{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2006:SRPWPLXHXIEEMLTN4WKVDJS7HC","short_pith_number":"pith:SRPWPLXH","canonical_record":{"source":{"id":"physics/0609184","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"physics.data-an","submitted_at":"2006-09-21T13:47:41Z","cross_cats_sorted":["cond-mat.stat-mech","physics.bio-ph","q-bio.PE"],"title_canon_sha256":"16ac133abfc3da9b9962b8ce4144cae858e6887eca2ecd4ab85c052d53c109da","abstract_canon_sha256":"710d32aadbe6ae20d940c5431c0dc85bcc10a0dc4edf6d99bc749843ac95e5c3"},"schema_version":"1.0"},"canonical_sha256":"945f67aee7ba08462e6de59551a65f38a1457e1bcdb96ffa84ec589fb2f86d7a","source":{"kind":"arxiv","id":"physics/0609184","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"physics/0609184","created_at":"2026-05-18T01:38:06Z"},{"alias_kind":"arxiv_version","alias_value":"physics/0609184v2","created_at":"2026-05-18T01:38:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.physics/0609184","created_at":"2026-05-18T01:38:06Z"},{"alias_kind":"pith_short_12","alias_value":"SRPWPLXHXIEE","created_at":"2026-05-18T12:25:54Z"},{"alias_kind":"pith_short_16","alias_value":"SRPWPLXHXIEEMLTN","created_at":"2026-05-18T12:25:54Z"},{"alias_kind":"pith_short_8","alias_value":"SRPWPLXH","created_at":"2026-05-18T12:25:54Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2006:SRPWPLXHXIEEMLTN4WKVDJS7HC","target":"record","payload":{"canonical_record":{"source":{"id":"physics/0609184","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"physics.data-an","submitted_at":"2006-09-21T13:47:41Z","cross_cats_sorted":["cond-mat.stat-mech","physics.bio-ph","q-bio.PE"],"title_canon_sha256":"16ac133abfc3da9b9962b8ce4144cae858e6887eca2ecd4ab85c052d53c109da","abstract_canon_sha256":"710d32aadbe6ae20d940c5431c0dc85bcc10a0dc4edf6d99bc749843ac95e5c3"},"schema_version":"1.0"},"canonical_sha256":"945f67aee7ba08462e6de59551a65f38a1457e1bcdb96ffa84ec589fb2f86d7a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:38:06.595913Z","signature_b64":"9jkLXcX/2dEEKeTL26szJ+xoTmRQPXSJDVumpWzFDI7JAwxAFwvtHu8kSWPn1UrXZiDSQMfDZ3ZUS5GlKnlRDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"945f67aee7ba08462e6de59551a65f38a1457e1bcdb96ffa84ec589fb2f86d7a","last_reissued_at":"2026-05-18T01:38:06.595520Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:38:06.595520Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"physics/0609184","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":"2026-05-18T01:38:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bJMctp+dCN4kaae5Ry6zw6AmqXsWDDDj96kUTLErWAXhpI/2RUTFu7IBIePWUfFrjdamL1Ti+UtEngqV5NQjBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-20T05:26:22.724019Z"},"content_sha256":"ed9c8c77fc52f31a37f52f04b27bd12e7388e29c7bbfc6ab4fa1a76de2b0f011","schema_version":"1.0","event_id":"sha256:ed9c8c77fc52f31a37f52f04b27bd12e7388e29c7bbfc6ab4fa1a76de2b0f011"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2006:SRPWPLXHXIEEMLTN4WKVDJS7HC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Impact of non-Poisson activity patterns on spreading processes","license":"","headline":"","cross_cats":["cond-mat.stat-mech","physics.bio-ph","q-bio.PE"],"primary_cat":"physics.data-an","authors_text":"Albert-Laszlo Barabasi, Alexei Vazquez, Lukacs Andras, Racz Balazs","submitted_at":"2006-09-21T13:47:41Z","abstract_excerpt":"Halting a computer or biological virus outbreak requires a detailed understanding of the timing of the interactions between susceptible and infected individuals. While current spreading models assume that users interact uniformly in time, following a Poisson process, a series of recent measurements indicate that the inter-contact time distribution is heavy tailed, corresponding to a temporally inhomogeneous bursty contact process. Here we show that the non-Poisson nature of the contact dynamics results in prevalence decay times significantly larger than predicted by the standard Poisson