{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:RHSS4S2GMGPFS3GMQEZTGFTIUT","short_pith_number":"pith:RHSS4S2G","schema_version":"1.0","canonical_sha256":"89e52e4b46619e596ccc8133331668a4e75bed1fa72ff47488fa31ac29867ab5","source":{"kind":"arxiv","id":"1511.08767","version":1},"attestation_state":"computed","paper":{"title":"Scale invariant behavior in a large N matrix model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-lat","authors_text":"Herbert Neuberger, Rajamani Narayanan","submitted_at":"2015-11-27T18:45:20Z","abstract_excerpt":"Eigenvalue distributions of properly regularized Wilson loop operators are used to study the transition from ultra-violet (UV) behavior to infra-red (IR) behavior in gauge theories coupled to matter that potentially have an IR fixed point (FP). We numerically demonstrate emergence of scale invariance in a matrix model that describes $SU(N)$ gauge theory coupled to two flavors of massless adjoint fermions in the large $N$ limit. The eigenvalue distribution of Wilson loops of varying sizes cannot be described by a universal lattice beta-function connecting the UV to the IR."},"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":"1511.08767","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-11-27T18:45:20Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"f652e3d3067309553f9bcc71483e33cd6a1a74ae6f08fe8625b48bf24f354ffc","abstract_canon_sha256":"707eac4ae50fea795bc91a47a91ceb23bbbc0fe6ca113903878bf886e0230f8c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:21:51.485228Z","signature_b64":"NouLS0HqNeEGEGr258xUY80hQ2Degj7Nm4EYmvGXbbktK8YplcjODeNv3/ROGxFK8jUbsqaOi62wU7o9p98iBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"89e52e4b46619e596ccc8133331668a4e75bed1fa72ff47488fa31ac29867ab5","last_reissued_at":"2026-05-18T01:21:51.484579Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:21:51.484579Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Scale invariant behavior in a large N matrix model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-lat","authors_text":"Herbert Neuberger, Rajamani Narayanan","submitted_at":"2015-11-27T18:45:20Z","abstract_excerpt":"Eigenvalue distributions of properly regularized Wilson loop operators are used to study the transition from ultra-violet (UV) behavior to infra-red (IR) behavior in gauge theories coupled to matter that potentially have an IR fixed point (FP). We numerically demonstrate emergence of scale invariance in a matrix model that describes $SU(N)$ gauge theory coupled to two flavors of massless adjoint fermions in the large $N$ limit. The eigenvalue distribution of Wilson loops of varying sizes cannot be described by a universal lattice beta-function connecting the UV to the IR."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.08767","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":""},"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":"1511.08767","created_at":"2026-05-18T01:21:51.484672+00:00"},{"alias_kind":"arxiv_version","alias_value":"1511.08767v1","created_at":"2026-05-18T01:21:51.484672+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.08767","created_at":"2026-05-18T01:21:51.484672+00:00"},{"alias_kind":"pith_short_12","alias_value":"RHSS4S2GMGPF","created_at":"2026-05-18T12:29:39.896362+00:00"},{"alias_kind":"pith_short_16","alias_value":"RHSS4S2GMGPFS3GM","created_at":"2026-05-18T12:29:39.896362+00:00"},{"alias_kind":"pith_short_8","alias_value":"RHSS4S2G","created_at":"2026-05-18T12:29:39.896362+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/RHSS4S2GMGPFS3GMQEZTGFTIUT","json":"https://pith.science/pith/RHSS4S2GMGPFS3GMQEZTGFTIUT.json","graph_json":"https://pith.science/api/pith-number/RHSS4S2GMGPFS3GMQEZTGFTIUT/graph.json","events_json":"https://pith.science/api/pith-number/RHSS4S2GMGPFS3GMQEZTGFTIUT/events.json","paper":"https://pith.science/paper/RHSS4S2G"},"agent_actions":{"view_html":"https://pith.science/pith/RHSS4S2GMGPFS3GMQEZTGFTIUT","download_json":"https://pith.science/pith/RHSS4S2GMGPFS3GMQEZTGFTIUT.json","view_paper":"https://pith.science/paper/RHSS4S2G","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1511.08767&json=true","fetch_graph":"https://pith.science/api/pith-number/RHSS4S2GMGPFS3GMQEZTGFTIUT/graph.json","fetch_events":"https://pith.science/api/pith-number/RHSS4S2GMGPFS3GMQEZTGFTIUT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RHSS4S2GMGPFS3GMQEZTGFTIUT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RHSS4S2GMGPFS3GMQEZTGFTIUT/action/storage_attestation","attest_author":"https://pith.science/pith/RHSS4S2GMGPFS3GMQEZTGFTIUT/action/author_attestation","sign_citation":"https://pith.science/pith/RHSS4S2GMGPFS3GMQEZTGFTIUT/action/citation_signature","submit_replication":"https://pith.science/pith/RHSS4S2GMGPFS3GMQEZTGFTIUT/action/replication_record"}},"created_at":"2026-05-18T01:21:51.484672+00:00","updated_at":"2026-05-18T01:21:51.484672+00:00"}