{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:FZEDTT7ZAJQKFG77UF7YXJX3LT","short_pith_number":"pith:FZEDTT7Z","canonical_record":{"source":{"id":"1609.04811","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2016-09-15T12:45:36Z","cross_cats_sorted":[],"title_canon_sha256":"34f159a1db9db01cc61f1e78020cc7b0c29870f7081cb638c412a76125a6de4c","abstract_canon_sha256":"aa68b613d2a594bb4185ed685f237f30ba553469b46552df8981623a83e26797"},"schema_version":"1.0"},"canonical_sha256":"2e4839cff90260a29bffa17f8ba6fb5cc80bd0662c11a274b388ae6d93ee52b1","source":{"kind":"arxiv","id":"1609.04811","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1609.04811","created_at":"2026-05-18T00:50:04Z"},{"alias_kind":"arxiv_version","alias_value":"1609.04811v2","created_at":"2026-05-18T00:50:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.04811","created_at":"2026-05-18T00:50:04Z"},{"alias_kind":"pith_short_12","alias_value":"FZEDTT7ZAJQK","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_16","alias_value":"FZEDTT7ZAJQKFG77","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_8","alias_value":"FZEDTT7Z","created_at":"2026-05-18T12:30:15Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:FZEDTT7ZAJQKFG77UF7YXJX3LT","target":"record","payload":{"canonical_record":{"source":{"id":"1609.04811","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2016-09-15T12:45:36Z","cross_cats_sorted":[],"title_canon_sha256":"34f159a1db9db01cc61f1e78020cc7b0c29870f7081cb638c412a76125a6de4c","abstract_canon_sha256":"aa68b613d2a594bb4185ed685f237f30ba553469b46552df8981623a83e26797"},"schema_version":"1.0"},"canonical_sha256":"2e4839cff90260a29bffa17f8ba6fb5cc80bd0662c11a274b388ae6d93ee52b1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:50:04.238075Z","signature_b64":"J6QNe1ktc3mjaARq+SkQH7ycHho8RcKqG9jK3T9mnGT6d0f0+J8LpwQS6WkNHX3qbKqzClVL9blfK28nJgZXBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2e4839cff90260a29bffa17f8ba6fb5cc80bd0662c11a274b388ae6d93ee52b1","last_reissued_at":"2026-05-18T00:50:04.237150Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:50:04.237150Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1609.04811","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:50:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cmG2hRnslBSuJebNpm3LJd2NIgtGwoPZb71WFMO8/AKaPvicDIQZv5Z3WYT5sxKL08xenakdTWsF6nx929AMCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T01:21:02.098049Z"},"content_sha256":"ef3ac0e5042252cdf2ec21d17a3558f26fb8ceef920d72cba50131283fd76160","schema_version":"1.0","event_id":"sha256:ef3ac0e5042252cdf2ec21d17a3558f26fb8ceef920d72cba50131283fd76160"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:FZEDTT7ZAJQKFG77UF7YXJX3LT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Spin-parity effect in violation of bell's inequalities for entangled states of parallel polarization","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Haifeng Zhang, Jianhua Wang, J.-Q. Liang, L.-F.Wei, Zhigang Song","submitted_at":"2016-09-15T12:45:36Z","abstract_excerpt":"Bell inequalities (BIs) derived in terms of quantum probability statistics are extended to general bipartite-entangled states of arbitrary spins with parallel polarization. The original formula of Bell for the two-spin singlet is slightly modified in the parallel configuration, while, the inequality for- mulated by Clauser-Horne-Shimony-Holt remains not changed. The violation of BIs indeed resulted from the quantum non-local correlation for spin-1=2 case. However, the inequalities are always satisfied for the spin-1 entangled states regardless of parallel or antiparallel polarizations of two s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.04811","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:50:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9IggU6zDjfTX+tZQI0Yy2bd6nJZEXgCT6wqVb7l8vpXDgr4BMvLHpglmGfP9bcKMtqmj71sKmrMkP3y0O4zQBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T01:21:02.098582Z"},"content_sha256":"60dd65fde90bba979ff9e73a942b5431e58d64a2f0324de686d9710e15d44ac4","schema_version":"1.0","event_id":"sha256:60dd65fde90bba979ff9e73a942b5431e58d64a2f0324de686d9710e15d44ac4"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FZEDTT7ZAJQKFG77UF7YXJX3LT/bundle.json","state_url":"https://pith.science/pith/