{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:GEFV5NRG5BDFUBN45AXAGMINRE","short_pith_number":"pith:GEFV5NRG","canonical_record":{"source":{"id":"1003.1383","kind":"arxiv","version":10},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-03-06T13:32:05Z","cross_cats_sorted":["physics.data-an"],"title_canon_sha256":"053d8cbb498168ab48c4b5fbad69c657200963504f042bbf3a2f92c4576c8e3a","abstract_canon_sha256":"1d9bb0e421d9e3bdc11f5a694d868331545123bcdf180f63af39c5a10df75238"},"schema_version":"1.0"},"canonical_sha256":"310b5eb626e8465a05bce82e03310d8911b7a0dc7a7c2ba19a4551498f399ad2","source":{"kind":"arxiv","id":"1003.1383","version":10},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1003.1383","created_at":"2026-05-18T02:08:45Z"},{"alias_kind":"arxiv_version","alias_value":"1003.1383v10","created_at":"2026-05-18T02:08:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.1383","created_at":"2026-05-18T02:08:45Z"},{"alias_kind":"pith_short_12","alias_value":"GEFV5NRG5BDF","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_16","alias_value":"GEFV5NRG5BDFUBN4","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_8","alias_value":"GEFV5NRG","created_at":"2026-05-18T12:26:07Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:GEFV5NRG5BDFUBN45AXAGMINRE","target":"record","payload":{"canonical_record":{"source":{"id":"1003.1383","kind":"arxiv","version":10},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-03-06T13:32:05Z","cross_cats_sorted":["physics.data-an"],"title_canon_sha256":"053d8cbb498168ab48c4b5fbad69c657200963504f042bbf3a2f92c4576c8e3a","abstract_canon_sha256":"1d9bb0e421d9e3bdc11f5a694d868331545123bcdf180f63af39c5a10df75238"},"schema_version":"1.0"},"canonical_sha256":"310b5eb626e8465a05bce82e03310d8911b7a0dc7a7c2ba19a4551498f399ad2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:08:45.427802Z","signature_b64":"uTbFhVVlvVopdk+pfyedCWEaJ8lABXd/nCpXAiP2e/DrVoqCnEhvsXm1nKRiZLOY+J+1yv7uMdzqWIuES8yNDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"310b5eb626e8465a05bce82e03310d8911b7a0dc7a7c2ba19a4551498f399ad2","last_reissued_at":"2026-05-18T02:08:45.426928Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:08:45.426928Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1003.1383","source_version":10,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:08:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"u4Sk7dNGhuAAoK297VtBeZmknNCjzs18OP0Dm0AONXWBo4AIQMMgP+z4Vn/UZOmKj+xar1k3fZBLiWhTuWGyBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T23:47:33.975742Z"},"content_sha256":"c6f7ad0b9fc7c79a7d7f2bd4007c02bbf9996b3315360bd6a210ee70b580e3a4","schema_version":"1.0","event_id":"sha256:c6f7ad0b9fc7c79a7d7f2bd4007c02bbf9996b3315360bd6a210ee70b580e3a4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:GEFV5NRG5BDFUBN45AXAGMINRE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Effect of significant data loss on identifying electric signals that precede rupture by detrended fluctuation analysis in natural time","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.data-an"],"primary_cat":"cond-mat.stat-mech","authors_text":"E.S. Skordas, N.V. Sarlis, P.A. Varotsos","submitted_at":"2010-03-06T13:32:05Z","abstract_excerpt":"Electric field variations that appear before rupture have been recently studied by employing the detrended fluctuation analysis (DFA) as a scaling method to quantify long-range temporal correlations. These studies revealed that seismic electric signals (SES) activities exhibit a scale invariant feature with an exponent $\\alpha_{DFA} \\approx 1$ over all scales investigated (around five orders of magnitude). Here, we study what happens upon significant data loss, which is a question of primary practical importance, and show that the DFA applied to the natural time representation of the remaining"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.1383","kind":"arxiv","version":10},"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":"2026-05-18T02:08:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"g30OP/+SV4Fi41mzGqbGDdu+hQbWdOmc05g/jJSPvA33dDElhdjkkOXK2qiduZFhDHPTgta1rk6UDmWxgEpRAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T23:47:33.976466Z"},"content_sha256":"28b5d16637f61d3cdbb15a846a52fd20e49c4fd3181b01d77e58885b81115aa4","schema_version":"1.0","event_id":"sha256:28b5d16637f61d3cdbb15a846a52fd20e49c4fd3181b01d77e58885b81115aa4"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GEFV5NRG5BDFUBN45AXAGMINRE/bundle.json","state_url":"https://pith.science