{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:DCSPKKPFOWLW3GET3TSCFUYCNC","short_pith_number":"pith:DCSPKKPF","canonical_record":{"source":{"id":"1412.5123","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-16T18:56:36Z","cross_cats_sorted":[],"title_canon_sha256":"6c2b378a522f09448a1748c99b023e5d88b38036be75edaeed610583c562d278","abstract_canon_sha256":"f59d84009ab18a3ba2df5f55bfb0a84fe345dc2cbdef2dae422c730d9b1c9877"},"schema_version":"1.0"},"canonical_sha256":"18a4f529e575976d9893dce422d30268ad21b4a08bcedd12792658de3c778497","source":{"kind":"arxiv","id":"1412.5123","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.5123","created_at":"2026-05-18T01:11:27Z"},{"alias_kind":"arxiv_version","alias_value":"1412.5123v3","created_at":"2026-05-18T01:11:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.5123","created_at":"2026-05-18T01:11:27Z"},{"alias_kind":"pith_short_12","alias_value":"DCSPKKPFOWLW","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_16","alias_value":"DCSPKKPFOWLW3GET","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_8","alias_value":"DCSPKKPF","created_at":"2026-05-18T12:28:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:DCSPKKPFOWLW3GET3TSCFUYCNC","target":"record","payload":{"canonical_record":{"source":{"id":"1412.5123","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-16T18:56:36Z","cross_cats_sorted":[],"title_canon_sha256":"6c2b378a522f09448a1748c99b023e5d88b38036be75edaeed610583c562d278","abstract_canon_sha256":"f59d84009ab18a3ba2df5f55bfb0a84fe345dc2cbdef2dae422c730d9b1c9877"},"schema_version":"1.0"},"canonical_sha256":"18a4f529e575976d9893dce422d30268ad21b4a08bcedd12792658de3c778497","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:11:27.532777Z","signature_b64":"TfYYFGXneTzs1ULBz37h+R0RNVR72RD+tLm8lIQnT9h0mWhX0tDGC2enmBGExDKOSka2vsTWJl6+65X2JJ6sAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"18a4f529e575976d9893dce422d30268ad21b4a08bcedd12792658de3c778497","last_reissued_at":"2026-05-18T01:11:27.532216Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:11:27.532216Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1412.5123","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:11:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hWQQve+0D3v3QVhpxUAO3EdEf3aj0Lsf98QB38DhlkiMljSFkzfyi0TWfrpGlsJCkaxwkcMNffiASLUBHGsbAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T23:31:13.013186Z"},"content_sha256":"8263cdbd0bc96d3a69fc8ced08c0e3e6b31ef46df4841d79b4c2a64ae5d042c9","schema_version":"1.0","event_id":"sha256:8263cdbd0bc96d3a69fc8ced08c0e3e6b31ef46df4841d79b4c2a64ae5d042c9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:DCSPKKPFOWLW3GET3TSCFUYCNC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Two-dimensional conformal field theory and the butterfly effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Daniel A. Roberts, Douglas Stanford","submitted_at":"2014-12-16T18:56:36Z","abstract_excerpt":"We study chaotic dynamics in two-dimensional conformal field theory through out-of-time order thermal correlators of the form $\\langle W(t)VW(t)V\\rangle$. We reproduce bulk calculations similar to those of [1], by studying the large $c$ Virasoro identity block. The contribution of this block to the above correlation function begins to decrease exponentially after a delay of $\\sim t_* - \\frac{\\beta}{2\\pi}\\log \\beta^2E_w E_v$, where $t_*$ is the scrambling time $\\frac{\\beta}{2\\pi}\\log c$, and $E_w,E_v$ are the energy scales of the $W,V$ operators."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.5123","kind":"arxiv","version":3},"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":"2026-05-18T01:11:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zXtL78j6EwD5CjGzdFhVnlf5zuXN/XZ+PEkwfGLGpHt5DhFM9Ze3RdhDTEdSKwevOsocDOPS5N4KwumK1gpjAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T23:31:13.013857Z"},"content_sha256":"c473b2a93f17ca870de1f362677bd2e39edd33b6c8c0d705ddf54df2405a831f","schema_version":"1.0","event_id":"sha256:c473b2a93f17ca870de1f362677bd2e39edd33b6c8c0d705ddf54df2405a831f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DCSPKKPFOWLW3GET3TSCFUYCNC/bundle.json","state_url":"https://pith.science/pith/DCSPKKPFOWLW3GET3TSCFUYCNC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DCSPKKPFOWLW3GET3TSCFUYCNC/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":"2026-05-25T23:31:13Z","links":{"resolver":"https://pith.science/pith/DCSPKKPFOWLW3GET3TSCFUYCNC","bundle":"https://pith.science/pith/DCSPKKPFOWLW3GET3TSCFUYCNC/bundle.json","state":"https://pith.science/pith/DCSPKKPFOWLW3GET3TSCFUYCNC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DCSPKKPFOWLW3GET3TSCFUYCNC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:DCSPKKPFOWLW3GET3TSCFUYCNC","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":"f59d84009ab18a3ba2df5f55bfb0a84fe345dc2cbdef2dae422c730d9b1c9877","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-16T18:56:36Z","title_canon_sha256":"6c2b378a522f09448a1748c99b023e5d88b38036be75edaeed610583c562d278"},"schema_version":"1.0","source":{"id":"1412.5123","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.5123","created_at":"2026-05-18T01:11:27Z"},{"alias_kind":"arxiv_version","alias_value":"1412.5123v3","created_at":"2026-05-18T01:11:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.5123","created_at":"2026-05-18T01:11:27Z"},{"alias_kind":"pith_short_12","alias_value":"DCSPKKPFOWLW","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_16","alias_value":"DCSPKKPFOWLW3GET","created_at":"2026-05-18T12:28:25Z"},{"alias_kind":"pith_short_8","alias_value":"DCSPKKPF","created_at":"2026-05-18T12:28:25Z"}],"graph_snapshots":[{"event_id":"sha256:c473b2a93f17ca870de1f362677bd2e39edd33b6c8c0d705ddf54df2405a831f","target":"graph","created_at":"2026-05-18T01:11:27Z","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":"We study chaotic dynamics in two-dimensional conformal field theory through out-of-time order thermal correlators of the form $\\langle W(t)VW(t)V\\rangle$. We reproduce bulk calculations similar to those of [1], by studying the large $c$ Virasoro identity block. The contribution of this block to the above correlation function begins to decrease exponentially after a delay of $\\sim t_* - \\frac{\\beta}{2\\pi}\\log \\beta^2E_w E_v$, where $t_*$ is the scrambling time $\\frac{\\beta}{2\\pi}\\log c$, and $E_w,E_v$ are the energy scales of the $W,V$ operators.","authors_text":"Daniel A. Roberts, Douglas Stanford","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-16T18:56:36Z","title":"Two-dimensional conformal field theory and the butterfly effect"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.5123","kind":"arxiv","version":3},"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":"sha256:8263cdbd0bc96d3a69fc8ced08c0e3e6b31ef46df4841d79b4c2a64ae5d042c9","target":"record","created_at":"2026-05-18T01:11:27Z","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":"f59d84009ab18a3ba2df5f55bfb0a84fe345dc2cbdef2dae422c730d9b1c9877","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-16T18:56:36Z","title_canon_sha256":"6c2b378a522f09448a1748c99b023e5d88b38036be75edaeed610583c562d278"},"schema_version":"1.0","source":{"id":"1412.5123","kind":"arxiv","version":3}},"canonical_sha256":"18a4f529e575976d9893dce422d30268ad21b4a08bcedd12792658de3c778497","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"18a4f529e575976d9893dce422d30268ad21b4a08bcedd12792658de3c778497","first_computed_at":"2026-05-18T01:11:27.532216Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:11:27.532216Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"TfYYFGXneTzs1ULBz37h+R0RNVR72RD+tLm8lIQnT9h0mWhX0tDGC2enmBGExDKOSka2vsTWJl6+65X2JJ6sAw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:11:27.532777Z","signed_message":"canonical_sha256_bytes"},"source_id":"1412.5123","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8263cdbd0bc96d3a69fc8ced08c0e3e6b31ef46df4841d79b4c2a64ae5d042c9","sha256:c473b2a93f17ca870de1f362677bd2e39edd33b6c8c0d705ddf54df2405a831f"],"state_sha256":"4259a777a4020fde18496c8938f94a525d71f6d8f5a8c54c67073252dd6055f5"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nMQxStFrVlejZLWmQEOBzSFmRxV2m5ZmnvCK/B+gPhKVXynGROeXprCB+RI78ZuRsktl5Bfe8UVxp6oKsgMpCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T23:31:13.017895Z","bundle_sha256":"8a70d29e313ecf96e4200837d097019b73a659ceb75ceadae76e6328f1fda190"}}