{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:OKA57UAWVP6V4KAYYZJ2TTT7NA","short_pith_number":"pith:OKA57UAW","canonical_record":{"source":{"id":"2608.08215","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2026-08-08T16:22:31Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"93a9f5d56b0adbc8c2e7bc7acea13b5c7e00cd5a054a7ebfc64bfdb1a3d1bafd","abstract_canon_sha256":"8dccc8292ea1feea06b088e72e82f1ce5fe772cbf1b6704722be3f35634c7b67"},"schema_version":"1.0"},"canonical_sha256":"7281dfd016abfd5e2818c653a9ce7f68090a11e10c62f39d78a34f2187559617","source":{"kind":"arxiv","id":"2608.08215","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2608.08215","created_at":"2026-08-11T01:22:00Z"},{"alias_kind":"arxiv_version","alias_value":"2608.08215v1","created_at":"2026-08-11T01:22:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2608.08215","created_at":"2026-08-11T01:22:00Z"},{"alias_kind":"pith_short_12","alias_value":"OKA57UAWVP6V","created_at":"2026-08-11T01:22:00Z"},{"alias_kind":"pith_short_16","alias_value":"OKA57UAWVP6V4KAY","created_at":"2026-08-11T01:22:00Z"},{"alias_kind":"pith_short_8","alias_value":"OKA57UAW","created_at":"2026-08-11T01:22:00Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:OKA57UAWVP6V4KAYYZJ2TTT7NA","target":"record","payload":{"canonical_record":{"source":{"id":"2608.08215","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2026-08-08T16:22:31Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"93a9f5d56b0adbc8c2e7bc7acea13b5c7e00cd5a054a7ebfc64bfdb1a3d1bafd","abstract_canon_sha256":"8dccc8292ea1feea06b088e72e82f1ce5fe772cbf1b6704722be3f35634c7b67"},"schema_version":"1.0"},"canonical_sha256":"7281dfd016abfd5e2818c653a9ce7f68090a11e10c62f39d78a34f2187559617","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-08-11T01:22:00.449529Z","signature_b64":"ZUGLYD3qIgPhoKA3AMNvMrM2GXMNcQfXSHAlHYrpT6n0I1qD9m6X951tM4skTPcpbqMp33SQrRQOOTgTMJCwCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7281dfd016abfd5e2818c653a9ce7f68090a11e10c62f39d78a34f2187559617","last_reissued_at":"2026-08-11T01:22:00.447187Z","signature_status":"signed_v1","first_computed_at":"2026-08-11T01:22:00.447187Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2608.08215","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-11T01:22:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GbmqKyou/G849ge/Vgzw7UAg8FYV+nNgqdQriX64SjMk0vE40Rrv3ZAEZqVf1XFpslnGUoYMaFCLohemw8CkAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T19:33:29.731520Z"},"content_sha256":"cf10a4301a6c5384d80b528a16063f41d684f408faaf9449129fc5c797298c95","schema_version":"1.0","event_id":"sha256:cf10a4301a6c5384d80b528a16063f41d684f408faaf9449129fc5c797298c95"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:OKA57UAWVP6V4KAYYZJ2TTT7NA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Opposite post-processing orders of fermionic horizon channels and their quantum-resource monotonicity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"quant-ph","authors_text":"Jin-Ming Liu, Shuhao Li","submitted_at":"2026-08-08T16:22:31Z","abstract_excerpt":"Relativistic quantum-information studies in noninertial and black-hole settings often determine resource behavior through explicit calculations for particular input states and state functionals, leaving unclear whether the recurring monotonic trends originate from those choices or from a common underlying structure. In this work, we formulate the effective single-mode fermionic horizon transformation as a pair of complementary exterior and interior quantum channels, corresponding respectively to the physically accessible and inaccessible sectors, and establish exact post-processing orders in o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2608.08215","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2608.08215/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-11T01:22:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Npi8PbcTwYMvbCA2F0LRXqag3mRXFV5Sl/AyhQZQO10mKLp4JWyf9gUwM2mBVZ92Hf+AVExOmvHuS2J+cmPmBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T19:33:29.732264Z"},"content_sha256":"3bca67501a3f230ff46fefd1e44802e2647833559c4711f1490c87c7a0aac8a7","schema_version":"1.0","event_id":"sha256:3bca67501a3f230ff46fefd1e44802e2647833559c4711f1490c87c7a0aac8a7"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:OKA57UAWVP6V4KAYYZJ2TTT7NA","target":"integrity","payload":{"note":"DOI is split by whitespace or line breaks in the printed bibliography. Reconstructed DOI 10.1103/PhysRevA.87.022338 resolves to 'Fermionic-mode entanglement in quantum information'. A reader following the printed text alone cannot reach it.","snippet":"N. Friis, A.R. Lee, D.E. Bruschi: Fermionic-mode entanglement in quantum information. Phys. Rev. A 87(2), 022338 (2013) https://doi.org/10.1103/PhysRevA. 