{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:6RJZXCYLXAMIFBKNVEJONEK5NQ","short_pith_number":"pith:6RJZXCYL","schema_version":"1.0","canonical_sha256":"f4539b8b0bb81882854da912e6915d6c204ce982ca601627090e8f1478fad946","source":{"kind":"arxiv","id":"1103.6285","version":2},"attestation_state":"computed","paper":{"title":"Phase diagram for the $\\nu=0$ quantum Hall state in monolayer graphene","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Maxim Kharitonov","submitted_at":"2011-03-31T19:58:34Z","abstract_excerpt":"The $\\nu=0$ quantum Hall state in a defect-free graphene sample is studied within the framework of quantum Hall ferromagnetism. We perform a systematic analysis of the pseudospin anisotropies, which arise from the valley and sublattice asymmetric short-range electron-electron (e-e) and electron-phonon (e-ph) interactions. The phase diagram, obtained in the presence of generic pseudospin anisotropy and the Zeeman effect, consists of four phases characterized by the following orders: spin-polarized ferromagnetic, canted antiferromagnetic, charge density wave, and Kekul\\'{e} distortion. We take i"},"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":"1103.6285","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-03-31T19:58:34Z","cross_cats_sorted":[],"title_canon_sha256":"1d71a758882a2d4310100fb96c72fa9a70269c7a8bb02ae785526c3debcf580e","abstract_canon_sha256":"3db6c44f228c492bbf3bded42794affcd0e0258e89cef8adbd7adb60b8294de5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:57:25.284388Z","signature_b64":"F4ggSThLOAWQUlJ8HHDRONxVKVIi5V6RP3NBz3Aew8TLwWJ36gV4TcdiqET8zE3fob9wIzr+AanfmjeTAoPjDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f4539b8b0bb81882854da912e6915d6c204ce982ca601627090e8f1478fad946","last_reissued_at":"2026-05-18T03:57:25.283487Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:57:25.283487Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phase diagram for the $\\nu=0$ quantum Hall state in monolayer graphene","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Maxim Kharitonov","submitted_at":"2011-03-31T19:58:34Z","abstract_excerpt":"The $\\nu=0$ quantum Hall state in a defect-free graphene sample is studied within the framework of quantum Hall ferromagnetism. We perform a systematic analysis of the pseudospin anisotropies, which arise from the valley and sublattice asymmetric short-range electron-electron (e-e) and electron-phonon (e-ph) interactions. The phase diagram, obtained in the presence of generic pseudospin anisotropy and the Zeeman effect, consists of four phases characterized by the following orders: spin-polarized ferromagnetic, canted antiferromagnetic, charge density wave, and Kekul\\'{e} distortion. We take i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1103.6285","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":"1103.6285","created_at":"2026-05-18T03:57:25.283642+00:00"},{"alias_kind":"arxiv_version","alias_value":"1103.6285v2","created_at":"2026-05-18T03:57:25.283642+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1103.6285","created_at":"2026-05-18T03:57:25.283642+00:00"},{"alias_kind":"pith_short_12","alias_value":"6RJZXCYLXAMI","created_at":"2026-05-18T12:26:22.705136+00:00"},{"alias_kind":"pith_short_16","alias_value":"6RJZXCYLXAMIFBKN","created_at":"2026-05-18T12:26:22.705136+00:00"},{"alias_kind":"pith_short_8","alias_value":"6RJZXCYL","created_at":"2026-05-18T12:26:22.705136+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/6RJZXCYLXAMIFBKNVEJONEK5NQ","json":"https://pith.science/pith/6RJZXCYLXAMIFBKNVEJONEK5NQ.json","graph_json":"https://pith.science/api/pith-number/6RJZXCYLXAMIFBKNVEJONEK5NQ/graph.json","events_json":"https://pith.science/api/pith-number/6RJZXCYLXAMIFBKNVEJONEK5NQ/events.json","paper":"https://pith.science/paper/6RJZXCYL"},"agent_actions":{"view_html":"https://pith.science/pith/6RJZXCYLXAMIFBKNVEJONEK5NQ","download_json":"https://pith.science/pith/6RJZXCYLXAMIFBKNVEJONEK5NQ.json","view_paper":"https://pith.science/paper/6RJZXCYL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1103.6285&json=true","fetch_graph":"https://pith.science/api/pith-number/6RJZXCYLXAMIFBKNVEJONEK5NQ/graph.json","fetch_events":"https://pith.science/api/pith-number/6RJZXCYLXAMIFBKNVEJONEK5NQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6RJZXCYLXAMIFBKNVEJONEK5NQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6RJZXCYLXAMIFBKNVEJONEK5NQ/action/storage_attestation","attest_author":"https://pith.science/pith/6RJZXCYLXAMIFBKNVEJONEK5NQ/action/author_attestation","sign_citation":"https://pith.science/pith/6RJZXCYLXAMIFBKNVEJONEK5NQ/action/citation_signature","submit_replication":"https://pith.science/pith/6RJZXCYLXAMIFBKNVEJONEK5NQ/action/replication_record"}},"created_at":"2026-05-18T03:57:25.283642+00:00","updated_at":"2026-05-18T03:57:25.283642+00:00"}