FZEDTT7ZAJQKFG77UF7YXJX3LT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FZEDTT7ZAJQKFG77UF7YXJX3LT/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-06T01:21:02Z","links":{"resolver":"https://pith.science/pith/FZEDTT7ZAJQKFG77UF7YXJX3LT","bundle":"https://pith.science/pith/FZEDTT7ZAJQKFG77UF7YXJX3LT/bundle.json","state":"https://pith.science/pith/FZEDTT7ZAJQKFG77UF7YXJX3LT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FZEDTT7ZAJQKFG77UF7YXJX3LT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:FZEDTT7ZAJQKFG77UF7YXJX3LT","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"aa68b613d2a594bb4185ed685f237f30ba553469b46552df8981623a83e26797","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2016-09-15T12:45:36Z","title_canon_sha256":"34f159a1db9db01cc61f1e78020cc7b0c29870f7081cb638c412a76125a6de4c"},"schema_version":"1.0","source":{"id":"1609.04811","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1609.04811","created_at":"2026-05-18T00:50:04Z"},{"alias_kind":"arxiv_version","alias_value":"1609.04811v2","created_at":"2026-05-18T00:50:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.04811","created_at":"2026-05-18T00:50:04Z"},{"alias_kind":"pith_short_12","alias_value":"FZEDTT7ZAJQK","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_16","alias_value":"FZEDTT7ZAJQKFG77","created_at":"2026-05-18T12:30:15Z"},{"alias_kind":"pith_short_8","alias_value":"FZEDTT7Z","created_at":"2026-05-18T12:30:15Z"}],"graph_snapshots":[{"event_id":"sha256:60dd65fde90bba979ff9e73a942b5431e58d64a2f0324de686d9710e15d44ac4","target":"graph","created_at":"2026-05-18T00:50:04Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"Bell inequalities (BIs) derived in terms of quantum probability statistics are extended to general bipartite-entangled states of arbitrary spins with parallel polarization. The original formula of Bell for the two-spin singlet is slightly modified in the parallel configuration, while, the inequality for- mulated by Clauser-Horne-Shimony-Holt remains not changed. The violation of BIs indeed resulted from the quantum non-local correlation for spin-1=2 case. However, the inequalities are always satisfied for the spin-1 entangled states regardless of parallel or antiparallel polarizations of two s","authors_text":"Haifeng Zhang, Jianhua Wang, J.-Q. Liang, L.-F.Wei, Zhigang Song","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2016-09-15T12:45:36Z","title":"Spin-parity effect in violation of bell's inequalities for entangled states of parallel polarization"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.04811","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:ef3ac0e5042252cdf2ec21d17a3558f26fb8ceef920d72cba50131283fd76160","target":"record","created_at":"2026-05-18T00:50:04Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"aa68b613d2a594bb4185ed685f237f30ba553469b46552df8981623a83e26797","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2016-09-15T12:45:36Z","title_canon_sha256":"34f159a1db9db01cc61f1e78020cc7b0c29870f7081cb638c412a76125a6de4c"},"schema_version":"1.0","source":{"id":"1609.04811","kind":"arxiv","version":2}},"canonical_sha256":"2e4839cff90260a29bffa17f8ba6fb5cc80bd0662c11a274b388ae6d93ee52b1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2e4839cff90260a29bffa17f8ba6fb5cc80bd0662c11a274b388ae6d93ee52b1","first_computed_at":"2026-05-18T00:50:04.237150Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:50:04.237150Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"J6QNe1ktc3mjaARq+SkQH7ycHho8RcKqG9jK3T9mnGT6d0f0+J8LpwQS6WkNHX3qbKqzClVL9blfK28nJgZXBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:50:04.238075Z","signed_message":"canonical_sha256_bytes"},"source_id":"1609.04811","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ef3ac0e5042252cdf2ec21d17a3558f26fb8ceef920d72cba50131283fd76160","sha256:60dd65fde90bba979ff9e73a942b5431e58d64a2f0324de686d9710e15d44ac4"],"state_sha256":"9b6611187dcb41954018d554010882cc6e188a196a32810f6ee232003638005b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RXVvsT4RUXJtbyp9mBtRZARZ3k2HxZjnC+UidAl+RjrqBU6OZlc1/ikbgY9gn+u8S1Qlm4GimdgjXmI+PE4lBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-06T01:21:02.101910Z","bundle_sha256":"7f87fb67283a1668adf6ae223379b1a67a445082f69a40913b5b6316f16993a5"}}