87.022338","arxiv_id":"2608.08215","detector":"doi_compliance","evidence":{"ref_index":93,"verdict_class":"incontrovertible","resolved_title":"Fermionic-mode entanglement in quantum information","printed_excerpt":"10.1103/physreva","reconstructed_doi":"10.1103/PhysRevA.87.022338"},"severity":"advisory","ref_index":93,"audited_at":"2026-08-12T00:29:11.844179Z","event_type":"pith.integrity.v1","detected_doi":"10.1103/PhysRevA.87.022338","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"004f7426d42cceabff5b86e531ad5dca03194027a7f4429450423c96db9c7cf2","paper_version":1,"verdict_class":"incontrovertible","resolved_title":"Fermionic-mode entanglement in quantum information","detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":19206,"payload_sha256":"b1682efe1fc0671e9bfd56568920874bde91801fda16f9b92b098aca2ed1f49b","signature_b64":"dDzYv92Y8TOChakZJIUuQPuLWXEVBlfNzB2uCsmKPKRaUO9PxU8KHQF/GHJj5lb73yo/D+nCtb2qowl8SaCLCQ==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-12T00:33:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"v+55s0JRZxGh4+2U8h+DDYWCeuKCBVPj/Mr9G/5gDEYsB3vDBv1lHyaWNg0aspx5oOmF50vAKQZqkSixoGvkDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T19:33:29.737653Z"},"content_sha256":"fbf00c3733cdb4a34d8002ccbddbcaf8ab09301c772ec020ec8a31221f3d33d5","schema_version":"1.0","event_id":"sha256:fbf00c3733cdb4a34d8002ccbddbcaf8ab09301c772ec020ec8a31221f3d33d5"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:OKA57UAWVP6V4KAYYZJ2TTT7NA","target":"integrity","payload":{"note":"DOI in the printed bibliography is fragmented by whitespace or line breaks. A longer candidate (10.2996/kmj/1138844604) was visible in the surrounding text but could not be confirmed against doi.org as printed.","snippet":"H. Umegaki: Conditional expectation in an operator alge- bra. IV. entropy and information. Kodai Math. Sem. Rep.14(2), 59–85 (1962) https://doi.org/10.2996/kmj/ 1138844604","arxiv_id":"2608.08215","detector":"doi_compliance","evidence":{"ref_index":82,"verdict_class":"incontrovertible","resolved_title":null,"printed_excerpt":"10.2996/kmj/","reconstructed_doi":"10.2996/kmj/1138844604"},"severity":"advisory","ref_index":82,"audited_at":"2026-08-12T00:29:11.844179Z","event_type":"pith.integrity.v1","detected_doi":"10.2996/kmj/1138844604","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"ef8f400fefa22c89a51ccb4e6989adc64ac0a8626328aae0f6a87f061bc93d2a","paper_version":1,"verdict_class":"incontrovertible","resolved_title":null,"detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":19205,"payload_sha256":"0e8032086a96122daaf6ec646b7ac30382069aeb198c3affb5a1898b847e0edb","signature_b64":"wFF95v+ln4eTw0DZQPepZJFcrojskHkCVbnog7jqQQERCqvsPHKg6l1rxaByqG5PuvoW2tVgfcf1bpz1BEW8Cw==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-12T00:33:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aSFEn8rJMetLFshzFXT/ZqNXni1/8+XU/7lwwcDBnQYhtgt9n5BwRYgwLFQV5kBP/7WgRCEoCxIcoUaP/vTvDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T19:33:29.738042Z"},"content_sha256":"e61b133d7f25c01bceb7188f5336459459324e4dd4ff7755b60f1d2b4f0988a1","schema_version":"1.0","event_id":"sha256:e61b133d7f25c01bceb7188f5336459459324e4dd4ff7755b60f1d2b4f0988a1"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:OKA57UAWVP6V4KAYYZJ2TTT7NA","target":"integrity","payload":{"note":"DOI in the printed bibliography is fragmented by whitespace or line breaks. A longer candidate (10.1109/CCC.2004.1313847) was visible in the surrounding text but could not be confirmed against doi.org as printed.","snippet":"R. Cleve, P. Høyer, B. Toner, J. Watrous: Consequences and limits of nonlocal strategies. In: Proceedings of the 19th IEEE Annual Conference on Computational Com- plexity, pp. 236–249. IEEE Computer Society, Los Alami- tos, CA, USA (2004). ","arxiv_id":"2608.08215","detector":"doi_compliance","evidence":{"ref_index":81,"verdict_class":"incontrovertible","resolved_title":null,"printed_excerpt":"10.1109/ccc.2004","reconstructed_doi":"10.1109/CCC.2004.1313847"},"severity":"advisory","ref_index":81,"audited_at":"2026-08-12T00:29:11.844179Z","event_type":"pith.integrity.v1","detected_doi":"10.1109/CCC.2004.1313847","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"f2bfe9226080bbd80cb413aef722a48a763ebb72bc38424e68d21de94bcbfd43","paper_version":1,"verdict_class":"incontrovertible","resolved_title":null,"detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":19204,"payload_sha256":"10716ee0570cce1e3214a1c815cdcbb63a2f6671b59819fd0278323bd7bf6fff","signature_b64":"Nz8ORlcRt4W0NHPKHkq5MAtvdpfU9Nev0nX+OWZQumLX/aJwfTsUvRZJlijOrjnk/vWXXpWMEerk/tcyeA0fDQ==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-12T00:33:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mzvtuKuT0TbFHiu2SefnLF4SNPtMKUm6UxmeexXNvACidtXJKwb4AzoRpbic5CXYwbShfxBbv9GxjcJaySWEAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T19:33:29.738415Z"},"content_sha256":"23c5dbac9bcad918ad08527255f8117d18bd29bf33bc4b57f2a8b8001fb9013b","schema_version":"1.0","event_id":"sha256:23c5dbac9bcad918ad08527255f8117d18bd29bf33bc4b57f2a8b8001fb9013b"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:OKA57UAWVP6V4KAYYZJ2TTT7NA","target":"integrity","payload":{"note":"DOI