proces"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"physics/0609184","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":"2026-05-18T01:38:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uBrJbxnkmMTJOV0POqvpCFURq6+Gt03ykwPNydcT1pPDVB68+NAPcZPswuNA9eutZOywaX7i82GYQSuKzV5lAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-20T05:26:22.724387Z"},"content_sha256":"4c1af0304957e9e2aed6a588278ab313bc9c74939d8daf99254b505b816b6fe7","schema_version":"1.0","event_id":"sha256:4c1af0304957e9e2aed6a588278ab313bc9c74939d8daf99254b505b816b6fe7"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SRPWPLXHXIEEMLTN4WKVDJS7HC/bundle.json","state_url":"https://pith.science/pith/SRPWPLXHXIEEMLTN4WKVDJS7HC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SRPWPLXHXIEEMLTN4WKVDJS7HC/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":"2026-06-20T05:26:22Z","links":{"resolver":"https://pith.science/pith/SRPWPLXHXIEEMLTN4WKVDJS7HC","bundle":"https://pith.science/pith/SRPWPLXHXIEEMLTN4WKVDJS7HC/bundle.json","state":"https://pith.science/pith/SRPWPLXHXIEEMLTN4WKVDJS7HC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SRPWPLXHXIEEMLTN4WKVDJS7HC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2006:SRPWPLXHXIEEMLTN4WKVDJS7HC","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":"710d32aadbe6ae20d940c5431c0dc85bcc10a0dc4edf6d99bc749843ac95e5c3","cross_cats_sorted":["cond-mat.stat-mech","physics.bio-ph","q-bio.PE"],"license":"","primary_cat":"physics.data-an","submitted_at":"2006-09-21T13:47:41Z","title_canon_sha256":"16ac133abfc3da9b9962b8ce4144cae858e6887eca2ecd4ab85c052d53c109da"},"schema_version":"1.0","source":{"id":"physics/0609184","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"physics/0609184","created_at":"2026-05-18T01:38:06Z"},{"alias_kind":"arxiv_version","alias_value":"physics/0609184v2","created_at":"2026-05-18T01:38:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.physics/0609184","created_at":"2026-05-18T01:38:06Z"},{"alias_kind":"pith_short_12","alias_value":"SRPWPLXHXIEE","created_at":"2026-05-18T12:25:54Z"},{"alias_kind":"pith_short_16","alias_value":"SRPWPLXHXIEEMLTN","created_at":"2026-05-18T12:25:54Z"},{"alias_kind":"pith_short_8","alias_value":"SRPWPLXH","created_at":"2026-05-18T12:25:54Z"}],"graph_snapshots":[{"event_id":"sha256:4c1af0304957e9e2aed6a588278ab313bc9c74939d8daf99254b505b816b6fe7","target":"graph","created_at":"2026-05-18T01:38:06Z","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":"Halting a computer or biological virus outbreak requires a detailed understanding of the timing of the interactions between susceptible and infected individuals. While current spreading models assume that users interact uniformly in time, following a Poisson process, a series of recent measurements indicate that the inter-contact time distribution is heavy tailed, corresponding to a temporally inhomogeneous bursty contact process. Here we show that the non-Poisson nature of the contact dynamics results in prevalence decay times significantly larger than predicted by the standard Poisson proces","authors_text":"Albert-Laszlo Barabasi, Alexei Vazquez, Lukacs Andras, Racz Balazs","cross_cats":["cond-mat.stat-mech","physics.bio-ph","q-bio.PE"],"headline":"","license":"","primary_cat":"physics.data-an","submitted_at":"2006-09-21T13:47:41Z","title":"Impact of non-Poisson activity patterns on spreading processes"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"physics/0609184","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:ed9c8c77fc52f31a37f52f04b27bd12e7388e29c7bbfc6ab4fa1a76de2b0f011","target":"record","created_at":"2026-05-18T01:38:06Z","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":"710d32aadbe6ae20d940c5431c0dc85bcc10a0dc4edf6d99bc749843ac95e5c3","cross_cats_sorted":["cond-mat.stat-mech","physics.bio-ph","q-bio.PE"],"license":"","primary_cat":"physics.data-an","submitted_at":"2006-09-21T13:47:41Z","title_canon_sha256":"16ac133abfc3da9b9962b8ce4144cae858e6887eca2ecd4ab85c052d53c109da"},"schema_version":"1.0","source":{"id":"physics/0609184","kind":"arxiv","version":2}},"canonical_sha256":"945f67aee7ba08462e6de59551a65f38a1457e1bcdb96ffa84ec589fb2f86d7a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"945f67aee7ba08462e6de59551a65f38a1457e1bcdb96ffa84ec589fb2f86d7a","first_computed_at":"2026-05-18T01:38:06.595520Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:38:06.595520Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"9jkLXcX/2dEEKeTL26szJ+xoTmRQPXSJDVumpWzFDI7JAwxAFwvtHu8kSWPn1UrXZiDSQMfDZ3ZUS5GlKnlRDw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:38:06.595913Z","signed_message":"canonical_sha256_bytes"},"source_id":"physics/0609184","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ed9c8c77fc52f31a37f52f04b27bd12e7388e29c7bbfc6ab4fa1a76de2b0f011","sha256:4c1af0304957e9e2aed6a588278ab313bc9c74939d8daf99254b505b816b6fe7"],"state_sha256":"a11f6af34903bc05c505d2a7e3c19871cec744136a2f10c5abb9f84ff50f126a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9o1oyYMQQ4GDDYVklun/u/H49yovyZTuc0bfY98KcKtAYlmRh6raOLBszgo7RpQ9nT5W/mYLLjqzjPUX12/PBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-20T05:26:22.726462Z","bundle_sha256":"1cbf0c8e9818a3465047ccbbcee169771ff26f8039600b2b61dce3291ea5e0be"}}