{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:PH6PM5XFNKF3BHXJLLTEV3WZFE","short_pith_number":"pith:PH6PM5XF","canonical_record":{"source":{"id":"1203.3296","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-03-15T09:45:31Z","cross_cats_sorted":["physics.chem-ph"],"title_canon_sha256":"6ab99292769f1ebbd93602d0a10ac8d0570f54604462ac85336c91d40c185297","abstract_canon_sha256":"1e387e7a353f4109142579b431ef902ea0515dc93489f0f814a50e8207351886"},"schema_version":"1.0"},"canonical_sha256":"79fcf676e56a8bb09ee95ae64aeed929171bfa54b86dea8aea7a15491cf4a0d0","source":{"kind":"arxiv","id":"1203.3296","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1203.3296","created_at":"2026-05-18T04:00:02Z"},{"alias_kind":"arxiv_version","alias_value":"1203.3296v1","created_at":"2026-05-18T04:00:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1203.3296","created_at":"2026-05-18T04:00:02Z"},{"alias_kind":"pith_short_12","alias_value":"PH6PM5XFNKF3","created_at":"2026-05-18T12:27:18Z"},{"alias_kind":"pith_short_16","alias_value":"PH6PM5XFNKF3BHXJ","created_at":"2026-05-18T12:27:18Z"},{"alias_kind":"pith_short_8","alias_value":"PH6PM5XF","created_at":"2026-05-18T12:27:18Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:PH6PM5XFNKF3BHXJLLTEV3WZFE","target":"record","payload":{"canonical_record":{"source":{"id":"1203.3296","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-03-15T09:45:31Z","cross_cats_sorted":["physics.chem-ph"],"title_canon_sha256":"6ab99292769f1ebbd93602d0a10ac8d0570f54604462ac85336c91d40c185297","abstract_canon_sha256":"1e387e7a353f4109142579b431ef902ea0515dc93489f0f814a50e8207351886"},"schema_version":"1.0"},"canonical_sha256":"79fcf676e56a8bb09ee95ae64aeed929171bfa54b86dea8aea7a15491cf4a0d0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:00:02.253664Z","signature_b64":"O7cuiWB6K+zprOJF3ukUj3P8C8p/0uS5I8lOl/PTJtX1wlNhUAxyWFW70/sB9gqQ+4n2WkMKVQryYJzjivZkCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"79fcf676e56a8bb09ee95ae64aeed929171bfa54b86dea8aea7a15491cf4a0d0","last_reissued_at":"2026-05-18T04:00:02.253008Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:00:02.253008Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1203.3296","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":"2026-05-18T04:00:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/3eual4r3Zt1hT9OvtkUMhCUWECsrkabUcFNT4nNelZvdrMEVR8RZ5C7YdIMPVUb3yWS0uHIg4OUihHWhyinDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-21T17:33:55.531283Z"},"content_sha256":"a38a48d1f110d9e22d4d486deee5244d520cae80823e161a9a8c2c285e8c9bf2","schema_version":"1.0","event_id":"sha256:a38a48d1f110d9e22d4d486deee5244d520cae80823e161a9a8c2c285e8c9bf2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:PH6PM5XFNKF3BHXJLLTEV3WZFE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Unusual Response to a Localized Perturbation in a Generalized Elastic Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.chem-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Aleksei Chechkin, Alessandro Taloni, Joseph Klafter","submitted_at":"2012-03-15T09:45:31Z","abstract_excerpt":"The generalized elastic model encompasses several physical systems such as polymers, membranes, single file systems, fluctuating surfaces and rough interfaces. We consider the case of an applied localized potential, namely an external force acting only on a single (tagged) probe, leaving the rest of the system unaffected. We derive the fractional Langevin equation for the tagged probe, as well as for a generic (untagged) probe, where the force is not directly applied. Within the framework of the fluctuation-dissipation relations, we discuss the unexpected physical scenarios arising when the fo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1203.3296","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":"2026-05-18T04:00:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Sj1R6LA8JFuedcHQ73iHt4TEa7c6NaYqFyAT5KjmcEgiS+3ZxkjMUnipWMu0hr0jkkIX7zpBd1tvBaHtWQTFCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-21T17:33:55.531650Z"},"content_sha256":"6bc58305bb49215cdc898c58a0746b07a4535fb0131543c0ce1837330cf6e737","schema_version":"1.0","event_id":"sha256:6bc58305bb49215cdc898c58a0746b07a4535fb0131543c0ce1837330cf6e737"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PH6PM5XFNKF3BHXJLLTEV3WZFE/bundle.json","state_url":"https://pith