"},{"alias_kind":"arxiv_version","alias_value":"1512.07227v2","created_at":"2026-05-18T01:23:02.109561+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1512.07227","created_at":"2026-05-18T01:23:02.109561+00:00"},{"alias_kind":"pith_short_12","alias_value":"35QQEKFMIYYB","created_at":"2026-05-18T12:29:02.477457+00:00"},{"alias_kind":"pith_short_16","alias_value":"35QQEKFMIYYBEEBN","created_at":"2026-05-18T12:29:02.477457+00:00"},{"alias_kind":"pith_short_8","alias_value":"35QQEKFM","created_at":"2026-05-18T12:29:02.477457+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.01762","citing_title":"Transverse momentum dependence of $\\Omega/\\phi$ ratio in high energy collisions","ref_index":57,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/35QQEKFMIYYBEEBN267PO7IVFY","json":"https://pith.science/pith/35QQEKFMIYYBEEBN267PO7IVFY.json","graph_json":"https://pith.science/api/pith-number/35QQEKFMIYYBEEBN267PO7IVFY/graph.json","events_json":"https://pith.science/api/pith-number/35QQEKFMIYYBEEBN267PO7IVFY/events.json","paper":"https://pith.science/paper/35QQEKFM"},"agent_actions":{"view_html":"https://pith.science/pith/35QQEKFMIYYBEEBN267PO7IVFY","download_json":"https://pith.science/pith/35QQEKFMIYYBEEBN267PO7IVFY.json","view_paper":"https://pith.science/paper/35QQEKFM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1512.07227&json=true","fetch_graph":"https://pith.science/api/pith-number/35QQEKFMIYYBEEBN267PO7IVFY/graph.json","fetch_events":"https://pith.science/api/pith-number/35QQEKFMIYYBEEBN267PO7IVFY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/35QQEKFMIYYBEEBN267PO7IVFY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/35QQEKFMIYYBEEBN267PO7IVFY/action/storage_attestation","attest_author":"https://pith.science/pith/35QQEKFMIYYBEEBN267PO7IVFY/action/author_attestation","sign_citation":"https://pith.science/pith/35QQEKFMIYYBEEBN267PO7IVFY/action/citation_signature","submit_replication":"https://pith.science/pith/35QQEKFMIYYBEEBN267PO7IVFY/action/replication_record"}},"created_at":"2026-05-18T01:23:02.109561+00:00","updated_at":"2026-05-18T01:23:02.109561+00:00"}