{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:HZQ4VQPLTBH57DNQ3S4BEL4BSY","short_pith_number":"pith:HZQ4VQPL","schema_version":"1.0","canonical_sha256":"3e61cac1eb984fdf8db0dcb8122f81960a8e6120fe6aa8f76cae6fbd0121e36d","source":{"kind":"arxiv","id":"2411.16922","version":2},"attestation_state":"computed","paper":{"title":"An entropic puzzle in periodic dilaton gravity and DSSYK","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Adam Levine, Andreas Blommaert, Jacopo Papalini, Klaas Parmentier, Thomas G. Mertens","submitted_at":"2024-11-25T20:45:46Z","abstract_excerpt":"We study 2d dilaton gravity theories with a periodic potential, with special emphasis on sine dilaton gravity, which is holographically dual to double-scaled SYK. The periodicity of the potentials implies a symmetry under (discrete) shifts in the momentum conjugate to the length of geodesic slices. This results in divergences. The correct definition is to gauge this symmetry. This discretizes the geodesic lengths. Lengths below a certain threshold are null states. Because of these null states, the entropy deviates drastically from Bekenstein-Hawking and the Hilbert space becomes finite dimensi"},"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":"2411.16922","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2024-11-25T20:45:46Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"190077eafb557f6584b09930a05e6b576a93a4dd714dd698fbf2f1029907d90b","abstract_canon_sha256":"198dfd14c9a3bf14ca494acfa828d66a4cb2844b104aed60e913b5c153a86149"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:57:54.850360Z","signature_b64":"dydAxXT2pbjsJbMhbDyciAntASM4kQPtPEIkP3ktr9LfwgjjzU1tQVp+1lxBZHiuYxaXqyWS9KzuWbqVPhqqCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3e61cac1eb984fdf8db0dcb8122f81960a8e6120fe6aa8f76cae6fbd0121e36d","last_reissued_at":"2026-07-05T10:57:54.849860Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:57:54.849860Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"An entropic puzzle in periodic dilaton gravity and DSSYK","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Adam Levine, Andreas Blommaert, Jacopo Papalini, Klaas Parmentier, Thomas G. Mertens","submitted_at":"2024-11-25T20:45:46Z","abstract_excerpt":"We study 2d dilaton gravity theories with a periodic potential, with special emphasis on sine dilaton gravity, which is holographically dual to double-scaled SYK. The periodicity of the potentials implies a symmetry under (discrete) shifts in the momentum conjugate to the length of geodesic slices. This results in divergences. The correct definition is to gauge this symmetry. This discretizes the geodesic lengths. Lengths below a certain threshold are null states. Because of these null states, the entropy deviates drastically from Bekenstein-Hawking and the Hilbert space becomes finite dimensi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.16922","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/2411.16922/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":"2411.16922","created_at":"2026-07-05T10:57:54.849915+00:00"},{"alias_kind":"arxiv_version","alias_value":"2411.16922v2","created_at":"2026-07-05T10:57:54.849915+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.16922","created_at":"2026-07-05T10:57:54.849915+00:00"},{"alias_kind":"pith_short_12","alias_value":"HZQ4VQPLTBH5","created_at":"2026-07-05T10:57:54.849915+00:00"},{"alias_kind":"pith_short_16","alias_value":"HZQ4VQPLTBH57DNQ","created_at":"2026-07-05T10:57:54.849915+00:00"},{"alias_kind":"pith_short_8","alias_value":"HZQ4VQPL","created_at":"2026-07-05T10:57:54.849915+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":15,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.26241","citing_title":"An