{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:RSF3EJXLFDUWQDKGXBNCPVN5R6","short_pith_number":"pith:RSF3EJXL","canonical_record":{"source":{"id":"1711.09945","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-11-27T19:31:58Z","cross_cats_sorted":["cond-mat.mes-hall","math-ph","math.MP"],"title_canon_sha256":"368799dec5490b2da5ebcaae9d11fe3e612981e1c9fab716768a9b405f7fc5f1","abstract_canon_sha256":"d04afdad3a6baf547b0a532bab5d22d062ef2c7899782b4694e87d707198d6d8"},"schema_version":"1.0"},"canonical_sha256":"8c8bb226eb28e9680d46b85a27d5bd8fa84c86f0c5cc0a48747659159afb477b","source":{"kind":"arxiv","id":"1711.09945","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.09945","created_at":"2026-05-18T00:15:58Z"},{"alias_kind":"arxiv_version","alias_value":"1711.09945v1","created_at":"2026-05-18T00:15:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.09945","created_at":"2026-05-18T00:15:58Z"},{"alias_kind":"pith_short_12","alias_value":"RSF3EJXLFDUW","created_at":"2026-05-18T12:31:39Z"},{"alias_kind":"pith_short_16","alias_value":"RSF3EJXLFDUWQDKG","created_at":"2026-05-18T12:31:39Z"},{"alias_kind":"pith_short_8","alias_value":"RSF3EJXL","created_at":"2026-05-18T12:31:39Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:RSF3EJXLFDUWQDKGXBNCPVN5R6","target":"record","payload":{"canonical_record":{"source":{"id":"1711.09945","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-11-27T19:31:58Z","cross_cats_sorted":["cond-mat.mes-hall","math-ph","math.MP"],"title_canon_sha256":"368799dec5490b2da5ebcaae9d11fe3e612981e1c9fab716768a9b405f7fc5f1","abstract_canon_sha256":"d04afdad3a6baf547b0a532bab5d22d062ef2c7899782b4694e87d707198d6d8"},"schema_version":"1.0"},"canonical_sha256":"8c8bb226eb28e9680d46b85a27d5bd8fa84c86f0c5cc0a48747659159afb477b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:15:58.593364Z","signature_b64":"2D2+LnlnFjHTvLLQ/sqXzC9EIN4l4ikQnYwaT3hSaRAOnhkVNXGeTKaQbwE1OPRIEvJOrXDpUveCceapjgbJDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8c8bb226eb28e9680d46b85a27d5bd8fa84c86f0c5cc0a48747659159afb477b","last_reissued_at":"2026-05-18T00:15:58.592814Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:15:58.592814Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1711.09945","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":"2026-05-18T00:15:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ip7A/OlQSvi92jGzWfp1YW5Be7coo/UI1nih5lJ8Bi10A579aU4w8t/6vfZ7AYHbduSQAKCjOvd12sVLvxfqCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T13:04:01.358803Z"},"content_sha256":"83ab78261ef426089f8deb4f750ea06c6d60fa338ea88b452bdfcef3fcb642d7","schema_version":"1.0","event_id":"sha256:83ab78261ef426089f8deb4f750ea06c6d60fa338ea88b452bdfcef3fcb642d7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:RSF3EJXLFDUWQDKGXBNCPVN5R6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Integrable time-dependent quantum Hamiltonians","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","math-ph","math.MP"],"primary_cat":"quant-ph","authors_text":"Aniket Patra, Chen Sun, Emil A. Yuzbashyan, Nikolai A. Sinitsyn, Vladimir Y. Chernyak","submitted_at":"2017-11-27T19:31:58Z","abstract_excerpt":"We formulate a set of conditions under which dynamics of a time-dependent quantum Hamiltonian are integrable. The main requirement is the existence of a nonabelian gauge field with zero curvature in the space of system parameters. Known solvable multistate Landau-Zener models satisfy these conditions. Our method provides a strategy to incorporate time-dependence into various quantum integrable models, so that the resulting non-stationary Schrodinger equation is exactly solvable. We also validate some prior conjectures, including the solution of the driven generalized Tavis-Cummings model."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.09945","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":""},"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":"2026-05-18T00:15:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WdvjxV30VHNaTG7vCm1VGxA8Qwe7ABZFJNgrGrNnTBmwkUWl3uvLCpW8k5UehSDDkHiBu8Wwb/gNWSJw5sZiBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T13:04:01.359424Z"},"content_sha256":"6d5633c13c897b8a12bb8031f0efe84423e4166dcc634614ec4d921f6c9bf26f","schema_version":"1.0","event_id":"sha256:6d5633c13c897b8a12bb8031f0efe84423e4166dcc634614ec4d921f6c9bf26f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RSF3EJXLFDUWQDKGXBNCPVN5R6/bundle.json