{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:MEMWCQ7VVAKGCTBYJVZVE2E3SS","short_pith_number":"pith:MEMWCQ7V","canonical_record":{"source":{"id":"1708.07163","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2017-08-23T19:39:35Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"951000a56979475b327ea990016547d6b20927daa8b6e7e11b25ac0696d84a02","abstract_canon_sha256":"41b9605d74d8e61d237eb0970a79ef09d9eca29886dc5a3d925de4032faa57a0"},"schema_version":"1.0"},"canonical_sha256":"61196143f5a814614c384d7352689b948a69e72f46a0f4a16eae61194a1c8d96","source":{"kind":"arxiv","id":"1708.07163","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.07163","created_at":"2026-05-18T00:24:51Z"},{"alias_kind":"arxiv_version","alias_value":"1708.07163v2","created_at":"2026-05-18T00:24:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.07163","created_at":"2026-05-18T00:24:51Z"},{"alias_kind":"pith_short_12","alias_value":"MEMWCQ7VVAKG","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_16","alias_value":"MEMWCQ7VVAKGCTBY","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_8","alias_value":"MEMWCQ7V","created_at":"2026-05-18T12:31:31Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:MEMWCQ7VVAKGCTBYJVZVE2E3SS","target":"record","payload":{"canonical_record":{"source":{"id":"1708.07163","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2017-08-23T19:39:35Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"951000a56979475b327ea990016547d6b20927daa8b6e7e11b25ac0696d84a02","abstract_canon_sha256":"41b9605d74d8e61d237eb0970a79ef09d9eca29886dc5a3d925de4032faa57a0"},"schema_version":"1.0"},"canonical_sha256":"61196143f5a814614c384d7352689b948a69e72f46a0f4a16eae61194a1c8d96","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:24:51.904948Z","signature_b64":"aHfAWlDigHoP1YdDIoiPzM9EW/1G0ej+mCF6hemIpMdWqsdzV0+NH4na5ujN2VehWlXM1yclfB78dSgFiaw9DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"61196143f5a814614c384d7352689b948a69e72f46a0f4a16eae61194a1c8d96","last_reissued_at":"2026-05-18T00:24:51.904418Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:24:51.904418Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1708.07163","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":"2026-05-18T00:24:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QNICvfmEdNAAaFXwEMHO2AsOFS/C6TE8Lm0aZyNGy15yySnoL8WpI+pxtKXz/jIwKKBiUWxvcCnmkNb9u6IaDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T20:02:00.502578Z"},"content_sha256":"ce047c8f109463de415abe7ccdc1c050650fea1f163ebbde780f37b920ae312d","schema_version":"1.0","event_id":"sha256:ce047c8f109463de415abe7ccdc1c050650fea1f163ebbde780f37b920ae312d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:MEMWCQ7VVAKGCTBYJVZVE2E3SS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Wave function correlations and the AC conductivity of disordered wires beyond the Mott-Berezinskii law","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.dis-nn","authors_text":"Andrei A. Fedorenko, G.M. Falco, Ilya A. Gruzberg","submitted_at":"2017-08-23T19:39:35Z","abstract_excerpt":"In one-dimensional disordered wires electronic states are localized at any energy. Correlations of the states at close positive energies and the AC conductivity $\\sigma(\\omega)$ in the limit of small frequency are described by the Mott-Berezinskii theory. We revisit the instanton approach to the statistics of wave functions and AC transport valid in the tails of the spectrum (large negative energies). Applying our recent results on functional determinants, we calculate exactly the integral over gaussian fluctuations around the exact two-instanton saddle point. We derive correlators of wave fun"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.07163","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":"2026-05-18T00:24:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"eraLL1dH9wFiZCRLb2TR2MAt3lQCxCD4OPYK6CukjCdplsSBr4aSAmN3wVg+/fINE4zmcU3ZjDo8H3wfnYfJBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T20:02:00.503251Z"},"content_sha256":"ca04811258f3050f8918ac3bb48acf0c971cb5a8053fc248ab350b43d71ceb0a","schema_version":"1.0","event_id":"sha256:ca04811258f3050f8918ac3bb48acf0c971cb5a8053fc248ab350b43d71ceb0a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MEMWCQ7VVAKGCTBYJVZVE2E3SS/bundle.json","state_url":"https://pith.science