{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:2LPK4MIWRQX4HGNL37TFP7A3VA","short_pith_number":"pith:2LPK4MIW","schema_version":"1.0","canonical_sha256":"d2deae31168c2fc399abdfe657fc1ba80bb95756505d1e304b944d1122feee95","source":{"kind":"arxiv","id":"0704.1460","version":1},"attestation_state":"computed","paper":{"title":"Landau-Lifshitz sigma-models, fermions and the AdS/CFT correspondence","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"B. Stefanski Jr","submitted_at":"2007-04-11T17:18:59Z","abstract_excerpt":"We define Landau-Lifshitz sigma models on general coset space $G/H$, with $H$ a maximal stability sub-group of $G$. These are non-relativistic models that have $G$-valued N\\\"other charges, local $H$ invariance and are classically integrable. Using this definition, we construct the $PSU(2,2|4)/PS(U(2|2)^2)$ Landau-Lifshitz sigma-model. This sigma model describes the thermodynamic limit of the spin-chain Hamiltonian obtained from the complete one-loop dilatation operator of the N=4 super Yang-Mills (SYM) theory. In the second part of the paper, we identify a number of consistent truncations of t"},"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":"0704.1460","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2007-04-11T17:18:59Z","cross_cats_sorted":[],"title_canon_sha256":"4b0dee5cfe1be37a74773dbb85957153110a5fcead291cac85029567038cc302","abstract_canon_sha256":"f5e7aff9848190490b9976da7b19053e456d97a47e24c2871c2cc2553a438593"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:18:37.149119Z","signature_b64":"aPzOSi3cDskc8pq7K4WrcGgaXt3nSRkoReKhvkWYfYAnvMoQTxYvjKgyVqTJjNYMep8c04FPFe/+cShw/hMdCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d2deae31168c2fc399abdfe657fc1ba80bb95756505d1e304b944d1122feee95","last_reissued_at":"2026-07-04T15:18:37.148733Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:18:37.148733Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Landau-Lifshitz sigma-models, fermions and the AdS/CFT correspondence","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"B. Stefanski Jr","submitted_at":"2007-04-11T17:18:59Z","abstract_excerpt":"We define Landau-Lifshitz sigma models on general coset space $G/H$, with $H$ a maximal stability sub-group of $G$. These are non-relativistic models that have $G$-valued N\\\"other charges, local $H$ invariance and are classically integrable. Using this definition, we construct the $PSU(2,2|4)/PS(U(2|2)^2)$ Landau-Lifshitz sigma-model. This sigma model describes the thermodynamic limit of the spin-chain Hamiltonian obtained from the complete one-loop dilatation operator of the N=4 super Yang-Mills (SYM) theory. In the second part of the paper, we identify a number of consistent truncations of t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0704.1460","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/0704.1460/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":"0704.1460","created_at":"2026-07-04T15:18:37.148794+00:00"},{"alias_kind":"arxiv_version","alias_value":"0704.1460v1","created_at":"2026-07-04T15:18:37.148794+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0704.1460","created_at":"2026-07-04T15:18:37.148794+00:00"},{"alias_kind":"pith_short_12","alias_value":"2LPK4MIWRQX4","created_at":"2026-07-04T15:18:37.148794+00:00"},{"alias_kind":"pith_short_16","alias_value":"2LPK4MIWRQX4HGNL","created_at":"2026-07-04T15:18:37.148794+00:00"},{"alias_kind":"pith_short_8","alias_value":"2LPK4MIW","created_at":"2026-07-04T15:18:37.148794+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.13598","citing_title":"An integrable deformed Landau-Lifshitz model with particle production?","ref_index":31,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2LPK4MIWRQX4HGNL37TFP7A3VA","json":"https://pith.science/pith/2LPK4MIWRQX4HGNL37TFP7A3VA.json","graph_json":"https://pith.science/api/pith-number/2LPK4MIWRQX4HGNL37TFP7A3VA/graph.json","events_json":"https://pith.science/api/pith-number/2LPK4MIWRQX4HGNL37TFP7A3VA/events.json","paper":"https://pith.science/paper/2LPK4MIW"},"agent_actions":{"view_html":"https://pith.science/pith/2LPK4MIWRQX4HGNL37TFP7A3VA","download_json":"https://pith.science/pith/2LPK4MIWRQX4HGNL37TFP7A3VA.json","view_paper":"https://pith.science/paper/2LPK4MIW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0704.1460&json=true","fetch_graph":"https://pith.science/api/pith-number/2LPK4MIWRQX4HGNL37TFP7A3VA/graph.json","fetch_events":"https://pith.science/api/pith-number/2LPK4MIWRQX4HGNL37TFP7A3VA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2LPK4MIWRQX4HGNL37TFP7A3VA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2LPK4MIWRQX4HGNL37TFP7A3VA/action/storage_attestation","attest_author":"https://pith.science/pith/2LPK4MIWRQX4HGNL37TFP7A3VA/action/author_attestation","sign_citation":"https://pith.science/pith/2LPK4MIWRQX4HGNL37TFP7A3VA/action/citation_signature","submit_replication":"https://pith.science/pith/2LPK4MIWRQX4HGNL37TFP7A3VA/action/replication_record"}},"created_at":"2026-07-04T15:18:37.148794+00:00","updated_at":"2026-07-04T15:18:37.148794+00:00"}