{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:CLQNLKBVZOBBVW33KEPZQSHKDH","short_pith_number":"pith:CLQNLKBV","canonical_record":{"source":{"id":"2408.08791","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2024-08-16T15:03:34Z","cross_cats_sorted":["cond-mat.mes-hall","physics.chem-ph","physics.comp-ph"],"title_canon_sha256":"6cff0bb7a6faa33a6988e9353123280a4c0c63ca398e9b7dc29ba6813dbe4d25","abstract_canon_sha256":"469176c07ee8c09a2a9cc9087256028cb4f2e932a6bdb8ac8ca487e1347e4111"},"schema_version":"1.0"},"canonical_sha256":"12e0d5a835cb821adb7b511f9848ea19c7c8d1f0eec7c0ab106c21aed1eb2244","source":{"kind":"arxiv","id":"2408.08791","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2408.08791","created_at":"2026-07-05T09:14:22Z"},{"alias_kind":"arxiv_version","alias_value":"2408.08791v2","created_at":"2026-07-05T09:14:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2408.08791","created_at":"2026-07-05T09:14:22Z"},{"alias_kind":"pith_short_12","alias_value":"CLQNLKBVZOBB","created_at":"2026-07-05T09:14:22Z"},{"alias_kind":"pith_short_16","alias_value":"CLQNLKBVZOBBVW33","created_at":"2026-07-05T09:14:22Z"},{"alias_kind":"pith_short_8","alias_value":"CLQNLKBV","created_at":"2026-07-05T09:14:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:CLQNLKBVZOBBVW33KEPZQSHKDH","target":"record","payload":{"canonical_record":{"source":{"id":"2408.08791","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2024-08-16T15:03:34Z","cross_cats_sorted":["cond-mat.mes-hall","physics.chem-ph","physics.comp-ph"],"title_canon_sha256":"6cff0bb7a6faa33a6988e9353123280a4c0c63ca398e9b7dc29ba6813dbe4d25","abstract_canon_sha256":"469176c07ee8c09a2a9cc9087256028cb4f2e932a6bdb8ac8ca487e1347e4111"},"schema_version":"1.0"},"canonical_sha256":"12e0d5a835cb821adb7b511f9848ea19c7c8d1f0eec7c0ab106c21aed1eb2244","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:14:22.911546Z","signature_b64":"N0KKAqYwldbCTJXAd4PPeNVz+hMk4aqdxaiUSqPsTvV8UNutxYbTVgxRdZlLQUfjC348RdO33uti8gVHJZH3Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"12e0d5a835cb821adb7b511f9848ea19c7c8d1f0eec7c0ab106c21aed1eb2244","last_reissued_at":"2026-07-05T09:14:22.911121Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:14:22.911121Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2408.08791","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":"2026-07-05T09:14:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZCTlndtKK/OQx41R8Xhp2kVWReaNSEWFK3cG8w4pZJ2UC2DSZ++xpHqnXYIrzzvS8A/DUKgXS0GEzW1Fp2OBAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T01:22:50.960689Z"},"content_sha256":"a6c69d36edaf5d33c61738743d1ef105c6fd5ef11446cdac7f9dcc85c550126a","schema_version":"1.0","event_id":"sha256:a6c69d36edaf5d33c61738743d1ef105c6fd5ef11446cdac7f9dcc85c550126a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:CLQNLKBVZOBBVW33KEPZQSHKDH","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dissipative split-charge formalism: Ohm's law, Nyquist noise, and non-contact friction","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall","physics.chem-ph","physics.comp-ph"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Martin H. M\\\"user","submitted_at":"2024-08-16T15:03:34Z","abstract_excerpt":"The split-charge equilibration method is extended to describe dissipative charge transfer similarly as the Drude model, whereby the generic frequency-dependent dielectric permitivitties or conductivities of dielectrics and metals can be mimicked. To demonstrate the feasibility of the approach, a resistor-capacitor circuit is simulated using an all-atom representation for resistor and capacitor. The simulated dynamics reproduce the expected charging process and Nyquist noise, the latter resulting from the thermal voltages acting on individual split charges. The method bears promise to model fri"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2408.08791","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2408.08791/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T09:14:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"26Xt6dFbf0pFyVVDnr4XKB3m7Bx6HCgLr2l0eYkGGrzSDKXDdP6nCOOA/MNBbG83lWQn8r26TApAFvnHJ4AHAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-06T01:22:50.961201Z"},"content_sha256":"d4791623d7b042aff26e017d576d76ca8d5329c6d32945ccb1c34d42c3b25d86","schema_version":"1.0","event_id":"sha256:d4791623d7b042aff26e017d576d76ca8d5329c6d32945ccb1c34d42c3b25d86"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/CLQNLKBVZOBBVW33KEPZQSHKDH/bundle.json","state_url":"https://pith.science/pith/CLQNLKBVZOBBVW33KEPZQSHKDH/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/CLQNLKBVZOBBVW33KEPZQSHKDH/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":"2026-08-06T01:22:50Z","links":{"resolver":"https://pith.science/pith/CLQNLKBVZOBBVW33KEPZQSHKDH","bundle":"https://pith.science/pith/CLQNLKBVZOBBVW33KEPZQSHKDH/bundle.json","state":"https://pith.science/pith/CLQNLKBVZOBBVW33KEPZQSHKDH/state.json","well_known_bundle":"https://pith.science/.well-known/pith/CLQNLKBVZOBBVW33KEPZQSHKDH/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:CLQNLKBVZOBBVW33KEPZQSHKDH","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":"469176c07ee8c09a2a9cc9087256028cb4f2e932a6bdb8ac8ca487e1347e4111","cross_cats_sorted":["cond-mat.mes-hall","physics.chem-ph","physics.comp-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2024-08-16T15:03:34Z","title_canon_sha256":"6cff0bb7a6faa33a6988e9353123280a4c0c63ca398e9b7dc29ba6813dbe4d25"},"schema_version":"1.0","source":{"id":"2408.08791","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2408.08791","created_at":"2026-07-05T09:14:22Z"},{"alias_kind":"arxiv_version","alias_value":"2408.08791v2","created_at":"2026-07-05T09:14:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2408.08791","created_at":"2026-07-05T09:14:22Z"},{"alias_kind":"pith_short_12","alias_value":"CLQNLKBVZOBB","created_at":"2026-07-05T09:14:22Z"},{"alias_kind":"pith_short_16","alias_value":"CLQNLKBVZOBBVW33","created_at":"2026-07-05T09:14:22Z"},{"alias_kind":"pith_short_8","alias_value":"CLQNLKBV","created_at":"2026-07-05T09:14:22Z"}],"graph_snapshots":[{"event_id":"sha256:d4791623d7b042aff26e017d576d76ca8d5329c6d32945ccb1c34d42c3b25d86","target":"graph","created_at":"2026-07-05T09:14:22Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2408.08791/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The split-charge equilibration method is extended to describe dissipative charge transfer similarly as the Drude model, whereby the generic frequency-dependent dielectric permitivitties or conductivities of dielectrics and metals can be mimicked. To demonstrate the feasibility of the approach, a resistor-capacitor circuit is simulated using an all-atom representation for resistor and capacitor. The simulated dynamics reproduce the expected charging process and Nyquist noise, the latter resulting from the thermal voltages acting on individual split charges. The method bears promise to model fri","authors_text":"Martin H. M\\\"user","cross_cats":["cond-mat.mes-hall","physics.chem-ph","physics.comp-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2024-08-16T15:03:34Z","title":"Dissipative split-charge formalism: Ohm's law, Nyquist noise, and non-contact friction"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2408.08791","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:a6c69d36edaf5d33c61738743d1ef105c6fd5ef11446cdac7f9dcc85c550126a","target":"record","created_at":"2026-07-05T09:14:22Z","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":"469176c07ee8c09a2a9cc9087256028cb4f2e932a6bdb8ac8ca487e1347e4111","cross_cats_sorted":["cond-mat.mes-hall","physics.chem-ph","physics.comp-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2024-08-16T15:03:34Z","title_canon_sha256":"6cff0bb7a6faa33a6988e9353123280a4c0c63ca398e9b7dc29ba6813dbe4d25"},"schema_version":"1.0","source":{"id":"2408.08791","kind":"arxiv","version":2}},"canonical_sha256":"12e0d5a835cb821adb7b511f9848ea19c7c8d1f0eec7c0ab106c21aed1eb2244","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"12e0d5a835cb821adb7b511f9848ea19c7c8d1f0eec7c0ab106c21aed1eb2244","first_computed_at":"2026-07-05T09:14:22.911121Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:14:22.911121Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"N0KKAqYwldbCTJXAd4PPeNVz+hMk4aqdxaiUSqPsTvV8UNutxYbTVgxRdZlLQUfjC348RdO33uti8gVHJZH3Ag==","signature_status":"signed_v1","signed_at":"2026-07-05T09:14:22.911546Z","signed_message":"canonical_sha256_bytes"},"source_id":"2408.08791","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a6c69d36edaf5d33c61738743d1ef105c6fd5ef11446cdac7f9dcc85c550126a","sha256:d4791623d7b042aff26e017d576d76ca8d5329c6d32945ccb1c34d42c3b25d86"],"state_sha256":"75efc47f0fbefc695533e20e31d9dd03f4a638c5985111dd527a59ba3da9feb6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ix/ouV7uMcmsG3cVQr9QMFUzlmj6YohnHimg47auQbpgUnaiL86REuANNVuX3+wRZ9kxa6ujMg3jZf4LbCYsCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-06T01:22:50.965116Z","bundle_sha256":"3743c48a69db7ba2dd5df1164bd354e6e20b181a9dfe0f241de74601d8ec2033"}}