{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:UPPQMX3LOXO633UTFCFYSZUFDC","short_pith_number":"pith:UPPQMX3L","schema_version":"1.0","canonical_sha256":"a3df065f6b75ddedee93288b89668518b64614c8949f4503967d37f678e93cdf","source":{"kind":"arxiv","id":"1010.3900","version":1},"attestation_state":"computed","paper":{"title":"Are back-to-back particle--antiparticle correlations observable in high energy nuclear collisions?","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Joern Knoll","submitted_at":"2010-10-19T13:19:30Z","abstract_excerpt":"Analytical formulae are presented which provide quantitative estimates for the suppression of the anticipated back-to-back particle--antiparticle correlations in high energy nuclear collisions due to the finite duration of the transition dynamics. They show that it is unlikely to observ the effect."},"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":"1010.3900","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-10-19T13:19:30Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"ed2d3c8b72a871972026cf45338aea496a5c9e80fa45bdf6be7c975e53cecc03","abstract_canon_sha256":"1975c90b1040537de9056d9b076b73f046066527cd988ada84bd21f1ec659c6c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:22:11.324476Z","signature_b64":"dc2Uf6w6G8N3e8ltvPzyHBpzsD9j0Z44B8jTClwlh9HjywNuJBk+tr0rQR3OcGMfppTzds6SloxeBHsjkoDbBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a3df065f6b75ddedee93288b89668518b64614c8949f4503967d37f678e93cdf","last_reissued_at":"2026-05-18T04:22:11.324059Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:22:11.324059Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Are back-to-back particle--antiparticle correlations observable in high energy nuclear collisions?","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Joern Knoll","submitted_at":"2010-10-19T13:19:30Z","abstract_excerpt":"Analytical formulae are presented which provide quantitative estimates for the suppression of the anticipated back-to-back particle--antiparticle correlations in high energy nuclear collisions due to the finite duration of the transition dynamics. They show that it is unlikely to observ the effect."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.3900","kind":"arxiv","version":1},"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":"1010.3900","created_at":"2026-05-18T04:22:11.324122+00:00"},{"alias_kind":"arxiv_version","alias_value":"1010.3900v1","created_at":"2026-05-18T04:22:11.324122+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.3900","created_at":"2026-05-18T04:22:11.324122+00:00"},{"alias_kind":"pith_short_12","alias_value":"UPPQMX3LOXO6","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_16","alias_value":"UPPQMX3LOXO633UT","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_8","alias_value":"UPPQMX3L","created_at":"2026-05-18T12:26:15.391820+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/UPPQMX3LOXO633UTFCFYSZUFDC","json":"https://pith.science/pith/UPPQMX3LOXO633UTFCFYSZUFDC.json","graph_json":"https://pith.science/api/pith-number/UPPQMX3LOXO633UTFCFYSZUFDC/graph.json","events_json":"https://pith.science/api/pith-number/UPPQMX3LOXO633UTFCFYSZUFDC/events.json","paper":"https://pith.science/paper/UPPQMX3L"},"agent_actions":{"view_html":"https://pith.science/pith/UPPQMX3LOXO633UTFCFYSZUFDC","download_json":"https://pith.science/pith/UPPQMX3LOXO633UTFCFYSZUFDC.json","view_paper":"https://pith.science/paper/UPPQMX3L","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1010.3900&json=true","fetch_graph":"https://pith.science/api/pith-number/UPPQMX3LOXO633UTFCFYSZUFDC/graph.json","fetch_events":"https://pith.science/api/pith-number/UPPQMX3LOXO633UTFCFYSZUFDC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UPPQMX3LOXO633UTFCFYSZUFDC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UPPQMX3LOXO633UTFCFYSZUFDC/action/storage_attestation","attest_author":"https://pith.science/pith/UPPQMX3LOXO633UTFCFYSZUFDC/action/author_attestation","sign_citation":"https://pith.science/pith/UPPQMX3LOXO633UTFCFYSZUFDC/action/citation_signature","submit_replication":"https://pith.science/pith/UPPQMX3LOXO633UTFCFYSZUFDC/action/replication_record"}},"created_at":"2026-05-18T04:22:11.324122+00:00","updated_at":"2026-05-18T04:22:11.324122+00:00"}