{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:PGS4VC7JNNZHBXYYUZP27OZB56","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"7ab38b89c126ea8509548e360340e83b602c2bcc0a03db60d5d9edd1281fdd36","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2022-02-08T16:18:50Z","title_canon_sha256":"459de82f4fb7c6f394b8b5521d8845929705a230bbcc3de458adeb7f0b1b4363"},"schema_version":"1.0","source":{"id":"2202.03970","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2202.03970","created_at":"2026-07-05T03:55:22Z"},{"alias_kind":"arxiv_version","alias_value":"2202.03970v1","created_at":"2026-07-05T03:55:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2202.03970","created_at":"2026-07-05T03:55:22Z"},{"alias_kind":"pith_short_12","alias_value":"PGS4VC7JNNZH","created_at":"2026-07-05T03:55:22Z"},{"alias_kind":"pith_short_16","alias_value":"PGS4VC7JNNZHBXYY","created_at":"2026-07-05T03:55:22Z"},{"alias_kind":"pith_short_8","alias_value":"PGS4VC7J","created_at":"2026-07-05T03:55:22Z"}],"graph_snapshots":[{"event_id":"sha256:79677f26e8539d2dce101235dbd0905dc342dc5a4aad528c496cc62fbe2b189e","target":"graph","created_at":"2026-07-05T03:55:22Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2202.03970/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In the holographic approach to cosmology, cosmological observables are described in terms of correlators of a three-dimensional boundary quantum field theory. As a concrete model, we study the $3D$ massless $SU(N)$ scalar matrix field theory with a $\\phi^4$ interaction. On the lattice, the energy-momentum tensor (EMT) in this theory can mix with the operator $\\phi^2$. We utilize the Wilson Flow to renormalize the EMT on the lattice, and present numerical results for the mixing coefficient for $N = 2$. Obtaining the renormalized EMT will allow us to make predictions for the CMB power spectra in","authors_text":"Andreas J\\\"uttner, Antonin Portelli, Ben Kitching-Morley, Elizabeth Dobson, Henrique Bergallo Rocha, Joseph K. L. Lee, Kostas Skenderis, Luigi Del Debbio, Valentin Nourry","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2022-02-08T16:18:50Z","title":"Renormalization of the $3D$ $SU(N)$ scalar energy-momentum tensor using the Wilson flow"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2202.03970","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:be5950191901597ed9a3ee33c7636a9b3d9ad693eb5fff2ae8edafb8a25ae972","target":"record","created_at":"2026-07-05T03:55:22Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"7ab38b89c126ea8509548e360340e83b602c2bcc0a03db60d5d9edd1281fdd36","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2022-02-08T16:18:50Z","title_canon_sha256":"459de82f4fb7c6f394b8b5521d8845929705a230bbcc3de458adeb7f0b1b4363"},"schema_version":"1.0","source":{"id":"2202.03970","kind":"arxiv","version":1}},"canonical_sha256":"79a5ca8be96b7270df18a65fafbb21efa69c41a5d9fecad0fc822e17bd5d04e7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"79a5ca8be96b7270df18a65fafbb21efa69c41a5d9fecad0fc822e17bd5d04e7","first_computed_at":"2026-07-05T03:55:22.245018Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T03:55:22.245018Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"sZGQAED+hPFBpXH9JlJb8TEw+4+1SFn7L7bzfhojMVuJ9yyT0YutVN9P9bajk1q2fifLRM6qx73JVirwzqw/Bw==","signature_status":"signed_v1","signed_at":"2026-07-05T03:55:22.245539Z","signed_message":"canonical_sha256_bytes"},"source_id":"2202.03970","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:be5950191901597ed9a3ee33c7636a9b3d9ad693eb5fff2ae8edafb8a25ae972","sha256:79677f26e8539d2dce101235dbd0905dc342dc5a4aad528c496cc62fbe2b189e"],"state_sha256":"b0a104b0510e58e123781827bee26a875b3ed24dcb84f49e0172c3dfa44c9972"}