observer's quantization of 3d de Sitter","ref_index":65,"is_internal_anchor":false},{"citing_arxiv_id":"2606.20220","citing_title":"Higher-loop wormhole length in sine-dilaton gravity from DSSYK Krylov complexity","ref_index":15,"is_internal_anchor":false},{"citing_arxiv_id":"2606.18739","citing_title":"ASEP/DSSYK duality and strange correlator","ref_index":37,"is_internal_anchor":false},{"citing_arxiv_id":"2606.03049","citing_title":"Holographic complexity of de-Sitter black holes","ref_index":128,"is_internal_anchor":false},{"citing_arxiv_id":"2605.13956","citing_title":"q-Askey Deformations of Double-Scaled SYK","ref_index":12,"is_internal_anchor":false},{"citing_arxiv_id":"2606.20220","citing_title":"Higher-loop wormhole length in sine-dilaton gravity from DSSYK Krylov complexity","ref_index":15,"is_internal_anchor":false},{"citing_arxiv_id":"2506.02109","citing_title":"Towards a microscopic description of de Sitter dynamics","ref_index":40,"is_internal_anchor":false},{"citing_arxiv_id":"2509.03930","citing_title":"Cap amplitudes in random matrix models","ref_index":9,"is_internal_anchor":false},{"citing_arxiv_id":"2510.22658","citing_title":"Toward Krylov-based holography in double-scaled SYK","ref_index":40,"is_internal_anchor":false},{"citing_arxiv_id":"2511.03779","citing_title":"Cosmological Entanglement Entropy from the von Neumann Algebra of Double-Scaled SYK & Its Connection with Krylov Complexity","ref_index":56,"is_internal_anchor":false},{"citing_arxiv_id":"2512.10101","citing_title":"The von Neumann algebraic quantum group $\\mathrm{SU}_q(1,1)\\rtimes \\mathbb{Z}_2$ and the DSSYK model","ref_index":27,"is_internal_anchor":false},{"citing_arxiv_id":"2601.09801","citing_title":"Probing the Chaos to Integrability Transition in Double-Scaled SYK","ref_index":44,"is_internal_anchor":false},{"citing_arxiv_id":"2602.06113","citing_title":"Deforming the Double-Scaled SYK & Reaching the Stretched Horizon From Finite Cutoff Holography","ref_index":109,"is_internal_anchor":false},{"citing_arxiv_id":"2605.13956","citing_title":"q-Askey Deformations of Double-Scaled SYK","ref_index":12,"is_internal_anchor":false},{"citing_arxiv_id":"2604.14387","citing_title":"Emergent States and Algebras from the Double-Scaling limit of Pure States in SYK","ref_index":86,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HZQ4VQPLTBH57DNQ3S4BEL4BSY","json":"https://pith.science/pith/HZQ4VQPLTBH57DNQ3S4BEL4BSY.json","graph_json":"https://pith.science/api/pith-number/HZQ4VQPLTBH57DNQ3S4BEL4BSY/graph.json","events_json":"https://pith.science/api/pith-number/HZQ4VQPLTBH57DNQ3S4BEL4BSY/events.json","paper":"https://pith.science/paper/HZQ4VQPL"},"agent_actions":{"view_html":"https://pith.science/pith/HZQ4VQPLTBH57DNQ3S4BEL4BSY","download_json":"https://pith.science/pith/HZQ4VQPLTBH57DNQ3S4BEL4BSY.json","view_paper":"https://pith.science/paper/HZQ4VQPL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2411.16922&json=true","fetch_graph":"https://pith.science/api/pith-number/HZQ4VQPLTBH57DNQ3S4BEL4BSY/graph.json","fetch_events":"https://pith.science/api/pith-number/HZQ4VQPLTBH57DNQ3S4BEL4BSY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HZQ4VQPLTBH57DNQ3S4BEL4BSY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HZQ4VQPLTBH57DNQ3S4BEL4BSY/action/storage_attestation","attest_author":"https://pith.science/pith/HZQ4VQPLTBH57DNQ3S4BEL4BSY/action/author_attestation","sign_citation":"https://pith.science/pith/HZQ4VQPLTBH57DNQ3S4BEL4BSY/action/citation_signature","submit_replication":"https://pith.science/pith/HZQ4VQPLTBH57DNQ3S4BEL4BSY/action/replication_record"}},"created_at":"2026-07-05T10:57:54.849915+00:00","updated_at":"2026-07-05T10:57:54.849915+00:00"}