is split by whitespace or line breaks in the printed bibliography. Reconstructed DOI 10.1103/PhysRevX.6.041028 resolves to 'Quantum Processes Which Do Not Use Coherence'. A reader following the printed text alone cannot reach it.","snippet":"B. Yadin, J. Ma, D. Girolami, M. Gu, V. Vedral: Quan- tum processes which do not use coherence. Phys. Rev. X 6(4), 041028 (2016) https://doi.org/10.1103/PhysRevX. 6.041028","arxiv_id":"2608.08215","detector":"doi_compliance","evidence":{"ref_index":73,"verdict_class":"incontrovertible","resolved_title":"Quantum Processes Which Do Not Use Coherence","printed_excerpt":"10.1103/physrevx","reconstructed_doi":"10.1103/PhysRevX.6.041028"},"severity":"advisory","ref_index":73,"audited_at":"2026-08-12T00:29:11.844179Z","event_type":"pith.integrity.v1","detected_doi":"10.1103/PhysRevX.6.041028","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"e9f32ae4d1d98c594439e566194737dd261ff86c187805445ef72e23ccedca0f","paper_version":1,"verdict_class":"incontrovertible","resolved_title":"Quantum Processes Which Do Not Use Coherence","detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":19203,"payload_sha256":"9e49cd16ba8bc8ea5ea526c9ff48cb4c6d1a836e30fc8c326a58214c9d5222f5","signature_b64":"kKE3RquQwGojDdMIQWWimXSbWbODtv2ruT7xu4B6bSF1Wr0MtLnUAWj1kzULP7j5E34MuoUEqL1N+l8QEd5vBQ==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-12T00:33:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yNM40cyUpX1/i5ErxTA8OfmzQMPea69h4ylGbYTKwo367CCZl4eNeWFgxDmQhhCqyUSwrnT8Mp8XEABc/AYnDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T19:33:29.738784Z"},"content_sha256":"4a696c939e444aa93e5ec5b3c3cbb66847782f7b9be8bfa24b16a84a81964818","schema_version":"1.0","event_id":"sha256:4a696c939e444aa93e5ec5b3c3cbb66847782f7b9be8bfa24b16a84a81964818"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:OKA57UAWVP6V4KAYYZJ2TTT7NA","target":"integrity","payload":{"note":"DOI is split by whitespace or line breaks in the printed bibliography. Reconstructed DOI 10.1103/RevModPhys.89.041003 resolves to '<i>Colloquium</i>: Quantum coherence as a resource'. A reader following the printed text alone cannot reach it.","snippet":"A. Streltsov, G. Adesso, M.B. Plenio: Colloquium: quan- tum coherence as a resource. Rev. Mod. Phys.89(4), 041003 (2017) https://doi.org/10.1103/RevModPhys.89. 041003","arxiv_id":"2608.08215","detector":"doi_compliance","evidence":{"ref_index":71,"verdict_class":"incontrovertible","resolved_title":"<i>Colloquium</i>: Quantum coherence as a resource","printed_excerpt":"10.1103/revmodphys.89","reconstructed_doi":"10.1103/RevModPhys.89.041003"},"severity":"advisory","ref_index":71,"audited_at":"2026-08-12T00:29:11.844179Z","event_type":"pith.integrity.v1","detected_doi":"10.1103/RevModPhys.89.041003","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"4468d9fb9a2eb9e1f7b2092b16a6cb11c6e9bb276b3514bebad33fa3da15a918","paper_version":1,"verdict_class":"incontrovertible","resolved_title":"<i>Colloquium</i>: Quantum coherence as a resource","detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":19202,"payload_sha256":"64a2d5d97ee7459442d7bb8e92742c3891951ed013aac431a705eb6523a27647","signature_b64":"7FfrCz7/lDrWMrXdrsRXKK6na2bj1n6Y9Lzd/QgP2Si1G97T04aRxs4VJqlgBErRCX/YroTNmbcmkLXTwTqADQ==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-12T00:33:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wvUy6RunrKVefG4+MWvaPpzTJtHOAr2gSCm8qqRZF3OvTiVghKd8+rgDQXvg9jOldQHp0IWtOncwfcIyJUzVBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T19:33:29.739151Z"},"content_sha256":"96f1d38b95f14ebe9c5225f396027478330eea0fccea28d419676d0b4aeb24c2","schema_version":"1.0","event_id":"sha256:96f1d38b95f14ebe9c5225f396027478330eea0fccea28d419676d0b4aeb24c2"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:OKA57UAWVP6V4KAYYZJ2TTT7NA","target":"integrity","payload":{"note":"DOI is split by whitespace or line breaks in the printed bibliography. Reconstructed DOI 10.1103/PhysRevLett.80.2245 resolves to 'Entanglement of Formation of an Arbitrary State of Two Qubits'. A reader following the printed text alone cannot reach it.","snippet":"W.K. Wootters: Entanglement of formation of an arbi- trary state of two qubits. Phys. Rev. Lett.80(10), 2245–2248 (1998) https://doi.org/10.1103/PhysRevLett. 