{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:F47LNZVG3XPOKAHF6TT2Q3TPOJ","short_pith_number":"pith:F47LNZVG","schema_version":"1.0","canonical_sha256":"2f3eb6e6a6dddee500e5f4e7a86e6f7255c2240739d3fd9538d7fe5ca92d6ddc","source":{"kind":"arxiv","id":"2512.10944","version":2},"attestation_state":"computed","paper":{"title":"Pair density wave in quarter metals from a repulsive fermionic interaction in graphene heterostructures: A renormalization group study","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.str-el","cond-mat.supr-con"],"primary_cat":"cond-mat.mes-hall","authors_text":"Bitan Roy, Sk Asrap Murshed","submitted_at":"2025-12-11T18:59:35Z","abstract_excerpt":"Electronic bands in chirally stacked $n$ layer carbon-based honeycomb heterostructures, encompassing rhombohedral or ABC ($n \\geq 3$), Bernal or AB bilayer ($n=2$), and monolayer ($n=1$) graphene, possess four-fold valley and spin degeneracy. Such systems with $n \\geq 2$, when subject to external perpendicular electric displacement fields, feature a fully degenerate metal at high doping, a spin polarized but valley degenerate half-metal at moderate doping, and a non-degenerate quarter metal at low doping. Due to the fully polarized nature of the quasiparticles in the quarter metal, realized ar"},"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":"2512.10944","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2025-12-11T18:59:35Z","cross_cats_sorted":["cond-mat.str-el","cond-mat.supr-con"],"title_canon_sha256":"d120c37cbd4f82d3c800486a39720afe6b243ffbe0fda2dcbee7e18b63ce88b6","abstract_canon_sha256":"dcd74e21578f9279da9acd99b5ba5a7e587da6ad5f9852c7a844f5eee990b8d3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-25T02:02:11.163026Z","signature_b64":"040kVGM5Y67ysodwOqBJFtc7R9OVSfOc/Lk/o3UZy6Op3MHA/+qf2EkChSK7dG7z64VGduNoLlqpY5rLvjuuDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2f3eb6e6a6dddee500e5f4e7a86e6f7255c2240739d3fd9538d7fe5ca92d6ddc","last_reissued_at":"2026-05-25T02:02:11.162098Z","signature_status":"signed_v1","first_computed_at":"2026-05-25T02:02:11.162098Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pair density wave in quarter metals from a repulsive fermionic interaction in graphene heterostructures: A renormalization group study","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.str-el","cond-mat.supr-con"],"primary_cat":"cond-mat.mes-hall","authors_text":"Bitan Roy, Sk Asrap Murshed","submitted_at":"2025-12-11T18:59:35Z","abstract_excerpt":"Electronic bands in chirally stacked $n$ layer carbon-based honeycomb heterostructures, encompassing rhombohedral or ABC ($n \\geq 3$), Bernal or AB bilayer ($n=2$), and monolayer ($n=1$) graphene, possess four-fold valley and spin degeneracy. Such systems with $n \\geq 2$, when subject to external perpendicular electric displacement fields, feature a fully degenerate metal at high doping, a spin polarized but valley degenerate half-metal at moderate doping, and a non-degenerate quarter metal at low doping. Due to the fully polarized nature of the quasiparticles in the quarter metal, realized ar"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2512.10944","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2512.10944/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2512.10944","created_at":"2026-05-25T02:02:11.162234+00:00"},{"alias_kind":"arxiv_version","alias_value":"2512.10944v2","created_at":"2026-05-25T02:02:11.162234+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2512.10944","created_at":"2026-05-25T02:02:11.162234+00:00"},{"alias_kind":"pith_short_12","alias_value":"F47LNZVG3XPO","created_at":"2026-05-25T02:02:11.162234+00:00"},{"alias_kind":"pith_short_16","alias_value":"F47LNZVG3XPOKAHF","created_at":"2026-05-25T02:02:11.162234+00:00"},{"alias_kind":"pith_short_8","alias_value":"F47LNZVG","created_at":"2026-05-25T02:02:11.162234+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/F47LNZVG3XPOKAHF6TT2Q3TPOJ","json":"https://pith.science/pith/F47LNZVG3XPOKAHF6TT2Q3TPOJ.json","graph_json":"https://pith.science/api/pith-number/F47LNZVG3XPOKAHF6TT2Q3TPOJ/graph.json","events_json":"https://pith.science/api/pith-number/F47LNZVG3XPOKAHF6TT2Q3TPOJ/events.json","paper":"https://pith.science/paper/F47LNZVG"},"agent_actions":{"view_html":"https://pith.science/pith/F47LNZVG3XPOKAHF6TT2Q3TPOJ","download_json":"https://pith.science/pith/F47LNZVG3XPOKAHF6TT2Q3TPOJ.json","view_paper":"https://pith.science/paper/F47LNZVG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2512.10944&json=true","fetch_graph":"https://pith.science/api/pith-number/F47LNZVG3XPOKAHF6TT2Q3TPOJ/graph.json","fetch_events":"https://pith.science/api/pith-number/F47LNZVG3XPOKAHF6TT2Q3TPOJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/F47LNZVG3XPOKAHF6TT2Q3TPOJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/F47LNZVG3XPOKAHF6TT2Q3TPOJ/action/storage_attestation","attest_author":"https://pith.science/pith/F47LNZVG3XPOKAHF6TT2Q3TPOJ/action/author_attestation","sign_citation":"https://pith.science/pith/F47LNZVG3XPOKAHF6TT2Q3TPOJ/action/citation_signature","submit_replication":"https://pith.science/pith/F47LNZVG3XPOKAHF6TT2Q3TPOJ/action/replication_record"}},"created_at":"2026-05-25T02:02:11.162234+00:00","updated_at":"2026-05-25T02:02:11.162234+00:00"}