{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:BPJLWNLKZULSDMUNRW5SKUKZTR","short_pith_number":"pith:BPJLWNLK","schema_version":"1.0","canonical_sha256":"0bd2bb356acd1721b28d8dbb2551599c54357e16d317a93ff73f0ec5c0eb64e9","source":{"kind":"arxiv","id":"2505.06420","version":1},"attestation_state":"computed","paper":{"title":"The spectrum of pure dS$_3$ gravity in the static patch","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Alexander Maloney, Joydeep Chakravarty, Keivan Namjou, Simon F. Ross","submitted_at":"2025-05-09T20:40:09Z","abstract_excerpt":"We consider the quantum mechanical description of the de Sitter static patch in three-dimensional general relativity. We consider a Lorentzian path integral that conjecturally computes the Fourier transform of the spectrum of the static patch Hamiltonian. We regulate a saddle point for this integral by a complex deformation that connects it to future infinity. Our computation is thus closely connected with the wave function of de Sitter gravity on a torus at future infinity. Motivated by this, we identify an infinite number of saddle points that contribute to our Lorentzian path integral. Thei"},"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":"2505.06420","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2025-05-09T20:40:09Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"69410dbb14e3ff288c99944e333c5c737795eb774d8f358332f75325350da4b2","abstract_canon_sha256":"cd45614040e94df1808add7704920f0de4a5513c6aa2cbc7450b77f1b7224bdb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:01:09.246779Z","signature_b64":"CBOtK0pe+9MzTTm4YjRkhKihHiDB+j9YZBx/JBfPzzzFc/Xb9PUV4Y01D9ES7gBLQGmUeoUaywMnssNTxAN0BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0bd2bb356acd1721b28d8dbb2551599c54357e16d317a93ff73f0ec5c0eb64e9","last_reissued_at":"2026-07-05T11:01:09.246284Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:01:09.246284Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The spectrum of pure dS$_3$ gravity in the static patch","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Alexander Maloney, Joydeep Chakravarty, Keivan Namjou, Simon F. Ross","submitted_at":"2025-05-09T20:40:09Z","abstract_excerpt":"We consider the quantum mechanical description of the de Sitter static patch in three-dimensional general relativity. We consider a Lorentzian path integral that conjecturally computes the Fourier transform of the spectrum of the static patch Hamiltonian. We regulate a saddle point for this integral by a complex deformation that connects it to future infinity. Our computation is thus closely connected with the wave function of de Sitter gravity on a torus at future infinity. Motivated by this, we identify an infinite number of saddle points that contribute to our Lorentzian path integral. Thei"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.06420","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2505.06420/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":"2505.06420","created_at":"2026-07-05T11:01:09.246354+00:00"},{"alias_kind":"arxiv_version","alias_value":"2505.06420v1","created_at":"2026-07-05T11:01:09.246354+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.06420","created_at":"2026-07-05T11:01:09.246354+00:00"},{"alias_kind":"pith_short_12","alias_value":"BPJLWNLKZULS","created_at":"2026-07-05T11:01:09.246354+00:00"},{"alias_kind":"pith_short_16","alias_value":"BPJLWNLKZULSDMUN","created_at":"2026-07-05T11:01:09.246354+00:00"},{"alias_kind":"pith_short_8","alias_value":"BPJLWNLK","created_at":"2026-07-05T11:01:09.246354+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.26241","citing_title":"An observer's quantization of 3d de Sitter","ref_index":31,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BPJLWNLKZULSDMUNRW5SKUKZTR","json":"https://pith.science/pith/BPJLWNLKZULSDMUNRW5SKUKZTR.json","graph_json":"https://pith.science/api/pith-number/BPJLWNLKZULSDMUNRW5SKUKZTR/graph.json","events_json":"https://pith.science/api/pith-number/BPJLWNLKZULSDMUNRW5SKUKZTR/events.json","paper":"https://pith.science/paper/BPJLWNLK"},"agent_actions":{"view_html":"https://pith.science/pith/BPJLWNLKZULSDMUNRW5SKUKZTR","download_json":"https://pith.science/pith/BPJLWNLKZULSDMUNRW5SKUKZTR.json","view_paper":"https://pith.science/paper/BPJLWNLK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2505.06420&json=true","fetch_graph":"https://pith.science/api/pith-number/BPJLWNLKZULSDMUNRW5SKUKZTR/graph.json","fetch_events":"https://pith.science/api/pith-number/BPJLWNLKZULSDMUNRW5SKUKZTR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BPJLWNLKZULSDMUNRW5SKUKZTR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BPJLWNLKZULSDMUNRW5SKUKZTR/action/storage_attestation","attest_author":"https://pith.science/pith/BPJLWNLKZULSDMUNRW5SKUKZTR/action/author_attestation","sign_citation":"https://pith.science/pith/BPJLWNLKZULSDMUNRW5SKUKZTR/action/citation_signature","submit_replication":"https://pith.science/pith/BPJLWNLKZULSDMUNRW5SKUKZTR/action/replication_record"}},"created_at":"2026-07-05T11:01:09.246354+00:00","updated_at":"2026-07-05T11:01:09.246354+00:00"}