.science/pith/PH6PM5XFNKF3BHXJLLTEV3WZFE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PH6PM5XFNKF3BHXJLLTEV3WZFE/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":"2026-06-21T17:33:55Z","links":{"resolver":"https://pith.science/pith/PH6PM5XFNKF3BHXJLLTEV3WZFE","bundle":"https://pith.science/pith/PH6PM5XFNKF3BHXJLLTEV3WZFE/bundle.json","state":"https://pith.science/pith/PH6PM5XFNKF3BHXJLLTEV3WZFE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PH6PM5XFNKF3BHXJLLTEV3WZFE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:PH6PM5XFNKF3BHXJLLTEV3WZFE","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":"1e387e7a353f4109142579b431ef902ea0515dc93489f0f814a50e8207351886","cross_cats_sorted":["physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-03-15T09:45:31Z","title_canon_sha256":"6ab99292769f1ebbd93602d0a10ac8d0570f54604462ac85336c91d40c185297"},"schema_version":"1.0","source":{"id":"1203.3296","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1203.3296","created_at":"2026-05-18T04:00:02Z"},{"alias_kind":"arxiv_version","alias_value":"1203.3296v1","created_at":"2026-05-18T04:00:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1203.3296","created_at":"2026-05-18T04:00:02Z"},{"alias_kind":"pith_short_12","alias_value":"PH6PM5XFNKF3","created_at":"2026-05-18T12:27:18Z"},{"alias_kind":"pith_short_16","alias_value":"PH6PM5XFNKF3BHXJ","created_at":"2026-05-18T12:27:18Z"},{"alias_kind":"pith_short_8","alias_value":"PH6PM5XF","created_at":"2026-05-18T12:27:18Z"}],"graph_snapshots":[{"event_id":"sha256:6bc58305bb49215cdc898c58a0746b07a4535fb0131543c0ce1837330cf6e737","target":"graph","created_at":"2026-05-18T04:00:02Z","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 generalized elastic model encompasses several physical systems such as polymers, membranes, single file systems, fluctuating surfaces and rough interfaces. We consider the case of an applied localized potential, namely an external force acting only on a single (tagged) probe, leaving the rest of the system unaffected. We derive the fractional Langevin equation for the tagged probe, as well as for a generic (untagged) probe, where the force is not directly applied. Within the framework of the fluctuation-dissipation relations, we discuss the unexpected physical scenarios arising when the fo","authors_text":"Aleksei Chechkin, Alessandro Taloni, Joseph Klafter","cross_cats":["physics.chem-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-03-15T09:45:31Z","title":"Unusual Response to a Localized Perturbation in a Generalized Elastic Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1203.3296","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:a38a48d1f110d9e22d4d486deee5244d520cae80823e161a9a8c2c285e8c9bf2","target":"record","created_at":"2026-05-18T04:00:02Z","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":"1e387e7a353f4109142579b431ef902ea0515dc93489f0f814a50e8207351886","cross_cats_sorted":["physics.chem-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-03-15T09:45:31Z","title_canon_sha256":"6ab99292769f1ebbd93602d0a10ac8d0570f54604462ac85336c91d40c185297"},"schema_version":"1.0","source":{"id":"1203.3296","kind":"arxiv","version":1}},"canonical_sha256":"79fcf676e56a8bb09ee95ae64aeed929171bfa54b86dea8aea7a15491cf4a0d0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"79fcf676e56a8bb09ee95ae64aeed929171bfa54b86dea8aea7a15491cf4a0d0","first_computed_at":"2026-05-18T04:00:02.253008Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:00:02.253008Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"O7cuiWB6K+zprOJF3ukUj3P8C8p/0uS5I8lOl/PTJtX1wlNhUAxyWFW70/sB9gqQ+4n2WkMKVQryYJzjivZkCA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:00:02.253664Z","signed_message":"canonical_sha256_bytes"},"source_id":"1203.3296","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a38a48d1f110d9e22d4d486deee5244d520cae80823e161a9a8c2c285e8c9bf2","sha256:6bc58305bb49215cdc898c58a0746b07a4535fb0131543c0ce1837330cf6e737"],"state_sha256":"218eaed690abc08dc03b0f43149598d16117c6054f5a4580ec2e277319b91962"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SR99wAJactfidcCc0PGKuvUIQrYHFwD+yyUd/soyjgv2JW5i14XlCXlNI6gn4mhvWQUP97QTUuOvXthJgXyJDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-21T17:33:55.533594Z","bundle_sha256":"b68e17cd7d29883c6e1ff5f410196c848bf6b75373865d50ece7efc31c1ac158"}}