{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:O42QPNNFQMLN4XXJGKO5JKAGWX","short_pith_number":"pith:O42QPNNF","schema_version":"1.0","canonical_sha256":"773507b5a58316de5ee9329dd4a806b5d38bc55600ba5bf87ae7dc3238cb2b07","source":{"kind":"arxiv","id":"1104.4224","version":1},"attestation_state":"computed","paper":{"title":"Unified quantitative model for magnetic and electronic spectra of the undoped cuprates","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"B. Dalla Piazza, H. Berger, H. M. Ronnow, M. Grioni, M. Guarise, M. Mourigal, T. Schmitt","submitted_at":"2011-04-21T10:23:25Z","abstract_excerpt":"Using low-energy projection of the one-band t-t'-t\"-Hubbard model we derive an effective spin-Hamiltonian and its spin-wave expansion to order 1/S. We fit the spin-wave dispersion of several parent compounds to the high-temperature superconducting cuprates: La2CuO4, Sr2CuO2Cl2 and Bi2Sr2YCu2O8. Our accurate quantitative determination of the one-band Hubbard model parameters allows prediction and comparison to experimental results of measurable quantities such as staggered moment, double occupancy density, spin-wave velocity and bimagnon excitation spectrum and density of states, which is discu"},"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":"1104.4224","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-04-21T10:23:25Z","cross_cats_sorted":[],"title_canon_sha256":"34f2a339fd3b95e1790bc145106e86f8699914707b419ec555244ee21329ec3c","abstract_canon_sha256":"4ffa83f0a43bbcdd1294c526bdfd1445ae7807029fb0de12b5d9eb4b82591c7b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:05:45.105030Z","signature_b64":"6hPCeX3RwpbmTvtaT5bolrajb6t0mFwep4w6XA1GWwuKxtaxutV5gtm55mDjxhB+KgK4aJrffW6OPrJUwZDSAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"773507b5a58316de5ee9329dd4a806b5d38bc55600ba5bf87ae7dc3238cb2b07","last_reissued_at":"2026-05-18T03:05:45.104576Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:05:45.104576Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Unified quantitative model for magnetic and electronic spectra of the undoped cuprates","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"B. Dalla Piazza, H. Berger, H. M. Ronnow, M. Grioni, M. Guarise, M. Mourigal, T. Schmitt","submitted_at":"2011-04-21T10:23:25Z","abstract_excerpt":"Using low-energy projection of the one-band t-t'-t\"-Hubbard model we derive an effective spin-Hamiltonian and its spin-wave expansion to order 1/S. We fit the spin-wave dispersion of several parent compounds to the high-temperature superconducting cuprates: La2CuO4, Sr2CuO2Cl2 and Bi2Sr2YCu2O8. Our accurate quantitative determination of the one-band Hubbard model parameters allows prediction and comparison to experimental results of measurable quantities such as staggered moment, double occupancy density, spin-wave velocity and bimagnon excitation spectrum and density of states, which is discu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1104.4224","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":"1104.4224","created_at":"2026-05-18T03:05:45.104643+00:00"},{"alias_kind":"arxiv_version","alias_value":"1104.4224v1","created_at":"2026-05-18T03:05:45.104643+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1104.4224","created_at":"2026-05-18T03:05:45.104643+00:00"},{"alias_kind":"pith_short_12","alias_value":"O42QPNNFQMLN","created_at":"2026-05-18T12:26:37.096874+00:00"},{"alias_kind":"pith_short_16","alias_value":"O42QPNNFQMLN4XXJ","created_at":"2026-05-18T12:26:37.096874+00:00"},{"alias_kind":"pith_short_8","alias_value":"O42QPNNF","created_at":"2026-05-18T12:26:37.096874+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/O42QPNNFQMLN4XXJGKO5JKAGWX","json":"https://pith.science/pith/O42QPNNFQMLN4XXJGKO5JKAGWX.json","graph_json":"https://pith.science/api/pith-number/O42QPNNFQMLN4XXJGKO5JKAGWX/graph.json","events_json":"https://pith.science/api/pith-number/O42QPNNFQMLN4XXJGKO5JKAGWX/events.json","paper":"https://pith.science/paper/O42QPNNF"},"agent_actions":{"view_html":"https://pith.science/pith/O42QPNNFQMLN4XXJGKO5JKAGWX","download_json":"https://pith.science/pith/O42QPNNFQMLN4XXJGKO5JKAGWX.json","view_paper":"https://pith.science/paper/O42QPNNF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1104.4224&json=true","fetch_graph":"https://pith.science/api/pith-number/O42QPNNFQMLN4XXJGKO5JKAGWX/graph.json","fetch_events":"https://pith.science/api/pith-number/O42QPNNFQMLN4XXJGKO5JKAGWX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/O42QPNNFQMLN4XXJGKO5JKAGWX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/O42QPNNFQMLN4XXJGKO5JKAGWX/action/storage_attestation","attest_author":"https://pith.science/pith/O42QPNNFQMLN4XXJGKO5JKAGWX/action/author_attestation","sign_citation":"https://pith.science/pith/O42QPNNFQMLN4XXJGKO5JKAGWX/action/citation_signature","submit_replication":"https://pith.science/pith/O42QPNNFQMLN4XXJGKO5JKAGWX/action/replication_record"}},"created_at":"2026-05-18T03:05:45.104643+00:00","updated_at":"2026-05-18T03:05:45.104643+00:00"}