80.2245","arxiv_id":"2608.08215","detector":"doi_compliance","evidence":{"ref_index":62,"verdict_class":"incontrovertible","resolved_title":"Entanglement of Formation of an Arbitrary State of Two Qubits","printed_excerpt":"10.1103/physrevlett","reconstructed_doi":"10.1103/PhysRevLett.80.2245"},"severity":"advisory","ref_index":62,"audited_at":"2026-08-12T00:29:11.844179Z","event_type":"pith.integrity.v1","detected_doi":"10.1103/PhysRevLett.80.2245","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"95d93058a537c76b29d36ea47ecafbd610c21554c48e27433ae64059fb383260","paper_version":1,"verdict_class":"incontrovertible","resolved_title":"Entanglement of Formation of an Arbitrary State of Two Qubits","detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":19201,"payload_sha256":"6511c82d39ffa498f21777914a546b682d189814c5fb046c630a120d07e54737","signature_b64":"hE9e0WBRC2D1EXHA0QN0wvAekPG08RH/gBR0+MjlhL4SKp/+7BHpJlDcKAONd/kRY++YFqcQ8iphcVcuB1tYAA==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-12T00:33:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LYCqoeXawPlXEtIQxtinh588Dju67N3+XQMNYneDqaPHDhuoBg2KWITtx+O3Imu8WL7oemqYOUS3dt2Q7HcPAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T19:33:29.739525Z"},"content_sha256":"b0be109a945607daae1bc435d1b9da1c65e915c1de5773dd60f62861b43b075e","schema_version":"1.0","event_id":"sha256:b0be109a945607daae1bc435d1b9da1c65e915c1de5773dd60f62861b43b075e"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:OKA57UAWVP6V4KAYYZJ2TTT7NA","target":"integrity","payload":{"note":"DOI is split by whitespace or line breaks in the printed bibliography. Reconstructed DOI 10.1103/PhysRevLett.95.090503 resolves to 'Logarithmic Negativity: A Full Entanglement Monotone That is not Convex'. A reader following the printed text alone cannot reach it.","snippet":"M.B. Plenio: Logarithmic negativity: a full entanglement monotone that is not convex. Phys. Rev. Lett.95(9), 090503 (2005) https://doi.org/10.1103/PhysRevLett.95. 090503","arxiv_id":"2608.08215","detector":"doi_compliance","evidence":{"ref_index":56,"verdict_class":"incontrovertible","resolved_title":"Logarithmic Negativity: A Full Entanglement Monotone That is not Convex","printed_excerpt":"10.1103/physrevlett.95","reconstructed_doi":"10.1103/PhysRevLett.95.090503"},"severity":"advisory","ref_index":56,"audited_at":"2026-08-12T00:29:11.844179Z","event_type":"pith.integrity.v1","detected_doi":"10.1103/PhysRevLett.95.090503","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"e76417e294ddd6a2f4bc814faf4652e5c4f955daa9dd021c845c5c4bba3747b4","paper_version":1,"verdict_class":"incontrovertible","resolved_title":"Logarithmic Negativity: A Full Entanglement Monotone That is not Convex","detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":19200,"payload_sha256":"934fbae38c67cdd520c0e971dd4f7a3e734d6dedb0b55f31c9b2044fe5cb0ab6","signature_b64":"cI+r7/ZIf9kC7EI3EHB/kFg9NEpnBy3VSjNEdALLaOAmNLLODHYcNs2cQkyhDQoEiZ8GY1C7EEmYV12reNgcDg==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-12T00:33:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KlA8FKMoXGtuEJzOkzSrv8VOI6d5COeUgI/zwJY59eiJz1xWQzllvmAKua1/LArq5OecpxYS/AY5T+jIDS+XAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T19:33:29.739887Z"},"content_sha256":"0928eb80b99cb275d5ba908f6f753705f5f1ff6e86c6e92b5678013f9cbf18d3","schema_version":"1.0","event_id":"sha256:0928eb80b99cb275d5ba908f6f753705f5f1ff6e86c6e92b5678013f9cbf18d3"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:OKA57UAWVP6V4KAYYZJ2TTT7NA","target":"integrity","payload":{"note":"DOI is split by whitespace or line breaks in the printed bibliography. Reconstructed DOI 10.1103/PhysRevD.89.065022 resolves to 'How the Hawking effect affects multipartite entanglement of Dirac particles in the background of a Schwarzschild black h'. A reader following the printed text alone cannot reach it.","snippet":"S. Xu, X.-k. Song, J.-d. Shi, L. Ye: How the Hawking effect affects multipartite entanglement of Dirac particles in the background of a Schwarzschild black hole. Phys. Rev. D 89(6), 065022 (2014) https://doi.org/10.1103/PhysRevD. 