{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:BKHKIVVGDKDKILGSO375PQZ5WG","short_pith_number":"pith:BKHKIVVG","schema_version":"1.0","canonical_sha256":"0a8ea456a61a86a42cd276ffd7c33db18cb07f99f597a523904084061cedfbd7","source":{"kind":"arxiv","id":"1303.0155","version":2},"attestation_state":"computed","paper":{"title":"N-person quantum Russian roulette","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Alexandre G M Schmidt, Piotr Frackiewicz","submitted_at":"2013-03-01T12:45:16Z","abstract_excerpt":"We generalize the concept of quantum Russian roulette introduced in [A.G.M. Schmidt, L. da Silva, Physica A 392 (2013) 400-410]. Our model coincides with the previous one in the case of the game with two players and gives the suitable quantum description for any finite number of players."},"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":"1303.0155","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-03-01T12:45:16Z","cross_cats_sorted":[],"title_canon_sha256":"b5a718d6dd352ff0ab29568ee9a7d634b32a1b657e3673b5207d9803a6bbfe20","abstract_canon_sha256":"4082f2b08f697cecb776ac4b03d329316afaa3dd618bd4975a36091b3d4a08a2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:29:29.237109Z","signature_b64":"e8x1F3JhSfq9Vcbrw2Cl3Q2vbXX81fYEkMPo6XR42DbpX/jZ+cESbEjTZ1X7RDEyiOap3yj89w1exTIzT2QGAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0a8ea456a61a86a42cd276ffd7c33db18cb07f99f597a523904084061cedfbd7","last_reissued_at":"2026-05-18T03:29:29.236273Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:29:29.236273Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"N-person quantum Russian roulette","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Alexandre G M Schmidt, Piotr Frackiewicz","submitted_at":"2013-03-01T12:45:16Z","abstract_excerpt":"We generalize the concept of quantum Russian roulette introduced in [A.G.M. Schmidt, L. da Silva, Physica A 392 (2013) 400-410]. Our model coincides with the previous one in the case of the game with two players and gives the suitable quantum description for any finite number of players."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.0155","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":"1303.0155","created_at":"2026-05-18T03:29:29.236429+00:00"},{"alias_kind":"arxiv_version","alias_value":"1303.0155v2","created_at":"2026-05-18T03:29:29.236429+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.0155","created_at":"2026-05-18T03:29:29.236429+00:00"},{"alias_kind":"pith_short_12","alias_value":"BKHKIVVGDKDK","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_16","alias_value":"BKHKIVVGDKDKILGS","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_8","alias_value":"BKHKIVVG","created_at":"2026-05-18T12:27:38.830355+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/BKHKIVVGDKDKILGSO375PQZ5WG","json":"https://pith.science/pith/BKHKIVVGDKDKILGSO375PQZ5WG.json","graph_json":"https://pith.science/api/pith-number/BKHKIVVGDKDKILGSO375PQZ5WG/graph.json","events_json":"https://pith.science/api/pith-number/BKHKIVVGDKDKILGSO375PQZ5WG/events.json","paper":"https://pith.science/paper/BKHKIVVG"},"agent_actions":{"view_html":"https://pith.science/pith/BKHKIVVGDKDKILGSO375PQZ5WG","download_json":"https://pith.science/pith/BKHKIVVGDKDKILGSO375PQZ5WG.json","view_paper":"https://pith.science/paper/BKHKIVVG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1303.0155&json=true","fetch_graph":"https://pith.science/api/pith-number/BKHKIVVGDKDKILGSO375PQZ5WG/graph.json","fetch_events":"https://pith.science/api/pith-number/BKHKIVVGDKDKILGSO375PQZ5WG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BKHKIVVGDKDKILGSO375PQZ5WG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BKHKIVVGDKDKILGSO375PQZ5WG/action/storage_attestation","attest_author":"https://pith.science/pith/BKHKIVVGDKDKILGSO375PQZ5WG/action/author_attestation","sign_citation":"https://pith.science/pith/BKHKIVVGDKDKILGSO375PQZ5WG/action/citation_signature","submit_replication":"https://pith.science/pith/BKHKIVVGDKDKILGSO375PQZ5WG/action/replication_record"}},"created_at":"2026-05-18T03:29:29.236429+00:00","updated_at":"2026-05-18T03:29:29.236429+00:00"}