{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:ARLWSSQSN2CKDGCZZ23XNYSKHG","short_pith_number":"pith:ARLWSSQS","schema_version":"1.0","canonical_sha256":"0457694a126e84a19859ceb776e24a39a7a564644ebff0549c003c398397b7d9","source":{"kind":"arxiv","id":"1701.05276","version":4},"attestation_state":"computed","paper":{"title":"Integrable Floquet dynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","math-ph","math.MP","quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Anatoli Polkovnikov, Vladimir Gritsev","submitted_at":"2017-01-19T01:42:26Z","abstract_excerpt":"We discuss several classes of integrable Floquet systems, i.e. systems which do not exhibit chaotic behavior even under a time dependent perturbation. The first class is associated with finite-dimensional Lie groups and infinite-dimensional generalization thereof. The second class is related to the row transfer matrices of the 2D statistical mechanics models. The third class of models, called here \"boost models\", is constructed as a periodic interchange of two Hamiltonians - one is the integrable lattice model Hamiltonian, while the second is the boost operator. The latter for known cases coin"},"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":"1701.05276","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-01-19T01:42:26Z","cross_cats_sorted":["hep-th","math-ph","math.MP","quant-ph"],"title_canon_sha256":"ea52fd3895c83b990ee02dfe4032974a62aa934da50cd2fc61c01a5a25ac5638","abstract_canon_sha256":"d4ffe62437eb01f286b2dc2b3c27726bd7b27de7d968f385eb06db7d316fdf1a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:18:04.207549Z","signature_b64":"V4xR2bGlXq6N9xOZITtzyz3ttT4mt1NcB4z3Lbt20RXW+/9WcsW+6qUjNbEG9dB/63XZ3toeeRvGHBbnW+r0Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0457694a126e84a19859ceb776e24a39a7a564644ebff0549c003c398397b7d9","last_reissued_at":"2026-05-18T00:18:04.207062Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:18:04.207062Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Integrable Floquet dynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","math-ph","math.MP","quant-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Anatoli Polkovnikov, Vladimir Gritsev","submitted_at":"2017-01-19T01:42:26Z","abstract_excerpt":"We discuss several classes of integrable Floquet systems, i.e. systems which do not exhibit chaotic behavior even under a time dependent perturbation. The first class is associated with finite-dimensional Lie groups and infinite-dimensional generalization thereof. The second class is related to the row transfer matrices of the 2D statistical mechanics models. The third class of models, called here \"boost models\", is constructed as a periodic interchange of two Hamiltonians - one is the integrable lattice model Hamiltonian, while the second is the boost operator. The latter for known cases coin"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.05276","kind":"arxiv","version":4},"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":"1701.05276","created_at":"2026-05-18T00:18:04.207149+00:00"},{"alias_kind":"arxiv_version","alias_value":"1701.05276v4","created_at":"2026-05-18T00:18:04.207149+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.05276","created_at":"2026-05-18T00:18:04.207149+00:00"},{"alias_kind":"pith_short_12","alias_value":"ARLWSSQSN2CK","created_at":"2026-05-18T12:31:08.081275+00:00"},{"alias_kind":"pith_short_16","alias_value":"ARLWSSQSN2CKDGCZ","created_at":"2026-05-18T12:31:08.081275+00:00"},{"alias_kind":"pith_short_8","alias_value":"ARLWSSQS","created_at":"2026-05-18T12:31:08.081275+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.05289","citing_title":"Emergent Spatial Structure and Entanglement Localization in Floquet Conformal Field Theory","ref_index":50,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ARLWSSQSN2CKDGCZZ23XNYSKHG","json":"https://pith.science/pith/ARLWSSQSN2CKDGCZZ23XNYSKHG.json","graph_json":"https://pith.science/api/pith-number/ARLWSSQSN2CKDGCZZ23XNYSKHG/graph.json","events_json":"https://pith.science/api/pith-number/ARLWSSQSN2CKDGCZZ23XNYSKHG/events.json","paper":"https://pith.science/paper/ARLWSSQS"},"agent_actions":{"view_html":"https://pith.science/pith/ARLWSSQSN2CKDGCZZ23XNYSKHG","download_json":"https://pith.science/pith/ARLWSSQSN2CKDGCZZ23XNYSKHG.json","view_paper":"https://pith.science/paper/ARLWSSQS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1701.05276&json=true","fetch_graph":"https://pith.science/api/pith-number/ARLWSSQSN2CKDGCZZ23XNYSKHG/graph.json","fetch_events":"https://pith.science/api/pith-number/ARLWSSQSN2CKDGCZZ23XNYSKHG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ARLWSSQSN2CKDGCZZ23XNYSKHG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ARLWSSQSN2CKDGCZZ23XNYSKHG/action/storage_attestation","attest_author":"https://pith.science/pith/ARLWSSQSN2CKDGCZZ23XNYSKHG/action/author_attestation","sign_citation":"https://pith.science/pith/ARLWSSQSN2CKDGCZZ23XNYSKHG/action/citation_signature","submit_replication":"https://pith.science/pith/ARLWSSQSN2CKDGCZZ23XNYSKHG/action/replication_record"}},"created_at":"2026-05-18T00:18:04.207149+00:00","updated_at":"2026-05-18T00:18:04.207149+00:00"}