{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:BNFVJBHIXBEUUSLCXG2QOM746V","short_pith_number":"pith:BNFVJBHI","schema_version":"1.0","canonical_sha256":"0b4b5484e8b8494a4962b9b50733fcf5500be698e69e6c74e66656d52ad2c01b","source":{"kind":"arxiv","id":"2011.09491","version":3},"attestation_state":"computed","paper":{"title":"Floquet conformal field theories with generally deformed Hamiltonians","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.stat-mech","cond-mat.str-el","math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Ashvin Vishwanath, Ruihua Fan, Xueda Wen, Yingfei Gu","submitted_at":"2020-11-18T19:01:42Z","abstract_excerpt":"In this work, we study non-equilibrium dynamics in Floquet conformal field theories (CFTs) in 1+1D, in which the driving Hamiltonian involves the energy-momentum density spatially modulated by an arbitrary smooth function. This generalizes earlier work which was restricted to the sine-square deformed type of Floquet Hamiltonians, operating within a $\\mathfrak{sl}_2$ sub-algebra. Here we show remarkably that the problem remains soluble in this generalized case which involves the full Virasoro algebra, based on a geometrical approach. It is found that the phase diagram is determined by the strob"},"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":"2011.09491","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2020-11-18T19:01:42Z","cross_cats_sorted":["cond-mat.stat-mech","cond-mat.str-el","math-ph","math.MP"],"title_canon_sha256":"b40d51d867bef76472ab461e76be88d5e4cdf5b89c7e19f3b23070ddc02cbf5b","abstract_canon_sha256":"a8b47145699ffff418704775e17daf83a77a5556a996192afb7e11ef9746c795"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:19:38.493064Z","signature_b64":"X73rPspKAzHLBRyl54WyRtJb22fUu3Nd6/iw+zJgkzD+wfPTMWOp85Pma3lSgNJGFP9NP9FlfsSShww0WjzkCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0b4b5484e8b8494a4962b9b50733fcf5500be698e69e6c74e66656d52ad2c01b","last_reissued_at":"2026-07-05T02:19:38.492620Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:19:38.492620Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Floquet conformal field theories with generally deformed Hamiltonians","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.stat-mech","cond-mat.str-el","math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Ashvin Vishwanath, Ruihua Fan, Xueda Wen, Yingfei Gu","submitted_at":"2020-11-18T19:01:42Z","abstract_excerpt":"In this work, we study non-equilibrium dynamics in Floquet conformal field theories (CFTs) in 1+1D, in which the driving Hamiltonian involves the energy-momentum density spatially modulated by an arbitrary smooth function. This generalizes earlier work which was restricted to the sine-square deformed type of Floquet Hamiltonians, operating within a $\\mathfrak{sl}_2$ sub-algebra. Here we show remarkably that the problem remains soluble in this generalized case which involves the full Virasoro algebra, based on a geometrical approach. It is found that the phase diagram is determined by the strob"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2011.09491","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2011.09491/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":"2011.09491","created_at":"2026-07-05T02:19:38.492673+00:00"},{"alias_kind":"arxiv_version","alias_value":"2011.09491v3","created_at":"2026-07-05T02:19:38.492673+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2011.09491","created_at":"2026-07-05T02:19:38.492673+00:00"},{"alias_kind":"pith_short_12","alias_value":"BNFVJBHIXBEU","created_at":"2026-07-05T02:19:38.492673+00:00"},{"alias_kind":"pith_short_16","alias_value":"BNFVJBHIXBEUUSLC","created_at":"2026-07-05T02:19:38.492673+00:00"},{"alias_kind":"pith_short_8","alias_value":"BNFVJBHI","created_at":"2026-07-05T02:19:38.492673+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.26250","citing_title":"Krylov Complexity in Periodically Driven CFTs and Critical Fermions","ref_index":41,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BNFVJBHIXBEUUSLCXG2QOM746V","json":"https://pith.science/pith/BNFVJBHIXBEUUSLCXG2QOM746V.json","graph_json":"https://pith.science/api/pith-number/BNFVJBHIXBEUUSLCXG2QOM746V/graph.json","events_json":"https://pith.science/api/pith-number/BNFVJBHIXBEUUSLCXG2QOM746V/events.json","paper":"https://pith.science/paper/BNFVJBHI"},"agent_actions":{"view_html":"https://pith.science/pith/BNFVJBHIXBEUUSLCXG2QOM746V","download_json":"https://pith.science/pith/BNFVJBHIXBEUUSLCXG2QOM746V.json","view_paper":"https://pith.science/paper/BNFVJBHI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2011.09491&json=true","fetch_graph":"https://pith.science/api/pith-number/BNFVJBHIXBEUUSLCXG2QOM746V/graph.json","fetch_events":"https://pith.science/api/pith-number/BNFVJBHIXBEUUSLCXG2QOM746V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BNFVJBHIXBEUUSLCXG2QOM746V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BNFVJBHIXBEUUSLCXG2QOM746V/action/storage_attestation","attest_author":"https://pith.science/pith/BNFVJBHIXBEUUSLCXG2QOM746V/action/author_attestation","sign_citation":"https://pith.science/pith/BNFVJBHIXBEUUSLCXG2QOM746V/action/citation_signature","submit_replication":"https://pith.science/pith/BNFVJBHIXBEUUSLCXG2QOM746V/action/replication_record"}},"created_at":"2026-07-05T02:19:38.492673+00:00","updated_at":"2026-07-05T02:19:38.492673+00:00"}