89.065022","arxiv_id":"2608.08215","detector":"doi_compliance","evidence":{"ref_index":40,"verdict_class":"incontrovertible","resolved_title":"How the Hawking effect affects multipartite entanglement of Dirac particles in the background of a Schwarzschild black hole","printed_excerpt":"10.1103/physrevd","reconstructed_doi":"10.1103/PhysRevD.89.065022"},"severity":"advisory","ref_index":40,"audited_at":"2026-08-12T00:29:11.844179Z","event_type":"pith.integrity.v1","detected_doi":"10.1103/PhysRevD.89.065022","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"1f15ade5f4e259d15b3e3ff95ce2fd12d5b61e2f43af8f87bdb2f9ba8f46c888","paper_version":1,"verdict_class":"incontrovertible","resolved_title":"How the Hawking effect affects multipartite entanglement of Dirac particles in the background of a Schwarzschild black hole","detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":19199,"payload_sha256":"16c281625bef17df31c0bbf378b4fb719099453a48977443f186df0df06a99dc","signature_b64":"x0Dzef6peyWcdvgLIwMBkZRGjtZs7OYFGEUxfmpkyqO7o6iqDZ/zUceavQMgVXyok7RYW4f/uGtfBdqipxjoCQ==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-12T00:33:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lK+rwK7HSP8JelqJ4YTidKcD1XIzmTd1qupQAOqIlxrwYtoMRy6I1ki1397ZaA6HNd40MneRpLGHwMfcm/k8BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T19:33:29.740536Z"},"content_sha256":"be923c3b6d387dec06df5f023b3b67668547f651e0de94bbfee1d182f0350053","schema_version":"1.0","event_id":"sha256:be923c3b6d387dec06df5f023b3b67668547f651e0de94bbfee1d182f0350053"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:OKA57UAWVP6V4KAYYZJ2TTT7NA","target":"integrity","payload":{"note":"DOI is split by whitespace or line breaks in the printed bibliography. Reconstructed DOI 10.1016/j.nuclphysb.2026.117559 resolves to 'Bosonic and fermionic mutual information of N-partite systems in dilaton black hole background'. A reader following the printed text alone cannot reach it.","snippet":"X.-W. Teng, R.-Y. Xu, H.-C. Yang, S.-M. Wu: Bosonic and fermionic mutual information of N-partite systems in dilaton black hole background. Nucl. Phys. B1029, 117559 (2026) https://doi.org/10.1016/j.nuclphysb.2026. 117559","arxiv_id":"2608.08215","detector":"doi_compliance","evidence":{"ref_index":39,"verdict_class":"incontrovertible","resolved_title":"Bosonic and fermionic mutual information of N-partite systems in dilaton black hole background","printed_excerpt":"10.1016/j.nuclphysb.2026","reconstructed_doi":"10.1016/j.nuclphysb.2026.117559"},"severity":"advisory","ref_index":39,"audited_at":"2026-08-12T00:29:11.844179Z","event_type":"pith.integrity.v1","detected_doi":"10.1016/j.nuclphysb.2026.117559","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"3a366016b4a31aac95e8d6b941079b77aa2d7707ac9df9faa69bb4caeaebf088","paper_version":1,"verdict_class":"incontrovertible","resolved_title":"Bosonic and fermionic mutual information of N-partite systems in dilaton black hole background","detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":19198,"payload_sha256":"c8d73cf2039bcb9330d5fc67c632d032b8b8a9e8e803b1ee486f15ae3f357977","signature_b64":"PrN4fBEl210ee0tjdL3ECPRdM6Z/8YSJCuqaZInAXrA3nXbTER0ZVipAS50UPGB2cj83vd37jxw4Ka05gMCjCw==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-12T00:33:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TqzYdbLW2+/Xo4Vd1qJZvLmH7ByUS17d4Pqj1YXnKq9TXSbRu8yVbjVGeW3Xecz9w972cDIFV/bFhHfPlkNhAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T19:33:29.741095Z"},"content_sha256":"c24839f273a4b365cbe5dc0fdd7d5fc0ee4ff4bf06c07859744bad0c4b711893","schema_version":"1.0","event_id":"sha256:c24839f273a4b365cbe5dc0fdd7d5fc0ee4ff4bf06c07859744bad0c4b711893"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:OKA57UAWVP6V4KAYYZJ2TTT7NA","target":"integrity","payload":{"note":"DOI in the printed bibliography is fragmented by whitespace or line breaks. A longer candidate (10.1140/epjc/s10052-026-15285-z) was visible in the surrounding text but could not be confirmed against doi.org as printed.","snippet":"W.-M. Li, J. Lu, S.-M. Wu: Entropic uncertainty and coherence in Einstein–Gauss–Bonnet gravity. Eur. Phys. J. C86(1), 59 (2026) https://doi.org/10.1140/epjc/ s10052-026-15285-z","arxiv_id":"2608.08215","detector":"doi_compliance","evidence":{"ref_index":30,"verdict_class":"incontrovertible","resolved_title":null,"printed_excerpt":"10.1140/epjc/","reconstructed_doi":"10.1140/epjc/s10052-026-15285-z"},"severity":"advisory","ref_index":30,"audited_at":"2026-08-12T00:29:11.844179Z","event_type":"pith.integrity.v1","detected_doi":"10.1140/epjc/s10052-026-15285-z","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"40dc00e7abb0912ba2d364a6d7b49d571b65946cb63f8f08427f7dc2727f6246","paper_version":1,"verdict_class":"incontrovertible","resolved_title":null,"detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":19197,"payload_sha256":"02eeba2fc22a357870b91bf28c99932486c53b35998deca1fb43efa44ef772e8","signature_b64":"WflsoZWrxoTnAayfm5lWFyfIBR6fV7rOfqIGvPUu1iiwBfykVAYYjBiuIQnUBX8jwRX8Gf3AheEPJAF1OnZiAA==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-12T00:33:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"C6hJO5Gxx0fhYFXnI7zlczQ/XSMGg0z9ZM4F2DmGJJhQjdEdiGevL3/uCtzq9RcxlsLxpFmekAR6K5e7sAXhDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T19:33:29.741536Z"},"content_sha256":"83d30a8809a197d63283565ec5605e43ddc0d6e29ad3761c74d341a886686fe8","schema_version":"1.0","event_id":"sha256:83d30a8809a197d63283565ec5605e43ddc0d6e29ad3761c74d341a886686fe8"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:OKA57UAWVP6V4KAYYZJ2TTT7NA","target":"integrity","payload":{"note":"DOI