{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:MEZY57KOZQDE4OA6W2VR5NXXQA","short_pith_number":"pith:MEZY57KO","canonical_record":{"source":{"id":"1811.09190","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-11-22T14:27:16Z","cross_cats_sorted":[],"title_canon_sha256":"42ccee9d03def08a675b13cf438b655f912e3cee25b101bc61fa8e76de949314","abstract_canon_sha256":"928ebe8158c80dd6b1998767a338deb7cf63c41f6c6353fd6cdae51565784c7c"},"schema_version":"1.0"},"canonical_sha256":"61338efd4ecc064e381eb6ab1eb6f78020fab6a90a54f2b07974c5bc5dc93919","source":{"kind":"arxiv","id":"1811.09190","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1811.09190","created_at":"2026-05-18T00:00:03Z"},{"alias_kind":"arxiv_version","alias_value":"1811.09190v1","created_at":"2026-05-18T00:00:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.09190","created_at":"2026-05-18T00:00:03Z"},{"alias_kind":"pith_short_12","alias_value":"MEZY57KOZQDE","created_at":"2026-05-18T12:32:37Z"},{"alias_kind":"pith_short_16","alias_value":"MEZY57KOZQDE4OA6","created_at":"2026-05-18T12:32:37Z"},{"alias_kind":"pith_short_8","alias_value":"MEZY57KO","created_at":"2026-05-18T12:32:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:MEZY57KOZQDE4OA6W2VR5NXXQA","target":"record","payload":{"canonical_record":{"source":{"id":"1811.09190","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-11-22T14:27:16Z","cross_cats_sorted":[],"title_canon_sha256":"42ccee9d03def08a675b13cf438b655f912e3cee25b101bc61fa8e76de949314","abstract_canon_sha256":"928ebe8158c80dd6b1998767a338deb7cf63c41f6c6353fd6cdae51565784c7c"},"schema_version":"1.0"},"canonical_sha256":"61338efd4ecc064e381eb6ab1eb6f78020fab6a90a54f2b07974c5bc5dc93919","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:00:03.980066Z","signature_b64":"PfnDuaAHJxSQDMCSO8OBMuWMlnwKk20cwfMlKssrZ5wuXPfNFVHLmmVIMkLVqGTp547cpyJhff6jRTyXuIYgCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"61338efd4ecc064e381eb6ab1eb6f78020fab6a90a54f2b07974c5bc5dc93919","last_reissued_at":"2026-05-18T00:00:03.979615Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:00:03.979615Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1811.09190","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":"2026-05-18T00:00:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BxwLB2ZhHugZoKmqppWgp9vBXqWjiIMPstSbuEk1xbgSr8PFTG4dOn/NxQ2MC3X+UD2smHG4YFfZ5zC0N9eLBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T05:46:06.796114Z"},"content_sha256":"bd627bc1e750318470a6b6aa1f558f43380681a02f307cbe0234249a41531fff","schema_version":"1.0","event_id":"sha256:bd627bc1e750318470a6b6aa1f558f43380681a02f307cbe0234249a41531fff"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:MEZY57KOZQDE4OA6W2VR5NXXQA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Amplitude of jump motion signatures in classical vibration-jump dynamic","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"John Ellis, Peter S.M. Townsend","submitted_at":"2018-11-22T14:27:16Z","abstract_excerpt":"The classical Langevin dynamics of a particle in a periodic potential energy landscape are studied via the intermediate scattering function (ISF). By construction, the particle performs coupled vibrational and activated jump motion with a wide separation of the vibrational period and the mean residence time between jumps. The long time limit of the ISF is a decaying tail proportional to the function that describes ideal jump motion in the absence of vibrations. The amplitude of the tail is unity in idealized jump dynamics models, but is reduced from unity by the intra-well motion. Analytical e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.09190","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":"2026-05-18T00:00:03Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VWZvwYpYuJWubqV4BCun8Mb3Xm8WNJ0FmmLfNO5VOrtlXsZf86ICd6iXAGyQVZFFhBSBZGu1ZJPOrRNfkduBCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T05:46:06.796468Z"},"content_sha256":"119a257b1ea10a8faefeb5eaf22f8465073e04a17eb40f9f71325aa81bc04dfa","schema_version":"1.0","event_id":"sha256:119a257b1ea10a8faefeb5eaf22f8465073e04a17eb40f9f71325aa81bc04dfa"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MEZY57KOZQDE4OA6W2VR5NXXQA/bundle.json","state_url":"https://pith