","state_url":"https://pith.science/pith/RSF3EJXLFDUWQDKGXBNCPVN5R6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RSF3EJXLFDUWQDKGXBNCPVN5R6/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":"2026-05-31T13:04:01Z","links":{"resolver":"https://pith.science/pith/RSF3EJXLFDUWQDKGXBNCPVN5R6","bundle":"https://pith.science/pith/RSF3EJXLFDUWQDKGXBNCPVN5R6/bundle.json","state":"https://pith.science/pith/RSF3EJXLFDUWQDKGXBNCPVN5R6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RSF3EJXLFDUWQDKGXBNCPVN5R6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:RSF3EJXLFDUWQDKGXBNCPVN5R6","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":"d04afdad3a6baf547b0a532bab5d22d062ef2c7899782b4694e87d707198d6d8","cross_cats_sorted":["cond-mat.mes-hall","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-11-27T19:31:58Z","title_canon_sha256":"368799dec5490b2da5ebcaae9d11fe3e612981e1c9fab716768a9b405f7fc5f1"},"schema_version":"1.0","source":{"id":"1711.09945","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1711.09945","created_at":"2026-05-18T00:15:58Z"},{"alias_kind":"arxiv_version","alias_value":"1711.09945v1","created_at":"2026-05-18T00:15:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.09945","created_at":"2026-05-18T00:15:58Z"},{"alias_kind":"pith_short_12","alias_value":"RSF3EJXLFDUW","created_at":"2026-05-18T12:31:39Z"},{"alias_kind":"pith_short_16","alias_value":"RSF3EJXLFDUWQDKG","created_at":"2026-05-18T12:31:39Z"},{"alias_kind":"pith_short_8","alias_value":"RSF3EJXL","created_at":"2026-05-18T12:31:39Z"}],"graph_snapshots":[{"event_id":"sha256:6d5633c13c897b8a12bb8031f0efe84423e4166dcc634614ec4d921f6c9bf26f","target":"graph","created_at":"2026-05-18T00:15:58Z","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":"We formulate a set of conditions under which dynamics of a time-dependent quantum Hamiltonian are integrable. The main requirement is the existence of a nonabelian gauge field with zero curvature in the space of system parameters. Known solvable multistate Landau-Zener models satisfy these conditions. Our method provides a strategy to incorporate time-dependence into various quantum integrable models, so that the resulting non-stationary Schrodinger equation is exactly solvable. We also validate some prior conjectures, including the solution of the driven generalized Tavis-Cummings model.","authors_text":"Aniket Patra, Chen Sun, Emil A. Yuzbashyan, Nikolai A. Sinitsyn, Vladimir Y. Chernyak","cross_cats":["cond-mat.mes-hall","math-ph","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-11-27T19:31:58Z","title":"Integrable time-dependent quantum Hamiltonians"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.09945","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":"sha256:83ab78261ef426089f8deb4f750ea06c6d60fa338ea88b452bdfcef3fcb642d7","target":"record","created_at":"2026-05-18T00:15:58Z","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":"d04afdad3a6baf547b0a532bab5d22d062ef2c7899782b4694e87d707198d6d8","cross_cats_sorted":["cond-mat.mes-hall","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-11-27T19:31:58Z","title_canon_sha256":"368799dec5490b2da5ebcaae9d11fe3e612981e1c9fab716768a9b405f7fc5f1"},"schema_version":"1.0","source":{"id":"1711.09945","kind":"arxiv","version":1}},"canonical_sha256":"8c8bb226eb28e9680d46b85a27d5bd8fa84c86f0c5cc0a48747659159afb477b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8c8bb226eb28e9680d46b85a27d5bd8fa84c86f0c5cc0a48747659159afb477b","first_computed_at":"2026-05-18T00:15:58.592814Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:15:58.592814Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2D2+LnlnFjHTvLLQ/sqXzC9EIN4l4ikQnYwaT3hSaRAOnhkVNXGeTKaQbwE1OPRIEvJOrXDpUveCceapjgbJDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:15:58.593364Z","signed_message":"canonical_sha256_bytes"},"source_id":"1711.09945","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:83ab78261ef426089f8deb4f750ea06c6d60fa338ea88b452bdfcef3fcb642d7","sha256:6d5633c13c897b8a12bb8031f0efe84423e4166dcc634614ec4d921f6c9bf26f"],"state_sha256":"eb02b63edc0f91002f72ff1bb27a97efc8b8a7965171a9c542258509723a6772"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"P4LIuXOPJdBzudRAenC1ZMtOfIJ3dZa3Z0jWG5L2oGLAoGPcTKSy2v1AhdcCjiLSOjvJM8YvmJ+nP4/NPbvdDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T13:04:01.363249Z","bundle_sha256":"1ba6a54ab466f940b0501111a937472d917977a59a9be64d0bcfc81c2668cc91"}}