is split by whitespace or line breaks in the printed bibliography. Reconstructed DOI 10.1016/j.physletb.2010.07.035 resolves to 'Entanglement redistribution in the Schwarzschild spacetime'. A reader following the printed text alone cannot reach it.","snippet":"J. Wang, Q. Pan, J. Jing: Entanglement redistribution in the Schwarzschild spacetime. Phys. Lett. B692(3), 202–205 (2010) https://doi.org/10.1016/j.physletb.2010. 07.035","arxiv_id":"2608.08215","detector":"doi_compliance","evidence":{"ref_index":27,"verdict_class":"incontrovertible","resolved_title":"Entanglement redistribution in the Schwarzschild spacetime","printed_excerpt":"10.1016/j.physletb.2010","reconstructed_doi":"10.1016/j.physletb.2010.07.035"},"severity":"advisory","ref_index":27,"audited_at":"2026-08-12T00:29:11.844179Z","event_type":"pith.integrity.v1","detected_doi":"10.1016/j.physletb.2010.07.035","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"c7fd311138ea2f319d00901ecb550e3a53126c051655a15c41d6d127dff4fefc","paper_version":1,"verdict_class":"incontrovertible","resolved_title":"Entanglement redistribution in the Schwarzschild spacetime","detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":19196,"payload_sha256":"cd6cfc22112efef59a7f590ac51460bea9f1450114b8f931e6e08a78542d6ce3","signature_b64":"lO6Fa8PMnPVUMY9fRRqcIA7lkGRjEPzA5zyBCcK/5ch6mzx9GS7AjVHnJqaIMRLos56S+yN3DEf/ZpjOEg5pCw==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-12T00:33:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"S/bEDYwPAFSlJd6DG20X7ac9orOg7pyh4zBXDVJBs2hQLvoDFXHk/XJqwYs98fd57e1Um+Np5otO35h6YSaVDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T19:33:29.742141Z"},"content_sha256":"fea028d3cd44b1732a3cfb3e5042115c67e5a708337f61d9909d9938a73b3d2c","schema_version":"1.0","event_id":"sha256:fea028d3cd44b1732a3cfb3e5042115c67e5a708337f61d9909d9938a73b3d2c"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:OKA57UAWVP6V4KAYYZJ2TTT7NA","target":"integrity","payload":{"note":"DOI in the printed bibliography is fragmented by whitespace or line breaks. A longer candidate (10.1088/1572-9494/ac01e4) was visible in the surrounding text but could not be confirmed against doi.org as printed.","snippet":"Y.-J. Lian, J.-M. Liu: Quantum Fisher informa- tion of a qubit-qutrit system in Garfinkle–Horowitz– Strominger dilation space–time. Commun. Theor. Phys. 73(8), 085102 (2021) https://doi.org/10.1088/1572-9494/ ac01e4","arxiv_id":"2608.08215","detector":"doi_compliance","evidence":{"ref_index":17,"verdict_class":"incontrovertible","resolved_title":null,"printed_excerpt":"10.1088/1572-9494/","reconstructed_doi":"10.1088/1572-9494/ac01e4"},"severity":"advisory","ref_index":17,"audited_at":"2026-08-12T00:29:11.844179Z","event_type":"pith.integrity.v1","detected_doi":"10.1088/1572-9494/ac01e4","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"182e016c8d431e59ba5da17c16d6abb2bc9e6e962a7992c5bca8c36e8fb39091","paper_version":1,"verdict_class":"incontrovertible","resolved_title":null,"detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":19195,"payload_sha256":"8e3cb314c170930c2b7900e8bc81922d50f69cab97124b37bf0afc28cefe0a19","signature_b64":"QDqD41zCNfZw6/N36wcIDfSY6tA/p1YU3xjq7Ywn6CXeYejbOWGNCNVeQ/yVsxoJdi2URr1xl0gcPCAHmccjBg==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-12T00:33:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NTkJSL6DMMBwz4BWC3k+d/Md9nyFslirEHC93fGn2BI2jA/ZzYyOsDcGT2k3IqB764AqLJc3ZSnMwWsEnIk1BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T19:33:29.742564Z"},"content_sha256":"ba5c5a8b18b2b340a9c201069c5befa9e98477bbfd62f8cb0d29f87f85905830","schema_version":"1.0","event_id":"sha256:ba5c5a8b18b2b340a9c201069c5befa9e98477bbfd62f8cb0d29f87f85905830"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:OKA57UAWVP6V4KAYYZJ2TTT7NA","target":"integrity","payload":{"note":"DOI is split by whitespace or line breaks in the printed bibliography. Reconstructed DOI 10.1002/andp.201800208 resolves to 'Entropic Uncertainty Relation for Dirac Particles in Garfinkle–Horowitz–Strominger Dilation Space–Time'. A reader following the printed text alone cannot reach it.","snippet":"Z.-Y. Zhang, J.