.science/pith/MEZY57KOZQDE4OA6W2VR5NXXQA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MEZY57KOZQDE4OA6W2VR5NXXQA/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":"2026-06-03T05:46:06Z","links":{"resolver":"https://pith.science/pith/MEZY57KOZQDE4OA6W2VR5NXXQA","bundle":"https://pith.science/pith/MEZY57KOZQDE4OA6W2VR5NXXQA/bundle.json","state":"https://pith.science/pith/MEZY57KOZQDE4OA6W2VR5NXXQA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MEZY57KOZQDE4OA6W2VR5NXXQA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:MEZY57KOZQDE4OA6W2VR5NXXQA","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":"928ebe8158c80dd6b1998767a338deb7cf63c41f6c6353fd6cdae51565784c7c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-11-22T14:27:16Z","title_canon_sha256":"42ccee9d03def08a675b13cf438b655f912e3cee25b101bc61fa8e76de949314"},"schema_version":"1.0","source":{"id":"1811.09190","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1811.09190","created_at":"2026-05-18T00:00:03Z"},{"alias_kind":"arxiv_version","alias_value":"1811.09190v1","created_at":"2026-05-18T00:00:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.09190","created_at":"2026-05-18T00:00:03Z"},{"alias_kind":"pith_short_12","alias_value":"MEZY57KOZQDE","created_at":"2026-05-18T12:32:37Z"},{"alias_kind":"pith_short_16","alias_value":"MEZY57KOZQDE4OA6","created_at":"2026-05-18T12:32:37Z"},{"alias_kind":"pith_short_8","alias_value":"MEZY57KO","created_at":"2026-05-18T12:32:37Z"}],"graph_snapshots":[{"event_id":"sha256:119a257b1ea10a8faefeb5eaf22f8465073e04a17eb40f9f71325aa81bc04dfa","target":"graph","created_at":"2026-05-18T00:00:03Z","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":"The classical Langevin dynamics of a particle in a periodic potential energy landscape are studied via the intermediate scattering function (ISF). By construction, the particle performs coupled vibrational and activated jump motion with a wide separation of the vibrational period and the mean residence time between jumps. The long time limit of the ISF is a decaying tail proportional to the function that describes ideal jump motion in the absence of vibrations. The amplitude of the tail is unity in idealized jump dynamics models, but is reduced from unity by the intra-well motion. Analytical e","authors_text":"John Ellis, Peter S.M. Townsend","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-11-22T14:27:16Z","title":"Amplitude of jump motion signatures in classical vibration-jump dynamic"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.09190","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:bd627bc1e750318470a6b6aa1f558f43380681a02f307cbe0234249a41531fff","target":"record","created_at":"2026-05-18T00:00:03Z","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":"928ebe8158c80dd6b1998767a338deb7cf63c41f6c6353fd6cdae51565784c7c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-11-22T14:27:16Z","title_canon_sha256":"42ccee9d03def08a675b13cf438b655f912e3cee25b101bc61fa8e76de949314"},"schema_version":"1.0","source":{"id":"1811.09190","kind":"arxiv","version":1}},"canonical_sha256":"61338efd4ecc064e381eb6ab1eb6f78020fab6a90a54f2b07974c5bc5dc93919","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"61338efd4ecc064e381eb6ab1eb6f78020fab6a90a54f2b07974c5bc5dc93919","first_computed_at":"2026-05-18T00:00:03.979615Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:00:03.979615Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PfnDuaAHJxSQDMCSO8OBMuWMlnwKk20cwfMlKssrZ5wuXPfNFVHLmmVIMkLVqGTp547cpyJhff6jRTyXuIYgCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:00:03.980066Z","signed_message":"canonical_sha256_bytes"},"source_id":"1811.09190","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bd627bc1e750318470a6b6aa1f558f43380681a02f307cbe0234249a41531fff","sha256:119a257b1ea10a8faefeb5eaf22f8465073e04a17eb40f9f71325aa81bc04dfa"],"state_sha256":"2763cfeab4bed176dd9ebf8e7d900acd346b272d537d121b03bca71758caa2e9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xhbFXd+/rgBVGJ7sGCE789n5rPbu6BU7afkst/noarRmismkn0ZvIzwtsT1wSkO3BgUFUJCe7qDHJ7yfhrx0Dg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T05:46:06.798574Z","bundle_sha256":"37804404b3d68f0b7a1e64a82be5f14f360d6206173ad16672b0c186d787936b"}}