{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:GPT2MR6USKNN7Y7D7X4AHNXSN7","short_pith_number":"pith:GPT2MR6U","schema_version":"1.0","canonical_sha256":"33e7a647d4929adfe3e3fdf803b6f26fed7f33e689a2bf13c13ef8007977f61a","source":{"kind":"arxiv","id":"2607.14042","version":1},"attestation_state":"computed","paper":{"title":"Negative shocks versus static patch holography","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Douglas Stanford, Haifeng Tang, Yiming Chen, Zhenbin Yang","submitted_at":"2026-07-15T17:13:10Z","abstract_excerpt":"We study a version of de Sitter static patch holography in which the Euclidean gravitational path integral, with an observer worldline included, is conjectured to compute a trace. Motivated by recent evidence for this conjecture from the sphere path integral, we test it further by inserting operators along the observer worldline and computing two-point functions and out-of-time-ordered four-point correlators (OTOCs). We extend an earlier OTOC calculation by Kolchmeyer and Liu using the shockwave formalism, incorporating both observer recoil and gravitational backreaction. We find that the OTOC"},"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":"2607.14042","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2026-07-15T17:13:10Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"5c4a8733eaf5590f49faf9bed01f55c1ed7ff2e29d64577ec140c517b6afdc08","abstract_canon_sha256":"d5e3ba3d691a7371e5a4b5584d718784bf4d651aadcb6366cb9e52d9de7701cb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-16T01:23:21.135249Z","signature_b64":"NHm4OA3u+TzLHwnHH7Ef+pl8oW/KVf1OgJflh5ZkJZHZHfW7Jb1w+Fmvd4lZR5aV+ktYz55g8or/d8cSV9XbAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"33e7a647d4929adfe3e3fdf803b6f26fed7f33e689a2bf13c13ef8007977f61a","last_reissued_at":"2026-07-16T01:23:21.134442Z","signature_status":"signed_v1","first_computed_at":"2026-07-16T01:23:21.134442Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Negative shocks versus static patch holography","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Douglas Stanford, Haifeng Tang, Yiming Chen, Zhenbin Yang","submitted_at":"2026-07-15T17:13:10Z","abstract_excerpt":"We study a version of de Sitter static patch holography in which the Euclidean gravitational path integral, with an observer worldline included, is conjectured to compute a trace. Motivated by recent evidence for this conjecture from the sphere path integral, we test it further by inserting operators along the observer worldline and computing two-point functions and out-of-time-ordered four-point correlators (OTOCs). We extend an earlier OTOC calculation by Kolchmeyer and Liu using the shockwave formalism, incorporating both observer recoil and gravitational backreaction. We find that the OTOC"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.14042","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/2607.14042/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":"2607.14042","created_at":"2026-07-16T01:23:21.134865+00:00"},{"alias_kind":"arxiv_version","alias_value":"2607.14042v1","created_at":"2026-07-16T01:23:21.134865+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.14042","created_at":"2026-07-16T01:23:21.134865+00:00"},{"alias_kind":"pith_short_12","alias_value":"GPT2MR6USKNN","created_at":"2026-07-16T01:23:21.134865+00:00"},{"alias_kind":"pith_short_16","alias_value":"GPT2MR6USKNN7Y7D","created_at":"2026-07-16T01:23:21.134865+00:00"},{"alias_kind":"pith_short_8","alias_value":"GPT2MR6U","created_at":"2026-07-16T01:23:21.134865+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GPT2MR6USKNN7Y7D7X4AHNXSN7","json":"https://pith.science/pith/GPT2MR6USKNN7Y7D7X4AHNXSN7.json","graph_json":"https://pith.science/api/pith-number/GPT2MR6USKNN7Y7D7X4AHNXSN7/graph.json","events_json":"https://pith.science/api/pith-number/GPT2MR6USKNN7Y7D7X4AHNXSN7/events.json","paper":"https://pith.science/paper/GPT2MR6U"},"agent_actions":{"view_html":"https://pith.science/pith/GPT2MR6USKNN7Y7D7X4AHNXSN7","download_json":"https://pith.science/pith/GPT2MR6USKNN7Y7D7X4AHNXSN7.json","view_paper":"https://pith.science/paper/GPT2MR6U","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2607.14042&json=true","fetch_graph":"https://pith.science/api/pith-number/GPT2MR6USKNN7Y7D7X4AHNXSN7/graph.json","fetch_events":"https://pith.science/api/pith-number/GPT2MR6USKNN7Y7D7X4AHNXSN7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GPT2MR6USKNN7Y7D7X4AHNXSN7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GPT2MR6USKNN7Y7D7X4AHNXSN7/action/storage_attestation","attest_author":"https://pith.science/pith/GPT2MR6USKNN7Y7D7X4AHNXSN7/action/author_attestation","sign_citation":"https://pith.science/pith/GPT2MR6USKNN7Y7D7X4AHNXSN7/action/citation_signature","submit_replication":"https://pith.science/pith/GPT2MR6USKNN7Y7D7X4AHNXSN7/action/replication_record"}},"created_at":"2026-07-16T01:23:21.134865+00:00","updated_at":"2026-07-16T01:23:21.134865+00:00"}