{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:EJ5TIGNJTN256ST6SYUHVHMZFL","short_pith_number":"pith:EJ5TIGNJ","schema_version":"1.0","canonical_sha256":"227b3419a99b75df4a7e96287a9d992af7f144e1b520553b8b397a2a30042861","source":{"kind":"arxiv","id":"hep-lat/0509038","version":2},"attestation_state":"computed","paper":{"title":"Fermion propagators in QED3 with velocity anisotropies","license":"","headline":"","cross_cats":["cond-mat.str-el","cond-mat.supr-con"],"primary_cat":"hep-lat","authors_text":"Iorwerth Owain Thomas, Simon Hands (University of Wales Swansea)","submitted_at":"2005-09-13T15:25:06Z","abstract_excerpt":"QED3 with fermi and gap anisotropies is considered to be a candidate effective field theory of high temperature superconductors. Simulations of a variant of the theory have demonstrated that there is evidence consistent with a phase transition to a chirally restored phase as the velocity anisotropy increases, and that the correlation lengths of pions in spatial directions behave in a manner consistent with the anisotropy being a relevant parameter of the theory. We present the first measurements of the fermion propagator in Landau gauge for this theory and suggest that the structure of this th"},"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":"hep-lat/0509038","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2005-09-13T15:25:06Z","cross_cats_sorted":["cond-mat.str-el","cond-mat.supr-con"],"title_canon_sha256":"62f033ef0367393e60d33e18cebf6c078d900e6fd395f5065d116ad1581748c9","abstract_canon_sha256":"831fa1e294dcc034085189ce28080ee7d9ca8f140dca93d69e7be1da6666889a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:38.897631Z","signature_b64":"UVfoIezeDTi/nwMqKIPIGN/qi57wrLmODitBleHGwuxVA69CIuA7cXanfX4WHQ/oO6g4FXll3xXyL1CBqhGMCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"227b3419a99b75df4a7e96287a9d992af7f144e1b520553b8b397a2a30042861","last_reissued_at":"2026-05-18T01:06:38.897037Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:38.897037Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Fermion propagators in QED3 with velocity anisotropies","license":"","headline":"","cross_cats":["cond-mat.str-el","cond-mat.supr-con"],"primary_cat":"hep-lat","authors_text":"Iorwerth Owain Thomas, Simon Hands (University of Wales Swansea)","submitted_at":"2005-09-13T15:25:06Z","abstract_excerpt":"QED3 with fermi and gap anisotropies is considered to be a candidate effective field theory of high temperature superconductors. Simulations of a variant of the theory have demonstrated that there is evidence consistent with a phase transition to a chirally restored phase as the velocity anisotropy increases, and that the correlation lengths of pions in spatial directions behave in a manner consistent with the anisotropy being a relevant parameter of the theory. We present the first measurements of the fermion propagator in Landau gauge for this theory and suggest that the structure of this th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0509038","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/0509038","created_at":"2026-05-18T01:06:38.897123+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0509038v2","created_at":"2026-05-18T01:06:38.897123+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0509038","created_at":"2026-05-18T01:06:38.897123+00:00"},{"alias_kind":"pith_short_12","alias_value":"EJ5TIGNJTN25","created_at":"2026-05-18T12:25:53.335082+00:00"},{"alias_kind":"pith_short_16","alias_value":"EJ5TIGNJTN256ST6","created_at":"2026-05-18T12:25:53.335082+00:00"},{"alias_kind":"pith_short_8","alias_value":"EJ5TIGNJ","created_at":"2026-05-18T12:25:53.335082+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/EJ5TIGNJTN256ST6SYUHVHMZFL","json":"https://pith.science/pith/EJ5TIGNJTN256ST6SYUHVHMZFL.json","graph_json":"https://pith.science/api/pith-number/EJ5TIGNJTN256ST6SYUHVHMZFL/graph.json","events_json":"https://pith.science/api/pith-number/EJ5TIGNJTN256ST6SYUHVHMZFL/events.json","paper":"https://pith.science/paper/EJ5TIGNJ"},"agent_actions":{"view_html":"https://pith.science/pith/EJ5TIGNJTN256ST6SYUHVHMZFL","download_json":"https://pith.science/pith/EJ5TIGNJTN256ST6SYUHVHMZFL.json","view_paper":"https://pith.science/paper/EJ5TIGNJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0509038&json=true","fetch_graph":"https://pith.science/api/pith-number/EJ5TIGNJTN256ST6SYUHVHMZFL/graph.json","fetch_events":"https://pith.science/api/pith-number/EJ5TIGNJTN256ST6SYUHVHMZFL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EJ5TIGNJTN256ST6SYUHVHMZFL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EJ5TIGNJTN256ST6SYUHVHMZFL/action/storage_attestation","attest_author":"https://pith.science/pith/EJ5TIGNJTN256ST6SYUHVHMZFL/action/author_attestation","sign_citation":"https://pith.science/pith/EJ5TIGNJTN256ST6SYUHVHMZFL/action/citation_signature","submit_replication":"https://pith.science/pith/EJ5TIGNJTN256ST6SYUHVHMZFL/action/replication_record"}},"created_at":"2026-05-18T01:06:38.897123+00:00","updated_at":"2026-05-18T01:06:38.897123+00:00"}