{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:AIXTFX6EOMDFTW5XCPFRZPOMX4","short_pith_number":"pith:AIXTFX6E","schema_version":"1.0","canonical_sha256":"022f32dfc4730659dbb713cb1cbdccbf00fb82d8a2408716ecbb16d3e479bb30","source":{"kind":"arxiv","id":"1407.4002","version":3},"attestation_state":"computed","paper":{"title":"Z$_N$ parafermion zero modes without Fractional Quantum Hall effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A.M. Tsvelik","submitted_at":"2014-07-15T14:20:13Z","abstract_excerpt":"I discuss a one-dimensional model of interacting fermions which collective excitations are Z$_N$-parafermions. The phase diagram of this model contains ground states with Charge Density Wave and superconducting quasi long range order. Boundaries between these phases contain zero energy parafermion modes."},"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":"1407.4002","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-07-15T14:20:13Z","cross_cats_sorted":[],"title_canon_sha256":"d87d7c7274de8a7b84f45415b325a4b9e5d936573a9cfaa258d0599b9d61af10","abstract_canon_sha256":"12ed47b2b77818cb1f7b7644a242705f5175b45db56fdadad3924118c085de00"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:45:22.922826Z","signature_b64":"BBRvcd6OR52J/YJFhRNPxl7mYIdXX1Qv6rhyhwolF9hqGK+3d+QfkJ1FkhYMsBYId6999+3cAhWk6JGRnghhBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"022f32dfc4730659dbb713cb1cbdccbf00fb82d8a2408716ecbb16d3e479bb30","last_reissued_at":"2026-05-18T02:45:22.922428Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:45:22.922428Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Z$_N$ parafermion zero modes without Fractional Quantum Hall effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A.M. Tsvelik","submitted_at":"2014-07-15T14:20:13Z","abstract_excerpt":"I discuss a one-dimensional model of interacting fermions which collective excitations are Z$_N$-parafermions. The phase diagram of this model contains ground states with Charge Density Wave and superconducting quasi long range order. Boundaries between these phases contain zero energy parafermion modes."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.4002","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1407.4002","created_at":"2026-05-18T02:45:22.922483+00:00"},{"alias_kind":"arxiv_version","alias_value":"1407.4002v3","created_at":"2026-05-18T02:45:22.922483+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.4002","created_at":"2026-05-18T02:45:22.922483+00:00"},{"alias_kind":"pith_short_12","alias_value":"AIXTFX6EOMDF","created_at":"2026-05-18T12:28:19.803747+00:00"},{"alias_kind":"pith_short_16","alias_value":"AIXTFX6EOMDFTW5X","created_at":"2026-05-18T12:28:19.803747+00:00"},{"alias_kind":"pith_short_8","alias_value":"AIXTFX6E","created_at":"2026-05-18T12:28:19.803747+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/AIXTFX6EOMDFTW5XCPFRZPOMX4","json":"https://pith.science/pith/AIXTFX6EOMDFTW5XCPFRZPOMX4.json","graph_json":"https://pith.science/api/pith-number/AIXTFX6EOMDFTW5XCPFRZPOMX4/graph.json","events_json":"https://pith.science/api/pith-number/AIXTFX6EOMDFTW5XCPFRZPOMX4/events.json","paper":"https://pith.science/paper/AIXTFX6E"},"agent_actions":{"view_html":"https://pith.science/pith/AIXTFX6EOMDFTW5XCPFRZPOMX4","download_json":"https://pith.science/pith/AIXTFX6EOMDFTW5XCPFRZPOMX4.json","view_paper":"https://pith.science/paper/AIXTFX6E","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1407.4002&json=true","fetch_graph":"https://pith.science/api/pith-number/AIXTFX6EOMDFTW5XCPFRZPOMX4/graph.json","fetch_events":"https://pith.science/api/pith-number/AIXTFX6EOMDFTW5XCPFRZPOMX4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AIXTFX6EOMDFTW5XCPFRZPOMX4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AIXTFX6EOMDFTW5XCPFRZPOMX4/action/storage_attestation","attest_author":"https://pith.science/pith/AIXTFX6EOMDFTW5XCPFRZPOMX4/action/author_attestation","sign_citation":"https://pith.science/pith/AIXTFX6EOMDFTW5XCPFRZPOMX4/action/citation_signature","submit_replication":"https://pith.science/pith/AIXTFX6EOMDFTW5XCPFRZPOMX4/action/replication_record"}},"created_at":"2026-05-18T02:45:22.922483+00:00","updated_at":"2026-05-18T02:45:22.922483+00:00"}