/pith/GEFV5NRG5BDFUBN45AXAGMINRE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GEFV5NRG5BDFUBN45AXAGMINRE/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":"2026-06-09T23:47:33Z","links":{"resolver":"https://pith.science/pith/GEFV5NRG5BDFUBN45AXAGMINRE","bundle":"https://pith.science/pith/GEFV5NRG5BDFUBN45AXAGMINRE/bundle.json","state":"https://pith.science/pith/GEFV5NRG5BDFUBN45AXAGMINRE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GEFV5NRG5BDFUBN45AXAGMINRE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:GEFV5NRG5BDFUBN45AXAGMINRE","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":"1d9bb0e421d9e3bdc11f5a694d868331545123bcdf180f63af39c5a10df75238","cross_cats_sorted":["physics.data-an"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-03-06T13:32:05Z","title_canon_sha256":"053d8cbb498168ab48c4b5fbad69c657200963504f042bbf3a2f92c4576c8e3a"},"schema_version":"1.0","source":{"id":"1003.1383","kind":"arxiv","version":10}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1003.1383","created_at":"2026-05-18T02:08:45Z"},{"alias_kind":"arxiv_version","alias_value":"1003.1383v10","created_at":"2026-05-18T02:08:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.1383","created_at":"2026-05-18T02:08:45Z"},{"alias_kind":"pith_short_12","alias_value":"GEFV5NRG5BDF","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_16","alias_value":"GEFV5NRG5BDFUBN4","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_8","alias_value":"GEFV5NRG","created_at":"2026-05-18T12:26:07Z"}],"graph_snapshots":[{"event_id":"sha256:28b5d16637f61d3cdbb15a846a52fd20e49c4fd3181b01d77e58885b81115aa4","target":"graph","created_at":"2026-05-18T02:08:45Z","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":"Electric field variations that appear before rupture have been recently studied by employing the detrended fluctuation analysis (DFA) as a scaling method to quantify long-range temporal correlations. These studies revealed that seismic electric signals (SES) activities exhibit a scale invariant feature with an exponent $\\alpha_{DFA} \\approx 1$ over all scales investigated (around five orders of magnitude). Here, we study what happens upon significant data loss, which is a question of primary practical importance, and show that the DFA applied to the natural time representation of the remaining","authors_text":"E.S. Skordas, N.V. Sarlis, P.A. Varotsos","cross_cats":["physics.data-an"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-03-06T13:32:05Z","title":"Effect of significant data loss on identifying electric signals that precede rupture by detrended fluctuation analysis in natural time"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.1383","kind":"arxiv","version":10},"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:c6f7ad0b9fc7c79a7d7f2bd4007c02bbf9996b3315360bd6a210ee70b580e3a4","target":"record","created_at":"2026-05-18T02:08:45Z","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":"1d9bb0e421d9e3bdc11f5a694d868331545123bcdf180f63af39c5a10df75238","cross_cats_sorted":["physics.data-an"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2010-03-06T13:32:05Z","title_canon_sha256":"053d8cbb498168ab48c4b5fbad69c657200963504f042bbf3a2f92c4576c8e3a"},"schema_version":"1.0","source":{"id":"1003.1383","kind":"arxiv","version":10}},"canonical_sha256":"310b5eb626e8465a05bce82e03310d8911b7a0dc7a7c2ba19a4551498f399ad2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"310b5eb626e8465a05bce82e03310d8911b7a0dc7a7c2ba19a4551498f399ad2","first_computed_at":"2026-05-18T02:08:45.426928Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:08:45.426928Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"uTbFhVVlvVopdk+pfyedCWEaJ8lABXd/nCpXAiP2e/DrVoqCnEhvsXm1nKRiZLOY+J+1yv7uMdzqWIuES8yNDg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:08:45.427802Z","signed_message":"canonical_sha256_bytes"},"source_id":"1003.1383","source_kind":"arxiv","source_version":10}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c6f7ad0b9fc7c79a7d7f2bd4007c02bbf9996b3315360bd6a210ee70b580e3a4","sha256:28b5d16637f61d3cdbb15a846a52fd20e49c4fd3181b01d77e58885b81115aa4"],"state_sha256":"57fb63d4ee753691ad8b9c36c506dc5947677bd4912a34eecca4566d69773172"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mmC9xlVAkWeaEq0CMQIFpEfe1TXdEptuKJt387MRSSGYCrinpTVxyUhGGj/F1b6xczHOclHaEkvwKzJ0Pb+WBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T23:47:33.980065Z","bundle_sha256":"e2d3741cec36e0f53027a65fac176cc4d831ad546060dfcbe36e0d5837e624ec"}}