{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:3VHJYRIVHJGONZSZRLTFB5AXUF","short_pith_number":"pith:3VHJYRIV","schema_version":"1.0","canonical_sha256":"dd4e9c45153a4ce6e6598ae650f417a174183d1c578107dd0a6c2968bb814a5c","source":{"kind":"arxiv","id":"2501.10641","version":2},"attestation_state":"computed","paper":{"title":"Asymptotic errors in adiabatic evolution","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Hyunwoo Oh, Thomas D. Cohen","submitted_at":"2025-01-18T03:02:56Z","abstract_excerpt":"The adiabatic theorem in quantum mechanics implies that if a system is in a discrete eigenstate of a Hamiltonian and the Hamiltonian evolves in time arbitrarily slowly, the system will remain in the corresponding eigenstate of the evolved Hamiltonian. Understanding corrections to the adiabatic result that arise when the evolution of the Hamiltonian is slow -- but not arbitrarily slow -- has become increasingly important, especially since adiabatic evolution has been proposed as a method of state preparation in quantum computing. This paper identifies two regimes, an adiabatic regime in which c"},"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":"2501.10641","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2025-01-18T03:02:56Z","cross_cats_sorted":[],"title_canon_sha256":"b40566941c8c3fbfd8436edf0f230e3696077b7318994c26d056883ea467c60b","abstract_canon_sha256":"773571e12c0e54e3756301c649486292476b633e1d86a8b321f32638c12918f2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:42:42.544619Z","signature_b64":"ACitPxbceRoudpQgtVyEfoUxHjOzR3wvdBELV+w552mxAEVtoUAzeIQNgwzYVtYAuNqx3X+WEmqm39jSVzeACg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dd4e9c45153a4ce6e6598ae650f417a174183d1c578107dd0a6c2968bb814a5c","last_reissued_at":"2026-07-05T10:42:42.544126Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:42:42.544126Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Asymptotic errors in adiabatic evolution","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Hyunwoo Oh, Thomas D. Cohen","submitted_at":"2025-01-18T03:02:56Z","abstract_excerpt":"The adiabatic theorem in quantum mechanics implies that if a system is in a discrete eigenstate of a Hamiltonian and the Hamiltonian evolves in time arbitrarily slowly, the system will remain in the corresponding eigenstate of the evolved Hamiltonian. Understanding corrections to the adiabatic result that arise when the evolution of the Hamiltonian is slow -- but not arbitrarily slow -- has become increasingly important, especially since adiabatic evolution has been proposed as a method of state preparation in quantum computing. This paper identifies two regimes, an adiabatic regime in which c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.10641","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2501.10641/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":"2501.10641","created_at":"2026-07-05T10:42:42.544191+00:00"},{"alias_kind":"arxiv_version","alias_value":"2501.10641v2","created_at":"2026-07-05T10:42:42.544191+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.10641","created_at":"2026-07-05T10:42:42.544191+00:00"},{"alias_kind":"pith_short_12","alias_value":"3VHJYRIVHJGO","created_at":"2026-07-05T10:42:42.544191+00:00"},{"alias_kind":"pith_short_16","alias_value":"3VHJYRIVHJGONZSZ","created_at":"2026-07-05T10:42:42.544191+00:00"},{"alias_kind":"pith_short_8","alias_value":"3VHJYRIV","created_at":"2026-07-05T10:42:42.544191+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/3VHJYRIVHJGONZSZRLTFB5AXUF","json":"https://pith.science/pith/3VHJYRIVHJGONZSZRLTFB5AXUF.json","graph_json":"https://pith.science/api/pith-number/3VHJYRIVHJGONZSZRLTFB5AXUF/graph.json","events_json":"https://pith.science/api/pith-number/3VHJYRIVHJGONZSZRLTFB5AXUF/events.json","paper":"https://pith.science/paper/3VHJYRIV"},"agent_actions":{"view_html":"https://pith.science/pith/3VHJYRIVHJGONZSZRLTFB5AXUF","download_json":"https://pith.science/pith/3VHJYRIVHJGONZSZRLTFB5AXUF.json","view_paper":"https://pith.science/paper/3VHJYRIV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2501.10641&json=true","fetch_graph":"https://pith.science/api/pith-number/3VHJYRIVHJGONZSZRLTFB5AXUF/graph.json","fetch_events":"https://pith.science/api/pith-number/3VHJYRIVHJGONZSZRLTFB5AXUF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3VHJYRIVHJGONZSZRLTFB5AXUF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3VHJYRIVHJGONZSZRLTFB5AXUF/action/storage_attestation","attest_author":"https://pith.science/pith/3VHJYRIVHJGONZSZRLTFB5AXUF/action/author_attestation","sign_citation":"https://pith.science/pith/3VHJYRIVHJGONZSZRLTFB5AXUF/action/citation_signature","submit_replication":"https://pith.science/pith/3VHJYRIVHJGONZSZRLTFB5AXUF/action/replication_record"}},"created_at":"2026-07-05T10:42:42.544191+00:00","updated_at":"2026-07-05T10:42:42.544191+00:00"}