{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:IP6UOWN4IAGGGROWFOBINCCGK6","short_pith_number":"pith:IP6UOWN4","canonical_record":{"source":{"id":"1705.03026","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-05-08T18:07:22Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"3a540eb2e5395e13467d6ca656b6a7744612daaff0585157ff072d83107dc1aa","abstract_canon_sha256":"16caebb2c2f32a04165db6600e33f51fc1ed23593365b76fa23317d9e60c8e20"},"schema_version":"1.0"},"canonical_sha256":"43fd4759bc400c6345d62b828688465796c392fac433a57f5e9b9a94b78861fe","source":{"kind":"arxiv","id":"1705.03026","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.03026","created_at":"2026-05-18T00:35:20Z"},{"alias_kind":"arxiv_version","alias_value":"1705.03026v1","created_at":"2026-05-18T00:35:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.03026","created_at":"2026-05-18T00:35:20Z"},{"alias_kind":"pith_short_12","alias_value":"IP6UOWN4IAGG","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_16","alias_value":"IP6UOWN4IAGGGROW","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_8","alias_value":"IP6UOWN4","created_at":"2026-05-18T12:31:21Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:IP6UOWN4IAGGGROWFOBINCCGK6","target":"record","payload":{"canonical_record":{"source":{"id":"1705.03026","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-05-08T18:07:22Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"3a540eb2e5395e13467d6ca656b6a7744612daaff0585157ff072d83107dc1aa","abstract_canon_sha256":"16caebb2c2f32a04165db6600e33f51fc1ed23593365b76fa23317d9e60c8e20"},"schema_version":"1.0"},"canonical_sha256":"43fd4759bc400c6345d62b828688465796c392fac433a57f5e9b9a94b78861fe","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:35:20.684598Z","signature_b64":"ehutiqax6r4yZ0CEJEcxnwdiDxe1PUPR1YQzh09NvlEoOc17sYYhprqY+YXs53sd3CJ7YBq+1XMrIADZe/P1Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"43fd4759bc400c6345d62b828688465796c392fac433a57f5e9b9a94b78861fe","last_reissued_at":"2026-05-18T00:35:20.684124Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:35:20.684124Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1705.03026","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:35:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"w/70PcYbclfKySgtvI6JjU1HzG47ppo3qUsd50Ay0IuNDEdU8A4A8l3HSLYrutJFxZ/o2hR2tJ46m7UZ1ELHAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T17:20:48.939707Z"},"content_sha256":"9afd7c9ff6cec805e19eb660cc4e10b798504959358477249ae3f475215cdcf4","schema_version":"1.0","event_id":"sha256:9afd7c9ff6cec805e19eb660cc4e10b798504959358477249ae3f475215cdcf4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:IP6UOWN4IAGGGROWFOBINCCGK6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Nonlinear Gravity from Entanglement in Conformal Field Theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Charles Rabideau, Eliot Hijano, Felix M. Haehl, Mark Van Raamsdonk, Onkar Parrikar, Thomas Faulkner","submitted_at":"2017-05-08T18:07:22Z","abstract_excerpt":"In this paper, we demonstrate the emergence of nonlinear gravitational equations directly from the physics of a broad class of conformal field theories. We consider CFT excited states defined by adding sources for scalar primary or stress tensor operators to the Euclidean path integral defining the vacuum state. For these states, we show that up to second order in the sources, the entanglement entropy for all ball-shaped regions can always be represented geometrically (via the Ryu-Takayanagi formula) by an asymptotically AdS geometry. We show that such a geometry necessarily satisfies Einstein"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.03026","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":""},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:35:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kfCgztacUQYwcuN7Et+GDLR65yk0mpDWNmaHCxZbjZG3sXPR1Oy8OQoyKLFJxg6GcyhFJscEwh7CZOtw9UuRAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T17:20:48.940113Z"},"content_sha256":"401dbf8c6fae5db41eec2a7d2c441d597ead10ae8606ab212d14932256dcec7b","schema_version":"1.0","event_id":"sha256:401dbf8c6fae5db41eec2a7d2c441d597ead10ae8606ab212d14932256dcec7b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/IP6UOWN4IAGGGROWFOBINCCGK6/bundle.json","state_url