{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:4GMV3KICN5GPDODQIBTXSH7BLR","short_pith_number":"pith:4GMV3KIC","schema_version":"1.0","canonical_sha256":"e1995da9026f4cf1b8704067791fe15c606f8a9ae69ce24f7e5c26fdbd363404","source":{"kind":"arxiv","id":"cond-mat/9609286","version":1},"attestation_state":"computed","paper":{"title":"Conductivity in a symmetry broken phase: Spinless fermions with $1/d$ corrections","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"Goetz S. Uhrig","submitted_at":"1996-09-30T16:25:57Z","abstract_excerpt":"The dynamic conductivity $\\sigma(\\omega)$ of strongly correlated electrons in a symmetry broken phase is investigated in the present work. The model considered consists of spinless fermions with repulsive interaction on a simple cubic lattice. The investigated symmetry broken phase is the charge density wave (CDW) with wave vector $Q=(\\pi,\\pi,\\pi)^\\dagger$ which occurs at half-filling. The calculations are based on the high dimensional approach, i.e. an expansion in the inverse dimension $1/d$ is used. The finite dimensionality is accounted for by the inclusion of linear terms in $1/d$ and the"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"cond-mat/9609286","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"1996-09-30T16:25:57Z","cross_cats_sorted":[],"title_canon_sha256":"3ad206da71053d434b6ec379a45864e83e5692b16820c03deb869de63138f2ce","abstract_canon_sha256":"486661ce3176723964c2b36ff67fafd4e2f078b5880eddc29c9bbd86b0778b16"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:07:09.290849Z","signature_b64":"vrOF7CSVlbPiTB1YlZ97JJQoNdikn7wovJ0dWtkpxJtZJJ9rlExMWMoHkpIrJB9mHQJHx//R6aSfhBJn8PuoAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e1995da9026f4cf1b8704067791fe15c606f8a9ae69ce24f7e5c26fdbd363404","last_reissued_at":"2026-05-18T01:07:09.290361Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:07:09.290361Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Conductivity in a symmetry broken phase: Spinless fermions with $1/d$ corrections","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"Goetz S. Uhrig","submitted_at":"1996-09-30T16:25:57Z","abstract_excerpt":"The dynamic conductivity $\\sigma(\\omega)$ of strongly correlated electrons in a symmetry broken phase is investigated in the present work. The model considered consists of spinless fermions with repulsive interaction on a simple cubic lattice. The investigated symmetry broken phase is the charge density wave (CDW) with wave vector $Q=(\\pi,\\pi,\\pi)^\\dagger$ which occurs at half-filling. The calculations are based on the high dimensional approach, i.e. an expansion in the inverse dimension $1/d$ is used. The finite dimensionality is accounted for by the inclusion of linear terms in $1/d$ and the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9609286","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/9609286","created_at":"2026-05-18T01:07:09.290436+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9609286v1","created_at":"2026-05-18T01:07:09.290436+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9609286","created_at":"2026-05-18T01:07:09.290436+00:00"},{"alias_kind":"pith_short_12","alias_value":"4GMV3KICN5GP","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_16","alias_value":"4GMV3KICN5GPDODQ","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_8","alias_value":"4GMV3KIC","created_at":"2026-05-18T12:25:47.700082+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4GMV3KICN5GPDODQIBTXSH7BLR","json":"https://pith.science/pith/4GMV3KICN5GPDODQIBTXSH7BLR.json","graph_json":"https://pith.science/api/pith-number/4GMV3KICN5GPDODQIBTXSH7BLR/graph.json","events_json":"https://pith.science/api/pith-number/4GMV3KICN5GPDODQIBTXSH7BLR/events.json","paper":"https://pith.science/paper/4GMV3KIC"},"agent_actions":{"view_html":"https://pith.science/pith/4GMV3KICN5GPDODQIBTXSH7BLR","download_json":"https://pith.science/pith/4GMV3KICN5GPDODQIBTXSH7BLR.json","view_paper":"https://pith.science/paper/4GMV3KIC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/9609286&json=true","fetch_graph":"https://pith.science/api/pith-number/4GMV3KICN5GPDODQIBTXSH7BLR/graph.json","fetch_events":"https://pith.science/api/pith-number/4GMV3KICN5GPDODQIBTXSH7BLR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4GMV3KICN5GPDODQIBTXSH7BLR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4GMV3KICN5GPDODQIBTXSH7BLR/action/storage_attestation","attest_author":"https://pith.science/pith/4GMV3KICN5GPDODQIBTXSH7BLR/action/author_attestation","sign_citation":"https://pith.science/pith/4GMV3KICN5GPDODQIBTXSH7BLR/action/citation_signature","submit_replication":"https://pith.science/pith/4GMV3KICN5GPDODQIBTXSH7BLR/action/replication_record"}},"created_at":"2026-05-18T01:07:09.290436+00:00","updated_at":"2026-05-18T01:07:09.290436+00:00"}