{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:E7MDBD6NPGVTQCC4WIZ4753LO6","short_pith_number":"pith:E7MDBD6N","schema_version":"1.0","canonical_sha256":"27d8308fcd79ab38085cb233cff76b77a84de586d6f1c38fccd59b71c49e3ca1","source":{"kind":"arxiv","id":"1510.07650","version":2},"attestation_state":"computed","paper":{"title":"Emergent Lorentz symmetry near fermionic quantum critical points in two and three dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","cond-mat.str-el"],"primary_cat":"hep-th","authors_text":"Bitan Roy, Igor F. Herbut, Vladimir Juricic","submitted_at":"2015-10-26T20:21:03Z","abstract_excerpt":"We study the renormalization group flow of the velocities in the field theory describing the coupling of the massless quasi-relativistic fermions to the bosons through the Yukawa coupling, as well as with both bosons and fermions coupled to a fluctuating $U(1)$ gauge field in two and three spatial dimensions. Different versions of this theory describe quantum critical behavior of interacting Dirac fermions in various condensed-matter systems. We perform an analysis using one-loop $\\epsilon-$expansion about three spatial dimensions, which is the upper critical dimension in the problem. In two d"},"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":"1510.07650","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-10-26T20:21:03Z","cross_cats_sorted":["cond-mat.stat-mech","cond-mat.str-el"],"title_canon_sha256":"18ebb2c243513c5087b7455304ad91b2bebdd043d8c8a415a5ae615b2d76a886","abstract_canon_sha256":"c4ce9dfff3d4dcde8244188785577e42c024301f23851c1897370a40fb9374d6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:17:18.481949Z","signature_b64":"eNI2FU8iNk0mYSuE+4UJ5wNtU9loHHITl6sybrVjYm6xyfK43Mbj2HNwy2obOKFDN90V0v0mYBBTrTZ4Fe6lAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"27d8308fcd79ab38085cb233cff76b77a84de586d6f1c38fccd59b71c49e3ca1","last_reissued_at":"2026-05-18T01:17:18.481531Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:17:18.481531Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Emergent Lorentz symmetry near fermionic quantum critical points in two and three dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","cond-mat.str-el"],"primary_cat":"hep-th","authors_text":"Bitan Roy, Igor F. Herbut, Vladimir Juricic","submitted_at":"2015-10-26T20:21:03Z","abstract_excerpt":"We study the renormalization group flow of the velocities in the field theory describing the coupling of the massless quasi-relativistic fermions to the bosons through the Yukawa coupling, as well as with both bosons and fermions coupled to a fluctuating $U(1)$ gauge field in two and three spatial dimensions. Different versions of this theory describe quantum critical behavior of interacting Dirac fermions in various condensed-matter systems. We perform an analysis using one-loop $\\epsilon-$expansion about three spatial dimensions, which is the upper critical dimension in the problem. In two d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1510.07650","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":"1510.07650","created_at":"2026-05-18T01:17:18.481596+00:00"},{"alias_kind":"arxiv_version","alias_value":"1510.07650v2","created_at":"2026-05-18T01:17:18.481596+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.07650","created_at":"2026-05-18T01:17:18.481596+00:00"},{"alias_kind":"pith_short_12","alias_value":"E7MDBD6NPGVT","created_at":"2026-05-18T12:29:19.899920+00:00"},{"alias_kind":"pith_short_16","alias_value":"E7MDBD6NPGVTQCC4","created_at":"2026-05-18T12:29:19.899920+00:00"},{"alias_kind":"pith_short_8","alias_value":"E7MDBD6N","created_at":"2026-05-18T12:29:19.899920+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/E7MDBD6NPGVTQCC4WIZ4753LO6","json":"https://pith.science/pith/E7MDBD6NPGVTQCC4WIZ4753LO6.json","graph_json":"https://pith.science/api/pith-number/E7MDBD6NPGVTQCC4WIZ4753LO6/graph.json","events_json":"https://pith.science/api/pith-number/E7MDBD6NPGVTQCC4WIZ4753LO6/events.json","paper":"https://pith.science/paper/E7MDBD6N"},"agent_actions":{"view_html":"https://pith.science/pith/E7MDBD6NPGVTQCC4WIZ4753LO6","download_json":"https://pith.science/pith/E7MDBD6NPGVTQCC4WIZ4753LO6.json","view_paper":"https://pith.science/paper/E7MDBD6N","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1510.07650&json=true","fetch_graph":"https://pith.science/api/pith-number/E7MDBD6NPGVTQCC4WIZ4753LO6/graph.json","fetch_events":"https://pith.science/api/pith-number/E7MDBD6NPGVTQCC4WIZ4753LO6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/E7MDBD6NPGVTQCC4WIZ4753LO6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/E7MDBD6NPGVTQCC4WIZ4753LO6/action/storage_attestation","attest_author":"https://pith.science/pith/E7MDBD6NPGVTQCC4WIZ4753LO6/action/author_attestation","sign_citation":"https://pith.science/pith/E7MDBD6NPGVTQCC4WIZ4753LO6/action/citation_signature","submit_replication":"https://pith.science/pith/E7MDBD6NPGVTQCC4WIZ4753LO6/action/replication_record"}},"created_at":"2026-05-18T01:17:18.481596+00:00","updated_at":"2026-05-18T01:17:18.481596+00:00"}