-M. Liu, Z. Hu, Y. Wang: Entropic uncer- tainty relation for Dirac particles in Garfinkle–Horowitz– Strominger dilation space–time. Ann. Phys. (Berlin) 530(11), 1800208 (2018) https://doi.org/10.1002/andp. 201800208","arxiv_id":"2608.08215","detector":"doi_compliance","evidence":{"ref_index":16,"verdict_class":"incontrovertible","resolved_title":"Entropic Uncertainty Relation for Dirac Particles in Garfinkle–Horowitz–Strominger Dilation Space–Time","printed_excerpt":"10.1002/andp","reconstructed_doi":"10.1002/andp.201800208"},"severity":"advisory","ref_index":16,"audited_at":"2026-08-12T00:29:11.844179Z","event_type":"pith.integrity.v1","detected_doi":"10.1002/andp.201800208","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"b1aa3106ed13bf44ef7534bc6299c2759a6bab53a374321bbbf3fcf138382450","paper_version":1,"verdict_class":"incontrovertible","resolved_title":"Entropic Uncertainty Relation for Dirac Particles in Garfinkle–Horowitz–Strominger Dilation Space–Time","detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":19194,"payload_sha256":"8d824dfdb4d46ddf5a1c7ea786475926ecb277511d56d90c27c31a3ec347a03e","signature_b64":"1XYS692KFrFoeh9ia5upihv9OpOrRL4BliBHEDuxTgeTU5YrYx1tt0Rnsx3cU5nKakmsPeYAZa5khwJDvwJIAQ==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-12T00:33:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5DsAVBIJzUwzwUT5MXGpr80mf3qxIfwUEWzfKBDGaNgxXO0rd1V/1PUZDwvOaN7x8kk0cRX4P/uCDuE3fnNIAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T19:33:29.742951Z"},"content_sha256":"64d9f80330ba857ee935229163d2df6fb2799306b9526db2a20d560818c52712","schema_version":"1.0","event_id":"sha256:64d9f80330ba857ee935229163d2df6fb2799306b9526db2a20d560818c52712"},{"event_type":"integrity_finding","subject_pith_number":"pith:2026:OKA57UAWVP6V4KAYYZJ2TTT7NA","target":"integrity","payload":{"note":"DOI is split by whitespace or line breaks in the printed bibliography. Reconstructed DOI 10.1103/PhysRevD.7.2850 resolves to 'Nonuniqueness of Canonical Field Quantization in Riemannian Space-Time'. A reader following the printed text alone cannot reach it.","snippet":"S.A. Fulling: Nonuniqueness of canonical field quanti- zation in Riemannian space-time. Phys. Rev. D7(10), 2850–2862 (1973) https://doi.org/10.1103/PhysRevD.7. 2850","arxiv_id":"2608.08215","detector":"doi_compliance","evidence":{"ref_index":2,"verdict_class":"incontrovertible","resolved_title":"Nonuniqueness of Canonical Field Quantization in Riemannian Space-Time","printed_excerpt":"10.1103/physrevd.7","reconstructed_doi":"10.1103/PhysRevD.7.2850"},"severity":"advisory","ref_index":2,"audited_at":"2026-08-12T00:29:11.844179Z","event_type":"pith.integrity.v1","detected_doi":"10.1103/PhysRevD.7.2850","detector_url":"https://pith.science/pith-integrity-protocol#doi_compliance","external_url":null,"finding_type":"recoverable_identifier","evidence_hash":"3a70234b13bae77f02ba66366db2d057f0aab448674edf05c69378dc7643be30","paper_version":1,"verdict_class":"incontrovertible","resolved_title":"Nonuniqueness of Canonical Field Quantization in Riemannian Space-Time","detector_version":"1.1.0","detected_arxiv_id":null,"integrity_event_id":19193,"payload_sha256":"981de5224776a3aac26c21b7c56ffae5661f7b0aebe88f2d12fc9a37a74c08b6","signature_b64":"0wG9ym1S1YASdB5ufqvHdiPq1e7HBzLdL32ZrqhCXB+K1ti5/1nnpBo8Pmz//2ilr206RppGqe/ubNiNI3NHAQ==","signing_key_id":"pith-v1-2026-05"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-08-12T00:33:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"81o6UIzxE9/H4Sltr+9vaU8eIPbpqe7ag80O+TNYWbaOf7D6E85xL2vfz65/KnWqtjLgzV7ToPhgS/vN1tf2Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T19:33:29.743350Z"},"content_sha256":"decb5db01076f89b470b35db91067c6bf37e883d693fdbf5f59408dffd0895ad","schema_version":"1.0","event_id":"sha256:decb5db01076f89b470b35db91067c6bf37e883d693fdbf5f59408dffd0895ad"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/OKA57UAWVP6V4KAYYZJ2TTT7NA/bundle.json","state_url":"https://pith.science/pith/OKA57UAWVP6V4KAYYZJ2TTT7NA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/OKA57UAWVP6V4KAYYZJ2TTT7NA/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":"2026-08-12T19:33:29Z","links":{"resolver":"https://pith.science/pith/OKA57UAWVP6V4KAYYZJ2TTT7NA","bundle":"https://pith.science/pith/OKA57UAWVP6V4KAYYZJ2TTT7NA/bundle.json","state":"https://pith.science/pith/OKA57UAWVP6V4KAYYZJ2TTT7NA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/OKA57UAWVP6V4KAYYZJ2TTT7NA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:OKA57UAWVP6V4KAYYZJ2TTT7NA","merge_version":"pith-open-graph-merge-v1","event_count":16,"valid_event_count":16,"invalid_event_count":0,"equivocation_count":1,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"8dccc8292ea1feea06b088e72e82f1ce5fe772cbf1b6704722be3f35634c7b67","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2026-08-08T16:22:31Z","title_canon_sha256":"93a9f5d56b0adbc8c2e7bc7acea13b5c7e00cd5a054a7ebfc64bfdb1a3d1bafd"},"schema_version":"