":"https://pith.science/pith/IP6UOWN4IAGGGROWFOBINCCGK6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/IP6UOWN4IAGGGROWFOBINCCGK6/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-28T17:20:48Z","links":{"resolver":"https://pith.science/pith/IP6UOWN4IAGGGROWFOBINCCGK6","bundle":"https://pith.science/pith/IP6UOWN4IAGGGROWFOBINCCGK6/bundle.json","state":"https://pith.science/pith/IP6UOWN4IAGGGROWFOBINCCGK6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/IP6UOWN4IAGGGROWFOBINCCGK6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:IP6UOWN4IAGGGROWFOBINCCGK6","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"16caebb2c2f32a04165db6600e33f51fc1ed23593365b76fa23317d9e60c8e20","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-05-08T18:07:22Z","title_canon_sha256":"3a540eb2e5395e13467d6ca656b6a7744612daaff0585157ff072d83107dc1aa"},"schema_version":"1.0","source":{"id":"1705.03026","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.03026","created_at":"2026-05-18T00:35:20Z"},{"alias_kind":"arxiv_version","alias_value":"1705.03026v1","created_at":"2026-05-18T00:35:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.03026","created_at":"2026-05-18T00:35:20Z"},{"alias_kind":"pith_short_12","alias_value":"IP6UOWN4IAGG","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_16","alias_value":"IP6UOWN4IAGGGROW","created_at":"2026-05-18T12:31:21Z"},{"alias_kind":"pith_short_8","alias_value":"IP6UOWN4","created_at":"2026-05-18T12:31:21Z"}],"graph_snapshots":[{"event_id":"sha256:401dbf8c6fae5db41eec2a7d2c441d597ead10ae8606ab212d14932256dcec7b","target":"graph","created_at":"2026-05-18T00:35:20Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"In this paper, we demonstrate the emergence of nonlinear gravitational equations directly from the physics of a broad class of conformal field theories. We consider CFT excited states defined by adding sources for scalar primary or stress tensor operators to the Euclidean path integral defining the vacuum state. For these states, we show that up to second order in the sources, the entanglement entropy for all ball-shaped regions can always be represented geometrically (via the Ryu-Takayanagi formula) by an asymptotically AdS geometry. We show that such a geometry necessarily satisfies Einstein","authors_text":"Charles Rabideau, Eliot Hijano, Felix M. Haehl, Mark Van Raamsdonk, Onkar Parrikar, Thomas Faulkner","cross_cats":["gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-05-08T18:07:22Z","title":"Nonlinear Gravity from Entanglement in Conformal Field Theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.03026","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:9afd7c9ff6cec805e19eb660cc4e10b798504959358477249ae3f475215cdcf4","target":"record","created_at":"2026-05-18T00:35:20Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"16caebb2c2f32a04165db6600e33f51fc1ed23593365b76fa23317d9e60c8e20","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-05-08T18:07:22Z","title_canon_sha256":"3a540eb2e5395e13467d6ca656b6a7744612daaff0585157ff072d83107dc1aa"},"schema_version":"1.0","source":{"id":"1705.03026","kind":"arxiv","version":1}},"canonical_sha256":"43fd4759bc400c6345d62b828688465796c392fac433a57f5e9b9a94b78861fe","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"43fd4759bc400c6345d62b828688465796c392fac433a57f5e9b9a94b78861fe","first_computed_at":"2026-05-18T00:35:20.684124Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:35:20.684124Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ehutiqax6r4yZ0CEJEcxnwdiDxe1PUPR1YQzh09NvlEoOc17sYYhprqY+YXs53sd3CJ7YBq+1XMrIADZe/P1Aw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:35:20.684598Z","signed_message":"canonical_sha256_bytes"},"source_id":"1705.03026","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9afd7c9ff6cec805e19eb660cc4e10b798504959358477249ae3f475215cdcf4","sha256:401dbf8c6fae5db41eec2a7d2c441d597ead10ae8606ab212d14932256dcec7b"],"state_sha256":"e7df469edb2663812238e96206918a86b9cb19d3ea622258e3e5b5289d39c7a4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9pDQkXyA0f0FCyVPGrnfkN3RGWEewT6WMApPj1QDJKyBreM948eK1CcNih4pOL0jOmdJr+GIorpXCDvR7GGVCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T17:20:48.942955Z","bundle_sha256":"ddf71815bc0f8c4fd4b876604624b663741e888312f317a4fa4ebf7f25f9ae34"}}