{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:SGTDRKEG7YDW3KCQQVSSTY7FTW","short_pith_number":"pith:SGTDRKEG","schema_version":"1.0","canonical_sha256":"91a638a886fe076da850856529e3e59dacd653399161720b5607acc37d40562c","source":{"kind":"arxiv","id":"1404.2926","version":2},"attestation_state":"computed","paper":{"title":"Competing charge-density-wave, magnetic and topological ground states at and near Dirac points in graphene in axial magnetic fields","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"Bitan Roy, Jay D. Sau","submitted_at":"2014-04-10T19:59:47Z","abstract_excerpt":"In the presence of axial magnetic fields that can be realized in deliberately buckled monolayer graphene, quasi-relativistic Dirac fermions may find themselves in a variety of broken symmetry phases even for weak interactions. Through a detailed Hartree self-consistent numerical calculation in finite strained graphene with cylindrical and open boundaries we establish the possibility of realizing a charge-density-wave order for the spinless fermions in the presence of weak nearest-neighbor repulsion. Such an instability gives rise to a staggered pattern of average fermionic density between bulk"},"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":"1404.2926","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-04-10T19:59:47Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"8056cb5d8e49e384a51f3e1e9ee3093be1d97b5f442b8d3a733d800a94821815","abstract_canon_sha256":"6938bf1d874dafac9612897fd72cdc262a1ab9ea13577f24ffcf95757a18a39d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:43:46.887281Z","signature_b64":"lQqAeg3rnotP0TkH+CJ+EVLHSp4tc9gV5vHybyoQVVccrvx+V4vCO4mxtYpD4XCe9OXvcdBLuuSEtNOIDEl4AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"91a638a886fe076da850856529e3e59dacd653399161720b5607acc37d40562c","last_reissued_at":"2026-05-18T02:43:46.886779Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:43:46.886779Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Competing charge-density-wave, magnetic and topological ground states at and near Dirac points in graphene in axial magnetic fields","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"Bitan Roy, Jay D. Sau","submitted_at":"2014-04-10T19:59:47Z","abstract_excerpt":"In the presence of axial magnetic fields that can be realized in deliberately buckled monolayer graphene, quasi-relativistic Dirac fermions may find themselves in a variety of broken symmetry phases even for weak interactions. Through a detailed Hartree self-consistent numerical calculation in finite strained graphene with cylindrical and open boundaries we establish the possibility of realizing a charge-density-wave order for the spinless fermions in the presence of weak nearest-neighbor repulsion. Such an instability gives rise to a staggered pattern of average fermionic density between bulk"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.2926","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":"1404.2926","created_at":"2026-05-18T02:43:46.886852+00:00"},{"alias_kind":"arxiv_version","alias_value":"1404.2926v2","created_at":"2026-05-18T02:43:46.886852+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.2926","created_at":"2026-05-18T02:43:46.886852+00:00"},{"alias_kind":"pith_short_12","alias_value":"SGTDRKEG7YDW","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_16","alias_value":"SGTDRKEG7YDW3KCQ","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_8","alias_value":"SGTDRKEG","created_at":"2026-05-18T12:28:49.207871+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/SGTDRKEG7YDW3KCQQVSSTY7FTW","json":"https://pith.science/pith/SGTDRKEG7YDW3KCQQVSSTY7FTW.json","graph_json":"https://pith.science/api/pith-number/SGTDRKEG7YDW3KCQQVSSTY7FTW/graph.json","events_json":"https://pith.science/api/pith-number/SGTDRKEG7YDW3KCQQVSSTY7FTW/events.json","paper":"https://pith.science/paper/SGTDRKEG"},"agent_actions":{"view_html":"https://pith.science/pith/SGTDRKEG7YDW3KCQQVSSTY7FTW","download_json":"https://pith.science/pith/SGTDRKEG7YDW3KCQQVSSTY7FTW.json","view_paper":"https://pith.science/paper/SGTDRKEG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1404.2926&json=true","fetch_graph":"https://pith.science/api/pith-number/SGTDRKEG7YDW3KCQQVSSTY7FTW/graph.json","fetch_events":"https://pith.science/api/pith-number/SGTDRKEG7YDW3KCQQVSSTY7FTW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SGTDRKEG7YDW3KCQQVSSTY7FTW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SGTDRKEG7YDW3KCQQVSSTY7FTW/action/storage_attestation","attest_author":"https://pith.science/pith/SGTDRKEG7YDW3KCQQVSSTY7FTW/action/author_attestation","sign_citation":"https://pith.science/pith/SGTDRKEG7YDW3KCQQVSSTY7FTW/action/citation_signature","submit_replication":"https://pith.science/pith/SGTDRKEG7YDW3KCQQVSSTY7FTW/action/replication_record"}},"created_at":"2026-05-18T02:43:46.886852+00:00","updated_at":"2026-05-18T02:43:46.886852+00:00"}