{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:Z7ODK2HDMP2NM2ZCT2IKSYXKZ6","short_pith_number":"pith:Z7ODK2HD","canonical_record":{"source":{"id":"1510.02214","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-10-08T07:39:23Z","cross_cats_sorted":["cond-mat.dis-nn"],"title_canon_sha256":"973822893b79f52b16ee261328c1e62e411b119a3091bcd7dd5bf00e810ca1fe","abstract_canon_sha256":"8896cb6a9549ebf454f671c2f09b40cc4981fbebceec6cae6aef39dc408848a4"},"schema_version":"1.0"},"canonical_sha256":"cfdc3568e363f4d66b229e90a962eacfa34f6a62d48a119c5b873a3757dbec78","source":{"kind":"arxiv","id":"1510.02214","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1510.02214","created_at":"2026-05-18T00:22:53Z"},{"alias_kind":"arxiv_version","alias_value":"1510.02214v3","created_at":"2026-05-18T00:22:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.02214","created_at":"2026-05-18T00:22:53Z"},{"alias_kind":"pith_short_12","alias_value":"Z7ODK2HDMP2N","created_at":"2026-05-18T12:29:52Z"},{"alias_kind":"pith_short_16","alias_value":"Z7ODK2HDMP2NM2ZC","created_at":"2026-05-18T12:29:52Z"},{"alias_kind":"pith_short_8","alias_value":"Z7ODK2HD","created_at":"2026-05-18T12:29:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:Z7ODK2HDMP2NM2ZCT2IKSYXKZ6","target":"record","payload":{"canonical_record":{"source":{"id":"1510.02214","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-10-08T07:39:23Z","cross_cats_sorted":["cond-mat.dis-nn"],"title_canon_sha256":"973822893b79f52b16ee261328c1e62e411b119a3091bcd7dd5bf00e810ca1fe","abstract_canon_sha256":"8896cb6a9549ebf454f671c2f09b40cc4981fbebceec6cae6aef39dc408848a4"},"schema_version":"1.0"},"canonical_sha256":"cfdc3568e363f4d66b229e90a962eacfa34f6a62d48a119c5b873a3757dbec78","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:22:53.129576Z","signature_b64":"b+xqdKaM/xqmetAtOMEg+RzdtzSkKLRjZ7x1lP1dzLjsoGxkrU7TE/dQexrl/rBxwPPtjzPGnxwACU+uJLMtDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cfdc3568e363f4d66b229e90a962eacfa34f6a62d48a119c5b873a3757dbec78","last_reissued_at":"2026-05-18T00:22:53.128978Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:22:53.128978Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1510.02214","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:22:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"l6e1d7a8OUh+qOCx0h/99roFWeHS+kVHR3xND9KoRvDl7gM1V5sS2+9thiZM0e8LzyWGWCrSn7ltB2V2e8tHCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T14:29:08.625242Z"},"content_sha256":"3163df8dcb9320f33b06ef1ab2deb56f17e6d07dfb090693a4f610ec3e6e7838","schema_version":"1.0","event_id":"sha256:3163df8dcb9320f33b06ef1ab2deb56f17e6d07dfb090693a4f610ec3e6e7838"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:Z7ODK2HDMP2NM2ZCT2IKSYXKZ6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Non-linear conductance in mesoscopic weakly disordered wires -- Interaction and magnetic field asymmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn"],"primary_cat":"cond-mat.mes-hall","authors_text":"Christophe Texier, Johannes Mitscherling","submitted_at":"2015-10-08T07:39:23Z","abstract_excerpt":"We study the non-linear conductance $\\mathcal{G}\\sim\\partial^2I/\\partial V^2|_{V=0}$ in coherent quasi-1D weakly disordered metallic wires. The analysis is based on the calculation of two fundamental correlators (correlations of conductance's functional derivatives and correlations of injectivities), which are obtained explicitly by using diagrammatic techniques. In a coherent wire of length $L$, we obtain $\\mathcal{G}\\sim0.006\\,E_\\mathrm{Th}^{-1}$ (and $\\langle\\mathcal{G}\\rangle=0$), where $E_\\mathrm{Th}=D/L^2$ is the Thouless energy and $D$ the diffusion constant; the small dimensionless fac"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1510.02214","kind":"arxiv","version":3},"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":"2026-05-18T00:22:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FXa+IwjUFUIavGA4qfMD8YrCsNWC2zt2LTTqUREBfLFRMZjSaqPDHEcJ5y1Mj0lOut/YiB6uF31azV0AYT+gAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T14:29:08.625741Z"},"content_sha256":"1c13ef993c0fe4a9d5667e87501fddd429515de760e6f8832966ba9d1c229cb5","schema_version":"1.0","event_id":"sha256:1c13ef993c0fe4a9d5667e87501fddd429515de760e6f8832966ba9d1c229cb5"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/Z7ODK2HDMP2NM2ZCT2IKSYXKZ6/bundle.json","state_url":"https://pith.science/pith/Z7ODK2HDMP2NM