{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:CALILC4LSHKLFIPTGMWBDAMY67","short_pith_number":"pith:CALILC4L","schema_version":"1.0","canonical_sha256":"1016858b8b91d4b2a1f3332c118198f7f8bd6fa2d1bc0b25e0a32e08fabf2710","source":{"kind":"arxiv","id":"2606.29770","version":1},"attestation_state":"computed","paper":{"title":"Krylov Complexity in Non-Inertial Quantum Systems","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["gr-qc","hep-ph","hep-th"],"primary_cat":"quant-ph","authors_text":"Hai-Qing Zhang, Lei-Hua Liu, Ming-Qi Ma, Shi-Cheng Liu","submitted_at":"2026-06-29T04:25:08Z","abstract_excerpt":"In this work, we formulate the Krylov complexity in non-In an inertial quantum system, the direct emergence of the $SU(1,1)$ sector from the Klein-Gordon symplectic form dictates that the Rindler pair-number sector naturally forms the Krylov basis for uniformly accelerating observers. Under this construction, we generalize the Bogoliubov coefficients by exploiting the $SU(1,1)$ group-structured Hamiltonian. Within this framework, we explicitly derive that the Krylov complexity is exactly equal to the mean number of correlated Rindler pairs generated via Bogoliubov mixing. Furthermore, the comp"},"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":"2606.29770","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2026-06-29T04:25:08Z","cross_cats_sorted":["gr-qc","hep-ph","hep-th"],"title_canon_sha256":"273a1272e3c05320f5affdc65c61274d74b7dbb246d3def7cbe6a4348f8ec481","abstract_canon_sha256":"333db0523cbd006bddfcd796fb0a1d8e5d3f2ca143c8dc84caf1a13dad630030"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-30T02:17:34.526651Z","signature_b64":"MnbeMmSpfrnSoTzOUNfMjccYhui5273SJRBzlgMwsJYvEgkQedJA7OmBCvsjohVxb0/SrjjWUgyBq+y6OzTRDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1016858b8b91d4b2a1f3332c118198f7f8bd6fa2d1bc0b25e0a32e08fabf2710","last_reissued_at":"2026-06-30T02:17:34.525997Z","signature_status":"signed_v1","first_computed_at":"2026-06-30T02:17:34.525997Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Krylov Complexity in Non-Inertial Quantum Systems","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["gr-qc","hep-ph","hep-th"],"primary_cat":"quant-ph","authors_text":"Hai-Qing Zhang, Lei-Hua Liu, Ming-Qi Ma, Shi-Cheng Liu","submitted_at":"2026-06-29T04:25:08Z","abstract_excerpt":"In this work, we formulate the Krylov complexity in non-In an inertial quantum system, the direct emergence of the $SU(1,1)$ sector from the Klein-Gordon symplectic form dictates that the Rindler pair-number sector naturally forms the Krylov basis for uniformly accelerating observers. Under this construction, we generalize the Bogoliubov coefficients by exploiting the $SU(1,1)$ group-structured Hamiltonian. Within this framework, we explicitly derive that the Krylov complexity is exactly equal to the mean number of correlated Rindler pairs generated via Bogoliubov mixing. Furthermore, the comp"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.29770","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/2606.29770/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2606.29770","created_at":"2026-06-30T02:17:34.526092+00:00"},{"alias_kind":"arxiv_version","alias_value":"2606.29770v1","created_at":"2026-06-30T02:17:34.526092+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.29770","created_at":"2026-06-30T02:17:34.526092+00:00"},{"alias_kind":"pith_short_12","alias_value":"CALILC4LSHKL","created_at":"2026-06-30T02:17:34.526092+00:00"},{"alias_kind":"pith_short_16","alias_value":"CALILC4LSHKLFIPT","created_at":"2026-06-30T02:17:34.526092+00:00"},{"alias_kind":"pith_short_8","alias_value":"CALILC4L","created_at":"2026-06-30T02:17:34.526092+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/CALILC4LSHKLFIPTGMWBDAMY67","json":"https://pith.science/pith/CALILC4LSHKLFIPTGMWBDAMY67.json","graph_json":"https://pith.science/api/pith-number/CALILC4LSHKLFIPTGMWBDAMY67/graph.json","events_json":"https://pith.science/api/pith-number/CALILC4LSHKLFIPTGMWBDAMY67/events.json","paper":"https://pith.science/paper/CALILC4L"},"agent_actions":{"view_html":"https://pith.science/pith/CALILC4LSHKLFIPTGMWBDAMY67","download_json":"https://pith.science/pith/CALILC4LSHKLFIPTGMWBDAMY67.json","view_paper":"https://pith.science/paper/CALILC4L","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2606.29770&json=true","fetch_graph":"https://pith.science/api/pith-number/CALILC4LSHKLFIPTGMWBDAMY67/graph.json","fetch_events":"https://pith.science/api/pith-number/CALILC4LSHKLFIPTGMWBDAMY67/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CALILC4LSHKLFIPTGMWBDAMY67/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CALILC4LSHKLFIPTGMWBDAMY67/action/storage_attestation","attest_author":"https://pith.science/pith/CALILC4LSHKLFIPTGMWBDAMY67/action/author_attestation","sign_citation":"https://pith.science/pith/CALILC4LSHKLFIPTGMWBDAMY67/action/citation_signature","submit_replication":"https://pith.science/pith/CALILC4LSHKLFIPTGMWBDAMY67/action/replication_record"}},"created_at":"2026-06-30T02:17:34.526092+00:00","updated_at":"2026-06-30T02:17:34.526092+00:00"}