{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:W32D37KDP3OHVDVQSSSFC32PEY","short_pith_number":"pith:W32D37KD","schema_version":"1.0","canonical_sha256":"b6f43dfd437edc7a8eb094a4516f4f260a2716d5d5b26b096ffcee09916142e3","source":{"kind":"arxiv","id":"2406.10899","version":2},"attestation_state":"computed","paper":{"title":"Notes on heating phase dynamics in Floquet CFTs and Modular quantization","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Baishali Roy, Bobby Ezhuthachan, Somnath Porey, Suchetan Das","submitted_at":"2024-06-16T11:23:22Z","abstract_excerpt":"In this article, we explore the connection between the heating phase of periodically driven CFTs and the Modular Hamiltonian of a subregion in the vacuum state. We show that the heating phase Hamiltonian corresponds to the Modular Hamiltonian, with the fixed points mapping to the endpoints of the subregion. In the bulk dual, we find that these fixed points correspond to the Ryu-Takayanagi surface of the AdS-Rindler wedge. Consequently, the entanglement entropy associated to the boundary interval within two fixed points exactly matches with the Rindler entropy of AdS-Rindler. We observe the eme"},"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":"2406.10899","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-06-16T11:23:22Z","cross_cats_sorted":[],"title_canon_sha256":"ffd338cf4978252ef29ee50d3d28ffad9a65f7d17c5c0f0b0f8bfb462e47e2c8","abstract_canon_sha256":"d087401156e68b542ad2b1343d39469424357c7f60fc56ae5001074838973628"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:42:37.206456Z","signature_b64":"tnz2BScGEdetZbIyvdatkCexMPcXuOMRfJ7mkS4uXyddfvzU3sU7y3gb16iSMVcQ4Y1kTZ2IhFUrWIP6Ee/lDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b6f43dfd437edc7a8eb094a4516f4f260a2716d5d5b26b096ffcee09916142e3","last_reissued_at":"2026-07-05T08:42:37.205954Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:42:37.205954Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Notes on heating phase dynamics in Floquet CFTs and Modular quantization","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Baishali Roy, Bobby Ezhuthachan, Somnath Porey, Suchetan Das","submitted_at":"2024-06-16T11:23:22Z","abstract_excerpt":"In this article, we explore the connection between the heating phase of periodically driven CFTs and the Modular Hamiltonian of a subregion in the vacuum state. We show that the heating phase Hamiltonian corresponds to the Modular Hamiltonian, with the fixed points mapping to the endpoints of the subregion. In the bulk dual, we find that these fixed points correspond to the Ryu-Takayanagi surface of the AdS-Rindler wedge. Consequently, the entanglement entropy associated to the boundary interval within two fixed points exactly matches with the Rindler entropy of AdS-Rindler. We observe the eme"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.10899","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/2406.10899/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":"2406.10899","created_at":"2026-07-05T08:42:37.206042+00:00"},{"alias_kind":"arxiv_version","alias_value":"2406.10899v2","created_at":"2026-07-05T08:42:37.206042+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.10899","created_at":"2026-07-05T08:42:37.206042+00:00"},{"alias_kind":"pith_short_12","alias_value":"W32D37KDP3OH","created_at":"2026-07-05T08:42:37.206042+00:00"},{"alias_kind":"pith_short_16","alias_value":"W32D37KDP3OHVDVQ","created_at":"2026-07-05T08:42:37.206042+00:00"},{"alias_kind":"pith_short_8","alias_value":"W32D37KD","created_at":"2026-07-05T08:42:37.206042+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.11984","citing_title":"Modular quantization and black holes","ref_index":56,"is_internal_anchor":false},{"citing_arxiv_id":"2605.26250","citing_title":"Krylov Complexity in Periodically Driven CFTs and Critical Fermions","ref_index":51,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/W32D37KDP3OHVDVQSSSFC32PEY","json":"https://pith.science/pith/W32D37KDP3OHVDVQSSSFC32PEY.json","graph_json":"https://pith.science/api/pith-number/W32D37KDP3OHVDVQSSSFC32PEY/graph.json","events_json":"https://pith.science/api/pith-number/W32D37KDP3OHVDVQSSSFC32PEY/events.json","paper":"https://pith.science/paper/W32D37KD"},"agent_actions":{"view_html":"https://pith.science/pith/W32D37KDP3OHVDVQSSSFC32PEY","download_json":"https://pith.science/pith/W32D37KDP3OHVDVQSSSFC32PEY.json","view_paper":"https://pith.science/paper/W32D37KD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2406.10899&json=true","fetch_graph":"https://pith.science/api/pith-number/W32D37KDP3OHVDVQSSSFC32PEY/graph.json","fetch_events":"https://pith.science/api/pith-number/W32D37KDP3OHVDVQSSSFC32PEY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/W32D37KDP3OHVDVQSSSFC32PEY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/W32D37KDP3OHVDVQSSSFC32PEY/action/storage_attestation","attest_author":"https://pith.science/pith/W32D37KDP3OHVDVQSSSFC32PEY/action/author_attestation","sign_citation":"https://pith.science/pith/W32D37KDP3OHVDVQSSSFC32PEY/action/citation_signature","submit_replication":"https://pith.science/pith/W32D37KDP3OHVDVQSSSFC32PEY/action/replication_record"}},"created_at":"2026-07-05T08:42:37.206042+00:00","updated_at":"2026-07-05T08:42:37.206042+00:00"}