{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:OVBT6XU54EDXTZ7X6DCISE3LIR","short_pith_number":"pith:OVBT6XU5","schema_version":"1.0","canonical_sha256":"75433f5e9de10779e7f7f0c489136b447cbb89d54f0e43000d7b220a40d64c89","source":{"kind":"arxiv","id":"2507.22594","version":1},"attestation_state":"computed","paper":{"title":"Anomalous dimensions and critical exponents for the Gross-Neveu-Yukawa model at five loops","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.str-el","hep-ph"],"primary_cat":"hep-th","authors_text":"A. Maier, J.A. Gracey, P. Marquard, Y. Schr\\\"oder","submitted_at":"2025-07-30T11:49:40Z","abstract_excerpt":"We renormalize the Gross-Neveu-Yukawa model with an $O(N)$ symmetry to $\\mathcal{O}(\\epsilon^5)$ in $d=4-\\epsilon$ dimensions and determine the anomalous dimensions of the fermion and scalar fields, $\\beta$-functions as well as the scalar field's mass operator. These are used to construct several $N$ dependent critical exponents relevant for quantum transitions in semi-metals and in particular those connected with graphene in three dimensions when $N=2$. Improved exponent estimates for scalar fermion transitions on a honeycomb lattice, when $N=1$, as well as for $N=5$ are also given to compare"},"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":"2507.22594","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2025-07-30T11:49:40Z","cross_cats_sorted":["cond-mat.str-el","hep-ph"],"title_canon_sha256":"5685776df894a456085ed7783d17cdb87ffb4a0659791c4dd6f9ba87ff274f8d","abstract_canon_sha256":"c49b058fb7e977db2748e448d1d830825dc33ae36f151abf5c2b1a0a5b9f749c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:45:45.061968Z","signature_b64":"EmrhcPCUKgaNCtYpwEDeknZjnUxBRAv3jRu+Qz5q9n4O8WojlMreEEWVlOjo+Mtjfzt0iGs1BvS0Bf7mroqACw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"75433f5e9de10779e7f7f0c489136b447cbb89d54f0e43000d7b220a40d64c89","last_reissued_at":"2026-07-05T11:45:45.061491Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:45:45.061491Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anomalous dimensions and critical exponents for the Gross-Neveu-Yukawa model at five loops","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.str-el","hep-ph"],"primary_cat":"hep-th","authors_text":"A. Maier, J.A. Gracey, P. Marquard, Y. Schr\\\"oder","submitted_at":"2025-07-30T11:49:40Z","abstract_excerpt":"We renormalize the Gross-Neveu-Yukawa model with an $O(N)$ symmetry to $\\mathcal{O}(\\epsilon^5)$ in $d=4-\\epsilon$ dimensions and determine the anomalous dimensions of the fermion and scalar fields, $\\beta$-functions as well as the scalar field's mass operator. These are used to construct several $N$ dependent critical exponents relevant for quantum transitions in semi-metals and in particular those connected with graphene in three dimensions when $N=2$. Improved exponent estimates for scalar fermion transitions on a honeycomb lattice, when $N=1$, as well as for $N=5$ are also given to compare"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2507.22594","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/2507.22594/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":"2507.22594","created_at":"2026-07-05T11:45:45.061548+00:00"},{"alias_kind":"arxiv_version","alias_value":"2507.22594v1","created_at":"2026-07-05T11:45:45.061548+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2507.22594","created_at":"2026-07-05T11:45:45.061548+00:00"},{"alias_kind":"pith_short_12","alias_value":"OVBT6XU54EDX","created_at":"2026-07-05T11:45:45.061548+00:00"},{"alias_kind":"pith_short_16","alias_value":"OVBT6XU54EDXTZ7X","created_at":"2026-07-05T11:45:45.061548+00:00"},{"alias_kind":"pith_short_8","alias_value":"OVBT6XU5","created_at":"2026-07-05T11:45:45.061548+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.07510","citing_title":"Boundary criticality in the Gross-Neveu-Yukawa model at higher orders","ref_index":41,"is_internal_anchor":false},{"citing_arxiv_id":"2604.15187","citing_title":"Extraordinary Surface Criticalities for Interacting Fermions","ref_index":39,"is_internal_anchor":false},{"citing_arxiv_id":"2604.10434","citing_title":"Connecting Supersymmetry to Non-Supersymmetric theories: the Gross-Neveu-Yukawa example","ref_index":4,"is_internal_anchor":false},{"citing_arxiv_id":"2604.13464","citing_title":"Four-loop Anomalous Dimensions of Scalar-QED Theory from Operator Product Expansion","ref_index":94,"is_internal_anchor":false},{"citing_arxiv_id":"2604.15187","citing_title":"Extraordinary Surface Criticalities for Interacting Fermions","ref_index":39,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OVBT6XU54EDXTZ7X6DCISE3LIR","json":"https://pith.science/pith/OVBT6XU54EDXTZ7X6DCISE3LIR.json","graph_json":"https://pith.science/api/pith-number/OVBT6XU54EDXTZ7X6DCISE3LIR/graph.json","events_json":"https://pith.science/api/pith-number/OVBT6XU54EDXTZ7X6DCISE3LIR/events.json","paper":"https://pith.science/paper/OVBT6XU5"},"agent_actions":{"view_html":"https://pith.science/pith/OVBT6XU54EDXTZ7X6DCISE3LIR","download_json":"https://pith.science/pith/OVBT6XU54EDXTZ7X6DCISE3LIR.json","view_paper":"https://pith.science/paper/OVBT6XU5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2507.22594&json=true","fetch_graph":"https://pith.science/api/pith-number/OVBT6XU54EDXTZ7X6DCISE3LIR/graph.json","fetch_events":"https://pith.science/api/pith-number/OVBT6XU54EDXTZ7X6DCISE3LIR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OVBT6XU54EDXTZ7X6DCISE3LIR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OVBT6XU54EDXTZ7X6DCISE3LIR/action/storage_attestation","attest_author":"https://pith.science/pith/OVBT6XU54EDXTZ7X6DCISE3LIR/action/author_attestation","sign_citation":"https://pith.science/pith/OVBT6XU54EDXTZ7X6DCISE3LIR/action/citation_signature","submit_replication":"https://pith.science/pith/OVBT6XU54EDXTZ7X6DCISE3LIR/action/replication_record"}},"created_at":"2026-07-05T11:45:45.061548+00:00","updated_at":"2026-07-05T11:45:45.061548+00:00"}