{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:46NHVMLUPHE7LBZBVBJARDEQ4S","short_pith_number":"pith:46NHVMLU","schema_version":"1.0","canonical_sha256":"e79a7ab17479c9f58721a852088c90e49546af4674adcc4642c6dae3161af396","source":{"kind":"arxiv","id":"2503.19963","version":1},"attestation_state":"computed","paper":{"title":"Gross-Neveu-XY quantum criticality in moir\\'e Dirac materials","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Bilal Hawashin, Lukas Janssen, Michael M. Scherer","submitted_at":"2025-03-25T18:00:01Z","abstract_excerpt":"Two-dimensional van-der-Waals materials offer a highly tunable platform for engineering electronic band structures and interactions. By employing techniques such as twisting, gating, or applying pressure, these systems enable precise control over the electronic excitation spectrum. In moir\\'e bilayer graphene, the tunability facilitates the transition from a symmetric Dirac semimetal phase through a quantum critical point into an interaction-induced long-range ordered phase with a finite band gap. At charge neutrality, the ordered state proposed to emerge from twist-angle tuning is the Kramers"},"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":"2503.19963","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-03-25T18:00:01Z","cross_cats_sorted":["cond-mat.mes-hall","hep-th"],"title_canon_sha256":"0633c18d75231b39390c9a1b4462d498d455ca4d20a5d98ce8e46a5afa426ea9","abstract_canon_sha256":"017fd14f983d632d3231bc80f382d0519b7d5f9ad6731d447291eb2df7523f41"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:14:57.164470Z","signature_b64":"jsyjioFQNzWHoJtjDd3xznmMf4Lcesq0xR1KSR5W/KImptyxgeyWQqRWRmF+Xe/zvvat9U5jk9wkEJvSd9KRCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e79a7ab17479c9f58721a852088c90e49546af4674adcc4642c6dae3161af396","last_reissued_at":"2026-07-05T11:14:57.163875Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:14:57.163875Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gross-Neveu-XY quantum criticality in moir\\'e Dirac materials","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","hep-th"],"primary_cat":"cond-mat.str-el","authors_text":"Bilal Hawashin, Lukas Janssen, Michael M. Scherer","submitted_at":"2025-03-25T18:00:01Z","abstract_excerpt":"Two-dimensional van-der-Waals materials offer a highly tunable platform for engineering electronic band structures and interactions. By employing techniques such as twisting, gating, or applying pressure, these systems enable precise control over the electronic excitation spectrum. In moir\\'e bilayer graphene, the tunability facilitates the transition from a symmetric Dirac semimetal phase through a quantum critical point into an interaction-induced long-range ordered phase with a finite band gap. At charge neutrality, the ordered state proposed to emerge from twist-angle tuning is the Kramers"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2503.19963","kind":"arxiv","version":1},"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/2503.19963/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":"2503.19963","created_at":"2026-07-05T11:14:57.163943+00:00"},{"alias_kind":"arxiv_version","alias_value":"2503.19963v1","created_at":"2026-07-05T11:14:57.163943+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2503.19963","created_at":"2026-07-05T11:14:57.163943+00:00"},{"alias_kind":"pith_short_12","alias_value":"46NHVMLUPHE7","created_at":"2026-07-05T11:14:57.163943+00:00"},{"alias_kind":"pith_short_16","alias_value":"46NHVMLUPHE7LBZB","created_at":"2026-07-05T11:14:57.163943+00:00"},{"alias_kind":"pith_short_8","alias_value":"46NHVMLU","created_at":"2026-07-05T11:14:57.163943+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2505.22723","citing_title":"Quantum multicriticality and emergent symmetry in Dirac systems with two order parameters at three-loop order","ref_index":45,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/46NHVMLUPHE7LBZBVBJARDEQ4S","json":"https://pith.science/pith/46NHVMLUPHE7LBZBVBJARDEQ4S.json","graph_json":"https://pith.science/api/pith-number/46NHVMLUPHE7LBZBVBJARDEQ4S/graph.json","events_json":"https://pith.science/api/pith-number/46NHVMLUPHE7LBZBVBJARDEQ4S/events.json","paper":"https://pith.science/paper/46NHVMLU"},"agent_actions":{"view_html":"https://pith.science/pith/46NHVMLUPHE7LBZBVBJARDEQ4S","download_json":"https://pith.science/pith/46NHVMLUPHE7LBZBVBJARDEQ4S.json","view_paper":"https://pith.science/paper/46NHVMLU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2503.19963&json=true","fetch_graph":"https://pith.science/api/pith-number/46NHVMLUPHE7LBZBVBJARDEQ4S/graph.json","fetch_events":"https://pith.science/api/pith-number/46NHVMLUPHE7LBZBVBJARDEQ4S/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/46NHVMLUPHE7LBZBVBJARDEQ4S/action/timestamp_anchor","attest_storage":"https://pith.science/pith/46NHVMLUPHE7LBZBVBJARDEQ4S/action/storage_attestation","attest_author":"https://pith.science/pith/46NHVMLUPHE7LBZBVBJARDEQ4S/action/author_attestation","sign_citation":"https://pith.science/pith/46NHVMLUPHE7LBZBVBJARDEQ4S/action/citation_signature","submit_replication":"https://pith.science/pith/46NHVMLUPHE7LBZBVBJARDEQ4S/action/replication_record"}},"created_at":"2026-07-05T11:14:57.163943+00:00","updated_at":"2026-07-05T11:14:57.163943+00:00"}