{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:L36XZOGWFPMEI5MZF5YY7BHSEJ","short_pith_number":"pith:L36XZOGW","canonical_record":{"source":{"id":"1705.01834","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-05-04T13:37:44Z","cross_cats_sorted":["cond-mat.stat-mech","gr-qc","quant-ph"],"title_canon_sha256":"a8b1c62acef9b6b5820d9f485ae93fc7b5a6763daaf3ee612ce48ed0c19ffecc","abstract_canon_sha256":"231a4fe6f675108ac68bcf45839e133294ce16040fe8d4e392672308f223cf4b"},"schema_version":"1.0"},"canonical_sha256":"5efd7cb8d62bd84475992f718f84f2225c268d3e98c115f5db9c125c91b29782","source":{"kind":"arxiv","id":"1705.01834","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.01834","created_at":"2026-05-18T00:32:43Z"},{"alias_kind":"arxiv_version","alias_value":"1705.01834v1","created_at":"2026-05-18T00:32:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.01834","created_at":"2026-05-18T00:32:43Z"},{"alias_kind":"pith_short_12","alias_value":"L36XZOGWFPME","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_16","alias_value":"L36XZOGWFPMEI5MZ","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_8","alias_value":"L36XZOGW","created_at":"2026-05-18T12:31:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:L36XZOGWFPMEI5MZF5YY7BHSEJ","target":"record","payload":{"canonical_record":{"source":{"id":"1705.01834","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-05-04T13:37:44Z","cross_cats_sorted":["cond-mat.stat-mech","gr-qc","quant-ph"],"title_canon_sha256":"a8b1c62acef9b6b5820d9f485ae93fc7b5a6763daaf3ee612ce48ed0c19ffecc","abstract_canon_sha256":"231a4fe6f675108ac68bcf45839e133294ce16040fe8d4e392672308f223cf4b"},"schema_version":"1.0"},"canonical_sha256":"5efd7cb8d62bd84475992f718f84f2225c268d3e98c115f5db9c125c91b29782","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:32:43.258804Z","signature_b64":"ERL0J7ZAv2RCTHM3RNS9rmROqoqg/c22ZPEWvkljkVk2YMPT2rgn5RuzoW7oivw0iLKOTF01iMqhkzChoNzBBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5efd7cb8d62bd84475992f718f84f2225c268d3e98c115f5db9c125c91b29782","last_reissued_at":"2026-05-18T00:32:43.258149Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:32:43.258149Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1705.01834","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":"2026-05-18T00:32:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bQ9SGvONAqqRhuUtEaCZirP5YJgcQpworTfKJI1D5fDxmZPV7RY03dpZPkaAbnoj6UL3soz3pajGJpDlIP4QBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-29T10:44:45.544518Z"},"content_sha256":"782102af6a35fcbbf292c2ef53b48d02452d2e0eb4458ed26bb4d7f4cec18c1f","schema_version":"1.0","event_id":"sha256:782102af6a35fcbbf292c2ef53b48d02452d2e0eb4458ed26bb4d7f4cec18c1f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:L36XZOGWFPMEI5MZF5YY7BHSEJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Holographic Fidelity Susceptibility","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","gr-qc","quant-ph"],"primary_cat":"hep-th","authors_text":"Amin Faraji Astaneh, Mohsen Alishahiha","submitted_at":"2017-05-04T13:37:44Z","abstract_excerpt":"For a field theory with a gravitational dual, we study holographic fidelity susceptibility for two states related by a deformation of a relevant operator. To do so, we study back reaction of a massive scalar field on the asymptotic behavior of the metric in an Einstein gravity coupled to a massive scalar field. Identifying the two states, holographically, with the original and back reacted geometries, the corresponding holographic fidelity susceptibility is given by the difference of the volume of an extremal time slice evaluated on the original and back reacted geometries."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.01834","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":"2026-05-18T00:32:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WyJHawKednMRi1oBabR7NTbdsYOtVp66Qn3PiwIEyXnLTI7nnsZw1C1/f00O8ytmx83MeEbMbggcK52YOPIPCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-29T10:44:45.544873Z"},"content_sha256":"4b586a7331eb81c7d281ba7f585cfa3645c228c06102aa87ced3c6a10346d856","schema_version":"1.0","event_id":"sha256:4b586a7331eb81c7d281ba7f585cfa3645c228c06102aa87ced3c6a10346d856"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/L36XZOGWFPMEI5MZF5YY7BHSEJ/bundle.json","state_url":"https://pith.science/pith/L36XZOGWFPMEI5MZF5YY7BHSEJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/L36XZOGWFPMEI5MZF5YY7BHSEJ/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":"2026-06-29T10:44:45Z","links":{"resolver":"https://pith.science/pith/L36XZOGWFPMEI5MZF5YY7BHSEJ","bundle":"https://pith.science/pith/L36XZOGWFPMEI5MZF5YY7BHSEJ/bundle.json","state":"https://pith.science/pith/L36XZOGWFPMEI5MZF5YY7BHSEJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/L36XZOGWFPMEI5MZF5YY7BHSEJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:L36XZOGWFPMEI5MZF5YY7BHSEJ","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":"231a4fe6f675108ac68bcf45839e133294ce16040fe8d4e392672308f223cf4b","cross_cats_sorted":["cond-mat.stat-mech","gr-qc","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-05-04T13:37:44Z","title_canon_sha256":"a8b1c62acef9b6b5820d9f485ae93fc7b5a6763daaf3ee612ce48ed0c19ffecc"},"schema_version":"1.0","source":{"id":"1705.01834","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.01834","created_at":"2026-05-18T00:32:43Z"},{"alias_kind":"arxiv_version","alias_value":"1705.01834v1","created_at":"2026-05-18T00:32:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.01834","created_at":"2026-05-18T00:32:43Z"},{"alias_kind":"pith_short_12","alias_value":"L36XZOGWFPME","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_16","alias_value":"L36XZOGWFPMEI5MZ","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_8","alias_value":"L36XZOGW","created_at":"2026-05-18T12:31:28Z"}],"graph_snapshots":[{"event_id":"sha256:4b586a7331eb81c7d281ba7f585cfa3645c228c06102aa87ced3c6a10346d856","target":"graph","created_at":"2026-05-18T00:32:43Z","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":"For a field theory with a gravitational dual, we study holographic fidelity susceptibility for two states related by a deformation of a relevant operator. To do so, we study back reaction of a massive scalar field on the asymptotic behavior of the metric in an Einstein gravity coupled to a massive scalar field. Identifying the two states, holographically, with the original and back reacted geometries, the corresponding holographic fidelity susceptibility is given by the difference of the volume of an extremal time slice evaluated on the original and back reacted geometries.","authors_text":"Amin Faraji Astaneh, Mohsen Alishahiha","cross_cats":["cond-mat.stat-mech","gr-qc","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-05-04T13:37:44Z","title":"Holographic Fidelity Susceptibility"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.01834","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":"sha256:782102af6a35fcbbf292c2ef53b48d02452d2e0eb4458ed26bb4d7f4cec18c1f","target":"record","created_at":"2026-05-18T00:32:43Z","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":"231a4fe6f675108ac68bcf45839e133294ce16040fe8d4e392672308f223cf4b","cross_cats_sorted":["cond-mat.stat-mech","gr-qc","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-05-04T13:37:44Z","title_canon_sha256":"a8b1c62acef9b6b5820d9f485ae93fc7b5a6763daaf3ee612ce48ed0c19ffecc"},"schema_version":"1.0","source":{"id":"1705.01834","kind":"arxiv","version":1}},"canonical_sha256":"5efd7cb8d62bd84475992f718f84f2225c268d3e98c115f5db9c125c91b29782","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5efd7cb8d62bd84475992f718f84f2225c268d3e98c115f5db9c125c91b29782","first_computed_at":"2026-05-18T00:32:43.258149Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:32:43.258149Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ERL0J7ZAv2RCTHM3RNS9rmROqoqg/c22ZPEWvkljkVk2YMPT2rgn5RuzoW7oivw0iLKOTF01iMqhkzChoNzBBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:32:43.258804Z","signed_message":"canonical_sha256_bytes"},"source_id":"1705.01834","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:782102af6a35fcbbf292c2ef53b48d02452d2e0eb4458ed26bb4d7f4cec18c1f","sha256:4b586a7331eb81c7d281ba7f585cfa3645c228c06102aa87ced3c6a10346d856"],"state_sha256":"9988741b7d0040ac2874a3ad551ffcbaa1e83d5ea9a4fe6f4ab942d42703607c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"chPQqThMQjN/ydJ+nqTwWrbltr6RRtC+A/q98IGjeXn0Qdj159SpuodnGzHfoe9cL+bml+onmtGdFHDPcMYMDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-29T10:44:45.546899Z","bundle_sha256":"b95a43fc27086da1a232e39bae5486e5935b950269cd5e8bf2d01d10c28d599d"}}