{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:3CVLXH3S2FKRRRWP266E6IRCYY","short_pith_number":"pith:3CVLXH3S","schema_version":"1.0","canonical_sha256":"d8aabb9f72d15518c6cfd7bc4f2222c60587bec571bc77937b95072f51551a79","source":{"kind":"arxiv","id":"1610.01548","version":3},"attestation_state":"computed","paper":{"title":"The arrow of time in open quantum systems and dynamical breaking of the resonance-antiresonance symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Gonzalo Ordonez, Naomichi Hatano","submitted_at":"2016-10-05T18:05:50Z","abstract_excerpt":"Open quantum systems are often represented by non-Hermitian effective Hamiltonians that have complex eigenvalues associated with resonances. In previous work we showed that the evolution of tight-binding open systems can be represented by an explicitly time-reversal symmetric expansion involving all the discrete eigenstates of the effective Hamiltonian. These eigenstates include complex-conjugate pairs of resonant and anti-resonant states. An initially time-reversal-symmetric state contains equal contributions from the resonant and anti-resonant states. Here we show that as the state evolves i"},"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":"1610.01548","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-10-05T18:05:50Z","cross_cats_sorted":[],"title_canon_sha256":"573f95242f047dd1e28f746540a986207d713bbf3124453c77630d267d68daab","abstract_canon_sha256":"2387d26e057c826a21e2ec842b1588f368269c38b615a17720ea414e24428b16"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:35:51.707036Z","signature_b64":"UxQOmDJh3j+CnG21dH+vEbdfkpwazd6vhbccKqUzmQWg/ED0kt2EZcUIYQhRm5v8MHEajNlLIYuVFSBYRZcbCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d8aabb9f72d15518c6cfd7bc4f2222c60587bec571bc77937b95072f51551a79","last_reissued_at":"2026-05-18T00:35:51.706574Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:35:51.706574Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The arrow of time in open quantum systems and dynamical breaking of the resonance-antiresonance symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Gonzalo Ordonez, Naomichi Hatano","submitted_at":"2016-10-05T18:05:50Z","abstract_excerpt":"Open quantum systems are often represented by non-Hermitian effective Hamiltonians that have complex eigenvalues associated with resonances. In previous work we showed that the evolution of tight-binding open systems can be represented by an explicitly time-reversal symmetric expansion involving all the discrete eigenstates of the effective Hamiltonian. These eigenstates include complex-conjugate pairs of resonant and anti-resonant states. An initially time-reversal-symmetric state contains equal contributions from the resonant and anti-resonant states. Here we show that as the state evolves i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.01548","kind":"arxiv","version":3},"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":"1610.01548","created_at":"2026-05-18T00:35:51.706640+00:00"},{"alias_kind":"arxiv_version","alias_value":"1610.01548v3","created_at":"2026-05-18T00:35:51.706640+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.01548","created_at":"2026-05-18T00:35:51.706640+00:00"},{"alias_kind":"pith_short_12","alias_value":"3CVLXH3S2FKR","created_at":"2026-05-18T12:29:55.572404+00:00"},{"alias_kind":"pith_short_16","alias_value":"3CVLXH3S2FKRRRWP","created_at":"2026-05-18T12:29:55.572404+00:00"},{"alias_kind":"pith_short_8","alias_value":"3CVLXH3S","created_at":"2026-05-18T12:29:55.572404+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.05878","citing_title":"Exact WKB analysis of inverted triple-well: resonance, PT-symmetry breaking, and resurgence","ref_index":132,"is_internal_anchor":false},{"citing_arxiv_id":"2604.05878","citing_title":"Exact WKB analysis of inverted triple-well: resonance, PT-symmetry breaking, and resurgence","ref_index":132,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3CVLXH3S2FKRRRWP266E6IRCYY","json":"https://pith.science/pith/3CVLXH3S2FKRRRWP266E6IRCYY.json","graph_json":"https://pith.science/api/pith-number/3CVLXH3S2FKRRRWP266E6IRCYY/graph.json","events_json":"https://pith.science/api/pith-number/3CVLXH3S2FKRRRWP266E6IRCYY/events.json","paper":"https://pith.science/paper/3CVLXH3S"},"agent_actions":{"view_html":"https://pith.science/pith/3CVLXH3S2FKRRRWP266E6IRCYY","download_json":"https://pith.science/pith/3CVLXH3S2FKRRRWP266E6IRCYY.json","view_paper":"https://pith.science/paper/3CVLXH3S","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1610.01548&json=true","fetch_graph":"https://pith.science/api/pith-number/3CVLXH3S2FKRRRWP266E6IRCYY/graph.json","fetch_events":"https://pith.science/api/pith-number/3CVLXH3S2FKRRRWP266E6IRCYY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3CVLXH3S2FKRRRWP266E6IRCYY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3CVLXH3S2FKRRRWP266E6IRCYY/action/storage_attestation","attest_author":"https://pith.science/pith/3CVLXH3S2FKRRRWP266E6IRCYY/action/author_attestation","sign_citation":"https://pith.science/pith/3CVLXH3S2FKRRRWP266E6IRCYY/action/citation_signature","submit_replication":"https://pith.science/pith/3CVLXH3S2FKRRRWP266E6IRCYY/action/replication_record"}},"created_at":"2026-05-18T00:35:51.706640+00:00","updated_at":"2026-05-18T00:35:51.706640+00:00"}