{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:KDOFOMMI6S5MAER2UOVISGV44Q","short_pith_number":"pith:KDOFOMMI","schema_version":"1.0","canonical_sha256":"50dc573188f4bac0123aa3aa891abce41f2ff4e99a36e05a73b9c24df570d15a","source":{"kind":"arxiv","id":"1801.02822","version":1},"attestation_state":"computed","paper":{"title":"Anomalous dimensions from boson lattice models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Augustine Larweh Mahu, Robert de Mello Koch, Shaun de Carvalho","submitted_at":"2018-01-09T07:03:26Z","abstract_excerpt":"Operators dual to strings attached to giant graviton branes in AdS$_5\\times$S$^5$ can be described rather explicitly in the dual ${\\cal N} = 4$ super Yang-Mills theory. They have a bare dimension of order $N$ so that for these operators the large $N$ limit and the planar limit are distinct: summing only the planar diagrams will not capture the large $N$ dynamics. Focusing on the one-loop $SU(3)$ sector of the theory, we consider operators that are a small deformation of a ${1\\over 2}-$BPS multi-giant graviton state. The diagonalization of the dilatation operator at one loop has been carried ou"},"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":"1801.02822","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-01-09T07:03:26Z","cross_cats_sorted":[],"title_canon_sha256":"a58e22cc48e38d1979296434bbec214cc3fe80e825748d2935e44ddcb2ef10a5","abstract_canon_sha256":"8a33df8f2e7d3e06ca8f51fefb15bf3030534dd2db15e53b23e3349f2f8b7fa7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:12:53.567971Z","signature_b64":"Uy4qF1QmivgK72aJUJFVK4ri1iJy6Sp4Vz7Ao1ncfJxijSCvfFvt8qHeHV1oSeeRpIlwimxZneEjdyZi9OxuCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"50dc573188f4bac0123aa3aa891abce41f2ff4e99a36e05a73b9c24df570d15a","last_reissued_at":"2026-05-18T00:12:53.567284Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:12:53.567284Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anomalous dimensions from boson lattice models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Augustine Larweh Mahu, Robert de Mello Koch, Shaun de Carvalho","submitted_at":"2018-01-09T07:03:26Z","abstract_excerpt":"Operators dual to strings attached to giant graviton branes in AdS$_5\\times$S$^5$ can be described rather explicitly in the dual ${\\cal N} = 4$ super Yang-Mills theory. They have a bare dimension of order $N$ so that for these operators the large $N$ limit and the planar limit are distinct: summing only the planar diagrams will not capture the large $N$ dynamics. Focusing on the one-loop $SU(3)$ sector of the theory, we consider operators that are a small deformation of a ${1\\over 2}-$BPS multi-giant graviton state. The diagonalization of the dilatation operator at one loop has been carried ou"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.02822","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":"1801.02822","created_at":"2026-05-18T00:12:53.567400+00:00"},{"alias_kind":"arxiv_version","alias_value":"1801.02822v1","created_at":"2026-05-18T00:12:53.567400+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.02822","created_at":"2026-05-18T00:12:53.567400+00:00"},{"alias_kind":"pith_short_12","alias_value":"KDOFOMMI6S5M","created_at":"2026-05-18T12:32:33.847187+00:00"},{"alias_kind":"pith_short_16","alias_value":"KDOFOMMI6S5MAER2","created_at":"2026-05-18T12:32:33.847187+00:00"},{"alias_kind":"pith_short_8","alias_value":"KDOFOMMI","created_at":"2026-05-18T12:32:33.847187+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/KDOFOMMI6S5MAER2UOVISGV44Q","json":"https://pith.science/pith/KDOFOMMI6S5MAER2UOVISGV44Q.json","graph_json":"https://pith.science/api/pith-number/KDOFOMMI6S5MAER2UOVISGV44Q/graph.json","events_json":"https://pith.science/api/pith-number/KDOFOMMI6S5MAER2UOVISGV44Q/events.json","paper":"https://pith.science/paper/KDOFOMMI"},"agent_actions":{"view_html":"https://pith.science/pith/KDOFOMMI6S5MAER2UOVISGV44Q","download_json":"https://pith.science/pith/KDOFOMMI6S5MAER2UOVISGV44Q.json","view_paper":"https://pith.science/paper/KDOFOMMI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1801.02822&json=true","fetch_graph":"https://pith.science/api/pith-number/KDOFOMMI6S5MAER2UOVISGV44Q/graph.json","fetch_events":"https://pith.science/api/pith-number/KDOFOMMI6S5MAER2UOVISGV44Q/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KDOFOMMI6S5MAER2UOVISGV44Q/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KDOFOMMI6S5MAER2UOVISGV44Q/action/storage_attestation","attest_author":"https://pith.science/pith/KDOFOMMI6S5MAER2UOVISGV44Q/action/author_attestation","sign_citation":"https://pith.science/pith/KDOFOMMI6S5MAER2UOVISGV44Q/action/citation_signature","submit_replication":"https://pith.science/pith/KDOFOMMI6S5MAER2UOVISGV44Q/action/replication_record"}},"created_at":"2026-05-18T00:12:53.567400+00:00","updated_at":"2026-05-18T00:12:53.567400+00:00"}