2ZCT2IKSYXKZ6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/Z7ODK2HDMP2NM2ZCT2IKSYXKZ6/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":"2026-06-02T14:29:08Z","links":{"resolver":"https://pith.science/pith/Z7ODK2HDMP2NM2ZCT2IKSYXKZ6","bundle":"https://pith.science/pith/Z7ODK2HDMP2NM2ZCT2IKSYXKZ6/bundle.json","state":"https://pith.science/pith/Z7ODK2HDMP2NM2ZCT2IKSYXKZ6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/Z7ODK2HDMP2NM2ZCT2IKSYXKZ6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:Z7ODK2HDMP2NM2ZCT2IKSYXKZ6","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":"8896cb6a9549ebf454f671c2f09b40cc4981fbebceec6cae6aef39dc408848a4","cross_cats_sorted":["cond-mat.dis-nn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-10-08T07:39:23Z","title_canon_sha256":"973822893b79f52b16ee261328c1e62e411b119a3091bcd7dd5bf00e810ca1fe"},"schema_version":"1.0","source":{"id":"1510.02214","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1510.02214","created_at":"2026-05-18T00:22:53Z"},{"alias_kind":"arxiv_version","alias_value":"1510.02214v3","created_at":"2026-05-18T00:22:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.02214","created_at":"2026-05-18T00:22:53Z"},{"alias_kind":"pith_short_12","alias_value":"Z7ODK2HDMP2N","created_at":"2026-05-18T12:29:52Z"},{"alias_kind":"pith_short_16","alias_value":"Z7ODK2HDMP2NM2ZC","created_at":"2026-05-18T12:29:52Z"},{"alias_kind":"pith_short_8","alias_value":"Z7ODK2HD","created_at":"2026-05-18T12:29:52Z"}],"graph_snapshots":[{"event_id":"sha256:1c13ef993c0fe4a9d5667e87501fddd429515de760e6f8832966ba9d1c229cb5","target":"graph","created_at":"2026-05-18T00:22:53Z","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":"We study the non-linear conductance $\\mathcal{G}\\sim\\partial^2I/\\partial V^2|_{V=0}$ in coherent quasi-1D weakly disordered metallic wires. The analysis is based on the calculation of two fundamental correlators (correlations of conductance's functional derivatives and correlations of injectivities), which are obtained explicitly by using diagrammatic techniques. In a coherent wire of length $L$, we obtain $\\mathcal{G}\\sim0.006\\,E_\\mathrm{Th}^{-1}$ (and $\\langle\\mathcal{G}\\rangle=0$), where $E_\\mathrm{Th}=D/L^2$ is the Thouless energy and $D$ the diffusion constant; the small dimensionless fac","authors_text":"Christophe Texier, Johannes Mitscherling","cross_cats":["cond-mat.dis-nn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-10-08T07:39:23Z","title":"Non-linear conductance in mesoscopic weakly disordered wires -- Interaction and magnetic field asymmetry"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1510.02214","kind":"arxiv","version":3},"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":"sha256:3163df8dcb9320f33b06ef1ab2deb56f17e6d07dfb090693a4f610ec3e6e7838","target":"record","created_at":"2026-05-18T00:22:53Z","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":"8896cb6a9549ebf454f671c2f09b40cc4981fbebceec6cae6aef39dc408848a4","cross_cats_sorted":["cond-mat.dis-nn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-10-08T07:39:23Z","title_canon_sha256":"973822893b79f52b16ee261328c1e62e411b119a3091bcd7dd5bf00e810ca1fe"},"schema_version":"1.0","source":{"id":"1510.02214","kind":"arxiv","version":3}},"canonical_sha256":"cfdc3568e363f4d66b229e90a962eacfa34f6a62d48a119c5b873a3757dbec78","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"cfdc3568e363f4d66b229e90a962eacfa34f6a62d48a119c5b873a3757dbec78","first_computed_at":"2026-05-18T00:22:53.128978Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:22:53.128978Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"b+xqdKaM/xqmetAtOMEg+RzdtzSkKLRjZ7x1lP1dzLjsoGxkrU7TE/dQexrl/rBxwPPtjzPGnxwACU+uJLMtDg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:22:53.129576Z","signed_message":"canonical_sha256_bytes"},"source_id":"1510.02214","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3163df8dcb9320f33b06ef1ab2deb56f17e6d07dfb090693a4f610ec3e6e7838","sha256:1c13ef993c0fe4a9d5667e87501fddd429515de760e6f8832966ba9d1c229cb5"],"state_sha256":"e697649163e215550ea010e876883d966cb007d62d46fde3b3106d3add19ee82"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TIkqOQFHfJz+w09PeduaHbdjL7fM2+V7NauSI9HGGpCZTm0o/Fc9U1eAybOB0XyEA4tDv2K/XOB1kdC7eS72Bw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T14:29:08.628195Z","bundle_sha256":"9500799d0e4fe89c6862befd3d1bfbfd7d5c2c20c79f6ab42c8a5a9ddce809c3"}}