1.0","source":{"id":"2608.08215","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2608.08215","created_at":"2026-08-11T01:22:00Z"},{"alias_kind":"arxiv_version","alias_value":"2608.08215v1","created_at":"2026-08-11T01:22:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2608.08215","created_at":"2026-08-11T01:22:00Z"},{"alias_kind":"pith_short_12","alias_value":"OKA57UAWVP6V","created_at":"2026-08-11T01:22:00Z"},{"alias_kind":"pith_short_16","alias_value":"OKA57UAWVP6V4KAY","created_at":"2026-08-11T01:22:00Z"},{"alias_kind":"pith_short_8","alias_value":"OKA57UAW","created_at":"2026-08-11T01:22:00Z"}],"graph_snapshots":[{"event_id":"sha256:3bca67501a3f230ff46fefd1e44802e2647833559c4711f1490c87c7a0aac8a7","target":"graph","created_at":"2026-08-11T01:22:00Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2608.08215/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Relativistic quantum-information studies in noninertial and black-hole settings often determine resource behavior through explicit calculations for particular input states and state functionals, leaving unclear whether the recurring monotonic trends originate from those choices or from a common underlying structure. In this work, we formulate the effective single-mode fermionic horizon transformation as a pair of complementary exterior and interior quantum channels, corresponding respectively to the physically accessible and inaccessible sectors, and establish exact post-processing orders in o","authors_text":"Jin-Ming Liu, Shuhao Li","cross_cats":["gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2026-08-08T16:22:31Z","title":"Opposite post-processing orders of fermionic horizon channels and their quantum-resource monotonicity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2608.08215","kind":"arxiv","version":1},"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:cf10a4301a6c5384d80b528a16063f41d684f408faaf9449129fc5c797298c95","target":"record","created_at":"2026-08-11T01:22:00Z","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":"8dccc8292ea1feea06b088e72e82f1ce5fe772cbf1b6704722be3f35634c7b67","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2026-08-08T16:22:31Z","title_canon_sha256":"93a9f5d56b0adbc8c2e7bc7acea13b5c7e00cd5a054a7ebfc64bfdb1a3d1bafd"},"schema_version":"1.0","source":{"id":"2608.08215","kind":"arxiv","version":1}},"canonical_sha256":"7281dfd016abfd5e2818c653a9ce7f68090a11e10c62f39d78a34f2187559617","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7281dfd016abfd5e2818c653a9ce7f68090a11e10c62f39d78a34f2187559617","first_computed_at":"2026-08-11T01:22:00.447187Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-08-11T01:22:00.447187Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ZUGLYD3qIgPhoKA3AMNvMrM2GXMNcQfXSHAlHYrpT6n0I1qD9m6X951tM4skTPcpbqMp33SQrRQOOTgTMJCwCA==","signature_status":"signed_v1","signed_at":"2026-08-11T01:22:00.449529Z","signed_message":"canonical_sha256_bytes"},"source_id":"2608.08215","source_kind":"arxiv","source_version":1}}},"equivocations":[{"signer_id":"pith.science","event_type":"integrity_finding","target":"integrity","event_ids":["sha256:0928eb80b99cb275d5ba908f6f753705f5f1ff6e86c6e92b5678013f9cbf18d3","sha256:23c5dbac9bcad918ad08527255f8117d18bd29bf33bc4b57f2a8b8001fb9013b","sha256:4a696c939e444aa93e5ec5b3c3cbb66847782f7b9be8bfa24b16a84a81964818","sha256:64d9f80330ba857ee935229163d2df6fb2799306b9526db2a20d560818c52712","sha256:83d30a8809a197d63283565ec5605e43ddc0d6e29ad3761c74d341a886686fe8","sha256:96f1d38b95f14ebe9c5225f396027478330eea0fccea28d419676d0b4aeb24c2","sha256:b0be109a945607daae1bc435d1b9da1c65e915c1de5773dd60f62861b43b075e","sha256:ba5c5a8b18b2b340a9c201069c5befa9e98477bbfd62f8cb0d29f87f85905830","sha256:be923c3b6d387dec06df5f023b3b67668547f651e0de94bbfee1d182f0350053","sha256:c24839f273a4b365cbe5dc0fdd7d5fc0ee4ff4bf06c07859744bad0c4b711893","sha256:decb5db01076f89b470b35db91067c6bf37e883d693fdbf5f59408dffd0895ad","sha256:e61b133d7f25c01bceb7188f5336459459324e4dd4ff7755b60f1d2b4f0988a1","sha256:fbf00c3733cdb4a34d8002ccbddbcaf8ab09301c772ec020ec8a31221f3d33d5","sha256:fea028d3cd44b1732a3cfb3e5042115c67e5a708337f61d9909d9938a73b3d2c"]}],"invalid_events":[],"applied_event_ids":["sha256:cf10a4301a6c5384d80b528a16063f41d684f408faaf9449129fc5c797298c95","sha256:3bca67501a3f230ff46fefd1e44802e2647833559c4711f1490c87c7a0aac8a7"],"state_sha256":"42b5a4b3ad16fc2e9cd0a5f3d2e3d95bd93496049b69191f99094ef9746108ff"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0Bp21CCBmAfUFdZvgDDn547XpO0Ktw4He4WpEjai0XHXUUF6bEpn0a9w6KMHjbC7b0eF00Wd8hZDuU1TgtAJBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-12T19:33:29.749981Z","bundle_sha256":"0e98689cbdb86652a143704f67a12f91c127bcfec4f185c58a84c4d7b08d5585"}}