{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:3T3TC6NEQVO6OXYGY22DIYRNCF","short_pith_number":"pith:3T3TC6NE","canonical_record":{"source":{"id":"1211.1175","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.soc-ph","submitted_at":"2012-11-06T10:57:29Z","cross_cats_sorted":["physics.data-an"],"title_canon_sha256":"47cb87008953e98c096b9e3d243b8e2089418927079d048e6c3d54bd3b886ebb","abstract_canon_sha256":"43196816c384bfff98955fab211d468bff15f517d3fc40ad4b45adb449f838ee"},"schema_version":"1.0"},"canonical_sha256":"dcf73179a4855de75f06c6b434622d1140d8e41467586e2ef5bb53d3c4bba8ac","source":{"kind":"arxiv","id":"1211.1175","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1211.1175","created_at":"2026-05-18T03:09:59Z"},{"alias_kind":"arxiv_version","alias_value":"1211.1175v2","created_at":"2026-05-18T03:09:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.1175","created_at":"2026-05-18T03:09:59Z"},{"alias_kind":"pith_short_12","alias_value":"3T3TC6NEQVO6","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_16","alias_value":"3T3TC6NEQVO6OXYG","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_8","alias_value":"3T3TC6NE","created_at":"2026-05-18T12:26:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:3T3TC6NEQVO6OXYGY22DIYRNCF","target":"record","payload":{"canonical_record":{"source":{"id":"1211.1175","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.soc-ph","submitted_at":"2012-11-06T10:57:29Z","cross_cats_sorted":["physics.data-an"],"title_canon_sha256":"47cb87008953e98c096b9e3d243b8e2089418927079d048e6c3d54bd3b886ebb","abstract_canon_sha256":"43196816c384bfff98955fab211d468bff15f517d3fc40ad4b45adb449f838ee"},"schema_version":"1.0"},"canonical_sha256":"dcf73179a4855de75f06c6b434622d1140d8e41467586e2ef5bb53d3c4bba8ac","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:09:59.755057Z","signature_b64":"Px2IajN/aNgpVjbZKzh/CH9UVZqy5hiI0Zt9JydrqVoX04uTRTc4VhfwD7BpR0J8mQWQkhl1qnGKBHiCAVU8Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dcf73179a4855de75f06c6b434622d1140d8e41467586e2ef5bb53d3c4bba8ac","last_reissued_at":"2026-05-18T03:09:59.754413Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:09:59.754413Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1211.1175","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:09:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3fTma8nYBLFCP/18VyDl+iVbLD5jpQZs5ZpSnCYlXF/UFj/IJUnmyl79Y1F1VpQkRtBfH76tQPOmeg4e0AvjCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-22T19:33:55.508064Z"},"content_sha256":"c8d35a780b7bd97bef7eb0d63244b54d63fff434c6775498c3ee085d787c6658","schema_version":"1.0","event_id":"sha256:c8d35a780b7bd97bef7eb0d63244b54d63fff434c6775498c3ee085d787c6658"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:3T3TC6NEQVO6OXYGY22DIYRNCF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Modelling bursty time series","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.data-an"],"primary_cat":"physics.soc-ph","authors_text":"B\\'alint T\\'oth, J\\'anos Kert\\'esz, Szabolcs Vajna","submitted_at":"2012-11-06T10:57:29Z","abstract_excerpt":"Many human-related activities show power-law decaying interevent time distribution with exponents usually varying between 1 and 2. We study a simple task-queuing model, which produces bursty time series due to the nontrivial dynamics of the task list. The model is characterised by a priority distribution as an input parameter, which describes the choice procedure from the list. We give exact results on the asymptotic behaviour of the model and we show that the interevent time distribution is power-law decaying for any kind of input distributions that remain normalizable in the infinite list li"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.1175","kind":"arxiv","version":2},"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":"2026-05-18T03:09:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WcJAIzslUsQyFVIjYzkJZ1GBeQNOqfCSo5uIqtudkKSZGmRxUxZKyTUsXQtztRSLiFO1OWVcN7J3BHBDWC3/AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-22T19:33:55.508425Z"},"content_sha256":"afa5bd52f618e0d531385556c22ac547307442eb1f2d9c74770e6d66da5f2d78","schema_version":"1.0","event_id":"sha256:afa5bd52f618e0d531385556c22ac547307442eb1f2d9c74770e6d66da5f2d78"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3T3TC6NEQVO6OXYGY22DIYRNCF/bundle.json","state_url":"https://pith.science/pith/3T3TC6NEQVO6OXYGY22DIYRNCF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3T3TC6NEQVO6OXYGY22DIYRNCF/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":"2026-05-22T19:33:55Z","links":{"resolver":"https://pith.science/pith/3T3TC6NEQVO6OXYGY22DIYRNCF","bundle":"https://pith.science/pith/3T3TC6NEQVO6OXYGY22DIYRNCF/bundle.json","state":"https://pith.science/pith/3T3TC6NEQVO6OXYGY22DIYRNCF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3T3TC6NEQVO6OXYGY22DIYRNCF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:3T3TC6NEQVO6OXYGY22DIYRNCF","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":"43196816c384bfff98955fab211d468bff15f517d3fc40ad4b45adb449f838ee","cross_cats_sorted":["physics.data-an"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.soc-ph","submitted_at":"2012-11-06T10:57:29Z","title_canon_sha256":"47cb87008953e98c096b9e3d243b8e2089418927079d048e6c3d54bd3b886ebb"},"schema_version":"1.0","source":{"id":"1211.1175","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1211.1175","created_at":"2026-05-18T03:09:59Z"},{"alias_kind":"arxiv_version","alias_value":"1211.1175v2","created_at":"2026-05-18T03:09:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.1175","created_at":"2026-05-18T03:09:59Z"},{"alias_kind":"pith_short_12","alias_value":"3T3TC6NEQVO6","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_16","alias_value":"3T3TC6NEQVO6OXYG","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_8","alias_value":"3T3TC6NE","created_at":"2026-05-18T12:26:53Z"}],"graph_snapshots":[{"event_id":"sha256:afa5bd52f618e0d531385556c22ac547307442eb1f2d9c74770e6d66da5f2d78","target":"graph","created_at":"2026-05-18T03:09:59Z","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":"Many human-related activities show power-law decaying interevent time distribution with exponents usually varying between 1 and 2. We study a simple task-queuing model, which produces bursty time series due to the nontrivial dynamics of the task list. The model is characterised by a priority distribution as an input parameter, which describes the choice procedure from the list. We give exact results on the asymptotic behaviour of the model and we show that the interevent time distribution is power-law decaying for any kind of input distributions that remain normalizable in the infinite list li","authors_text":"B\\'alint T\\'oth, J\\'anos Kert\\'esz, Szabolcs Vajna","cross_cats":["physics.data-an"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.soc-ph","submitted_at":"2012-11-06T10:57:29Z","title":"Modelling bursty time series"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.1175","kind":"arxiv","version":2},"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:c8d35a780b7bd97bef7eb0d63244b54d63fff434c6775498c3ee085d787c6658","target":"record","created_at":"2026-05-18T03:09:59Z","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":"43196816c384bfff98955fab211d468bff15f517d3fc40ad4b45adb449f838ee","cross_cats_sorted":["physics.data-an"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.soc-ph","submitted_at":"2012-11-06T10:57:29Z","title_canon_sha256":"47cb87008953e98c096b9e3d243b8e2089418927079d048e6c3d54bd3b886ebb"},"schema_version":"1.0","source":{"id":"1211.1175","kind":"arxiv","version":2}},"canonical_sha256":"dcf73179a4855de75f06c6b434622d1140d8e41467586e2ef5bb53d3c4bba8ac","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"dcf73179a4855de75f06c6b434622d1140d8e41467586e2ef5bb53d3c4bba8ac","first_computed_at":"2026-05-18T03:09:59.754413Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:09:59.754413Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Px2IajN/aNgpVjbZKzh/CH9UVZqy5hiI0Zt9JydrqVoX04uTRTc4VhfwD7BpR0J8mQWQkhl1qnGKBHiCAVU8Ag==","signature_status":"signed_v1","signed_at":"2026-05-18T03:09:59.755057Z","signed_message":"canonical_sha256_bytes"},"source_id":"1211.1175","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c8d35a780b7bd97bef7eb0d63244b54d63fff434c6775498c3ee085d787c6658","sha256:afa5bd52f618e0d531385556c22ac547307442eb1f2d9c74770e6d66da5f2d78"],"state_sha256":"98095895317668db29cc079f17c622ef2db0a596fae9e7d9e553cf45bd87d336"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UqZm4+BM4aXsNhrzoXwLP0Vyw4Os2cZNaUwqEbf8aLao8CWJJVt1cpOa0JK1mrRuds0yWFZqB9drqpJO+3fpDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-22T19:33:55.510541Z","bundle_sha256":"9ce7070fa13d7c8e5892526a25cff86777db56135eb3784b886feb8d198cfb74"}}