{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:SQCLTM6UQKJMAQBFRVXXNBOVEA","short_pith_number":"pith:SQCLTM6U","schema_version":"1.0","canonical_sha256":"9404b9b3d48292c040258d6f7685d5200d831902eeecef068cef51dee678a316","source":{"kind":"arxiv","id":"1801.01419","version":1},"attestation_state":"computed","paper":{"title":"Spin-orbital model of stoichiometric LaMnO$_3$ with tetragonal distortions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"Andrzej M. Ole\\'s, Mateusz Snamina","submitted_at":"2018-01-04T16:07:47Z","abstract_excerpt":"The model developed for LaMnO$_3$ addresses the spin-orbital order by superexchange and Jahn-Teller orbital interactions in the cubic (perovskite) symmetry up to now whereas real crystal structure is strongly deformed. We identify and explain three \\textit{a priori} important physical effects arising from tetragonal deformation: (i) the splitting of $e_g$ orbitals $\\propto E_z$, (ii) the directional renormalization of $d-p$ hybridization $t_{pd}$, and (iii) the directional renormalization of charge excitation energies. Using the example of LaMnO$_3$ crystal we evaluate their magnitude. It is f"},"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":"1801.01419","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-01-04T16:07:47Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"3cb3823bfb134e94a09feb22ca3a685860c9b64ea1831b863b1e8698b0ec457a","abstract_canon_sha256":"03fcf2e797eae92327747aa2513de581e66c1f81d88a0bbad512a1396f526b44"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:20:04.879152Z","signature_b64":"VncP8X33hTT+VmbaCIUgTrz9+TDEMQXG0+miqnK+vytRNHz+rntozB5fwAuXMbMMIFVIUBO0XMbqcYGsihuBAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9404b9b3d48292c040258d6f7685d5200d831902eeecef068cef51dee678a316","last_reissued_at":"2026-05-18T00:20:04.878425Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:20:04.878425Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Spin-orbital model of stoichiometric LaMnO$_3$ with tetragonal distortions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"Andrzej M. Ole\\'s, Mateusz Snamina","submitted_at":"2018-01-04T16:07:47Z","abstract_excerpt":"The model developed for LaMnO$_3$ addresses the spin-orbital order by superexchange and Jahn-Teller orbital interactions in the cubic (perovskite) symmetry up to now whereas real crystal structure is strongly deformed. We identify and explain three \\textit{a priori} important physical effects arising from tetragonal deformation: (i) the splitting of $e_g$ orbitals $\\propto E_z$, (ii) the directional renormalization of $d-p$ hybridization $t_{pd}$, and (iii) the directional renormalization of charge excitation energies. Using the example of LaMnO$_3$ crystal we evaluate their magnitude. It is f"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.01419","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":"1801.01419","created_at":"2026-05-18T00:20:04.878536+00:00"},{"alias_kind":"arxiv_version","alias_value":"1801.01419v1","created_at":"2026-05-18T00:20:04.878536+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.01419","created_at":"2026-05-18T00:20:04.878536+00:00"},{"alias_kind":"pith_short_12","alias_value":"SQCLTM6UQKJM","created_at":"2026-05-18T12:32:53.628368+00:00"},{"alias_kind":"pith_short_16","alias_value":"SQCLTM6UQKJMAQBF","created_at":"2026-05-18T12:32:53.628368+00:00"},{"alias_kind":"pith_short_8","alias_value":"SQCLTM6U","created_at":"2026-05-18T12:32:53.628368+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/SQCLTM6UQKJMAQBFRVXXNBOVEA","json":"https://pith.science/pith/SQCLTM6UQKJMAQBFRVXXNBOVEA.json","graph_json":"https://pith.science/api/pith-number/SQCLTM6UQKJMAQBFRVXXNBOVEA/graph.json","events_json":"https://pith.science/api/pith-number/SQCLTM6UQKJMAQBFRVXXNBOVEA/events.json","paper":"https://pith.science/paper/SQCLTM6U"},"agent_actions":{"view_html":"https://pith.science/pith/SQCLTM6UQKJMAQBFRVXXNBOVEA","download_json":"https://pith.science/pith/SQCLTM6UQKJMAQBFRVXXNBOVEA.json","view_paper":"https://pith.science/paper/SQCLTM6U","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1801.01419&json=true","fetch_graph":"https://pith.science/api/pith-number/SQCLTM6UQKJMAQBFRVXXNBOVEA/graph.json","fetch_events":"https://pith.science/api/pith-number/SQCLTM6UQKJMAQBFRVXXNBOVEA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SQCLTM6UQKJMAQBFRVXXNBOVEA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SQCLTM6UQKJMAQBFRVXXNBOVEA/action/storage_attestation","attest_author":"https://pith.science/pith/SQCLTM6UQKJMAQBFRVXXNBOVEA/action/author_attestation","sign_citation":"https://pith.science/pith/SQCLTM6UQKJMAQBFRVXXNBOVEA/action/citation_signature","submit_replication":"https://pith.science/pith/SQCLTM6UQKJMAQBFRVXXNBOVEA/action/replication_record"}},"created_at":"2026-05-18T00:20:04.878536+00:00","updated_at":"2026-05-18T00:20:04.878536+00:00"}