/pith/MEMWCQ7VVAKGCTBYJVZVE2E3SS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MEMWCQ7VVAKGCTBYJVZVE2E3SS/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":"2026-05-26T20:02:00Z","links":{"resolver":"https://pith.science/pith/MEMWCQ7VVAKGCTBYJVZVE2E3SS","bundle":"https://pith.science/pith/MEMWCQ7VVAKGCTBYJVZVE2E3SS/bundle.json","state":"https://pith.science/pith/MEMWCQ7VVAKGCTBYJVZVE2E3SS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MEMWCQ7VVAKGCTBYJVZVE2E3SS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:MEMWCQ7VVAKGCTBYJVZVE2E3SS","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":"41b9605d74d8e61d237eb0970a79ef09d9eca29886dc5a3d925de4032faa57a0","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2017-08-23T19:39:35Z","title_canon_sha256":"951000a56979475b327ea990016547d6b20927daa8b6e7e11b25ac0696d84a02"},"schema_version":"1.0","source":{"id":"1708.07163","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.07163","created_at":"2026-05-18T00:24:51Z"},{"alias_kind":"arxiv_version","alias_value":"1708.07163v2","created_at":"2026-05-18T00:24:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.07163","created_at":"2026-05-18T00:24:51Z"},{"alias_kind":"pith_short_12","alias_value":"MEMWCQ7VVAKG","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_16","alias_value":"MEMWCQ7VVAKGCTBY","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_8","alias_value":"MEMWCQ7V","created_at":"2026-05-18T12:31:31Z"}],"graph_snapshots":[{"event_id":"sha256:ca04811258f3050f8918ac3bb48acf0c971cb5a8053fc248ab350b43d71ceb0a","target":"graph","created_at":"2026-05-18T00:24:51Z","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":"In one-dimensional disordered wires electronic states are localized at any energy. Correlations of the states at close positive energies and the AC conductivity $\\sigma(\\omega)$ in the limit of small frequency are described by the Mott-Berezinskii theory. We revisit the instanton approach to the statistics of wave functions and AC transport valid in the tails of the spectrum (large negative energies). Applying our recent results on functional determinants, we calculate exactly the integral over gaussian fluctuations around the exact two-instanton saddle point. We derive correlators of wave fun","authors_text":"Andrei A. Fedorenko, G.M. Falco, Ilya A. Gruzberg","cross_cats":["cond-mat.mes-hall"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2017-08-23T19:39:35Z","title":"Wave function correlations and the AC conductivity of disordered wires beyond the Mott-Berezinskii law"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.07163","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:ce047c8f109463de415abe7ccdc1c050650fea1f163ebbde780f37b920ae312d","target":"record","created_at":"2026-05-18T00:24:51Z","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":"41b9605d74d8e61d237eb0970a79ef09d9eca29886dc5a3d925de4032faa57a0","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2017-08-23T19:39:35Z","title_canon_sha256":"951000a56979475b327ea990016547d6b20927daa8b6e7e11b25ac0696d84a02"},"schema_version":"1.0","source":{"id":"1708.07163","kind":"arxiv","version":2}},"canonical_sha256":"61196143f5a814614c384d7352689b948a69e72f46a0f4a16eae61194a1c8d96","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"61196143f5a814614c384d7352689b948a69e72f46a0f4a16eae61194a1c8d96","first_computed_at":"2026-05-18T00:24:51.904418Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:24:51.904418Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"aHfAWlDigHoP1YdDIoiPzM9EW/1G0ej+mCF6hemIpMdWqsdzV0+NH4na5ujN2VehWlXM1yclfB78dSgFiaw9DQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:24:51.904948Z","signed_message":"canonical_sha256_bytes"},"source_id":"1708.07163","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ce047c8f109463de415abe7ccdc1c050650fea1f163ebbde780f37b920ae312d","sha256:ca04811258f3050f8918ac3bb48acf0c971cb5a8053fc248ab350b43d71ceb0a"],"state_sha256":"1fe79ff92c39e03ef09d00f457d26407f301d4d487f4bf0c7af6e8ca3fa7de02"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"POCfrqWEKrtxk9tokIebINRXxufPhfKr8laIq1CgMMmPk/lb6GcIpD15QbzCbsRqgg6rV9Sg4xxZMaUY/aQUBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T20:02:00.506697Z","bundle_sha256":"267cb1ead25ecc5c59253a04c43fb026ea8f7d69901af255f084958588601b9d"}}