{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:SQCLTM6UQKJMAQBFRVXXNBOVEA","short_pith_number":"pith:SQCLTM6U","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"},"canonical_sha256":"9404b9b3d48292c040258d6f7685d5200d831902eeecef068cef51dee678a316","source":{"kind":"arxiv","id":"1801.01419","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.01419","created_at":"2026-05-18T00:20:04Z"},{"alias_kind":"arxiv_version","alias_value":"1801.01419v1","created_at":"2026-05-18T00:20:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.01419","created_at":"2026-05-18T00:20:04Z"},{"alias_kind":"pith_short_12","alias_value":"SQCLTM6UQKJM","created_at":"2026-05-18T12:32:53Z"},{"alias_kind":"pith_short_16","alias_value":"SQCLTM6UQKJMAQBF","created_at":"2026-05-18T12:32:53Z"},{"alias_kind":"pith_short_8","alias_value":"SQCLTM6U","created_at":"2026-05-18T12:32:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:SQCLTM6UQKJMAQBFRVXXNBOVEA","target":"record","payload":{"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"},"canonical_sha256":"9404b9b3d48292c040258d6f7685d5200d831902eeecef068cef51dee678a316","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"},"source_kind":"arxiv","source_id":"1801.01419","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:20:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nKrGr/ebDRyg8wUQlz2cbWhKSuu3sbuZDWL9UitH5KwpBqUloqk6JXwjNNcI7KdoLNI9WoLe/X2sK091qLUdDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-23T15:39:19.211068Z"},"content_sha256":"4b714194ad1dfc94c754729eb88c70e3909845d9ee0db7e71ba36060749b53f8","schema_version":"1.0","event_id":"sha256:4b714194ad1dfc94c754729eb88c70e3909845d9ee0db7e71ba36060749b53f8"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:SQCLTM6UQKJMAQBFRVXXNBOVEA","target":"graph","payload":{"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:20:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rm5MlDHLESk1IJ0txAdq1jN+LXm17XyRprpaY+NNXQvUYAJ2CjWIPjtm7RBxnQfkbLbtaZSYmBeUsX3GTqxQCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-23T15:39:19.211432Z"},"content_sha256":"1fd1278f01035fc884cadd829aed724b5edf8039a1ac73aee6a6798c6a41d04c","schema_version":"1.0","event_id":"sha256:1fd1278f01035fc884cadd829aed724b5edf8039a1ac73aee6a6798c6a41d04c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SQCLTM6UQKJMAQBFRVXXNBOVEA/bundle.json","state_url":"https://pith.science/pith/SQCLTM6UQKJMAQBFRVXXNBOVEA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SQCLTM6UQKJMAQBFRVXXNBOVEA/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-23T15:39:19Z","links":{"resolver":"https://pith.science/pith/SQCLTM6UQKJMAQBFRVXXNBOVEA","bundle":"https://pith.science/pith/SQCLTM6UQKJMAQBFRVXXNBOVEA/bundle.json","state":"https://pith.science/pith/SQCLTM6UQKJMAQBFRVXXNBOVEA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SQCLTM6UQKJMAQBFRVXXNBOVEA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:SQCLTM6UQKJMAQBFRVXXNBOVEA","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":"03fcf2e797eae92327747aa2513de581e66c1f81d88a0bbad512a1396f526b44","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-01-04T16:07:47Z","title_canon_sha256":"3cb3823bfb134e94a09feb22ca3a685860c9b64ea1831b863b1e8698b0ec457a"},"schema_version":"1.0","source":{"id":"1801.01419","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.01419","created_at":"2026-05-18T00:20:04Z"},{"alias_kind":"arxiv_version","alias_value":"1801.01419v1","created_at":"2026-05-18T00:20:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.01419","created_at":"2026-05-18T00:20:04Z"},{"alias_kind":"pith_short_12","alias_value":"SQCLTM6UQKJM","created_at":"2026-05-18T12:32:53Z"},{"alias_kind":"pith_short_16","alias_value":"SQCLTM6UQKJMAQBF","created_at":"2026-05-18T12:32:53Z"},{"alias_kind":"pith_short_8","alias_value":"SQCLTM6U","created_at":"2026-05-18T12:32:53Z"}],"graph_snapshots":[{"event_id":"sha256:1fd1278f01035fc884cadd829aed724b5edf8039a1ac73aee6a6798c6a41d04c","target":"graph","created_at":"2026-05-18T00:20:04Z","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"},"paper":{"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","authors_text":"Andrzej M. Ole\\'s, Mateusz Snamina","cross_cats":["cond-mat.mtrl-sci"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-01-04T16:07:47Z","title":"Spin-orbital model of stoichiometric LaMnO$_3$ with tetragonal distortions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.01419","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":"sha256:4b714194ad1dfc94c754729eb88c70e3909845d9ee0db7e71ba36060749b53f8","target":"record","created_at":"2026-05-18T00:20:04Z","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":"03fcf2e797eae92327747aa2513de581e66c1f81d88a0bbad512a1396f526b44","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-01-04T16:07:47Z","title_canon_sha256":"3cb3823bfb134e94a09feb22ca3a685860c9b64ea1831b863b1e8698b0ec457a"},"schema_version":"1.0","source":{"id":"1801.01419","kind":"arxiv","version":1}},"canonical_sha256":"9404b9b3d48292c040258d6f7685d5200d831902eeecef068cef51dee678a316","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9404b9b3d48292c040258d6f7685d5200d831902eeecef068cef51dee678a316","first_computed_at":"2026-05-18T00:20:04.878425Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:20:04.878425Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"VncP8X33hTT+VmbaCIUgTrz9+TDEMQXG0+miqnK+vytRNHz+rntozB5fwAuXMbMMIFVIUBO0XMbqcYGsihuBAw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:20:04.879152Z","signed_message":"canonical_sha256_bytes"},"source_id":"1801.01419","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4b714194ad1dfc94c754729eb88c70e3909845d9ee0db7e71ba36060749b53f8","sha256:1fd1278f01035fc884cadd829aed724b5edf8039a1ac73aee6a6798c6a41d04c"],"state_sha256":"63402f7a4907c9273b527aee0ef24668d2ed2c9748502f9fd2bda15d1a68a6a2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ogYd2VysO3FrGy9ahzKd4p7uLwwWpzGH0esz73E+WBosoX1Wr6w0nHl5IMaMngJl6TIcdY7pIe7uAC5ENjs4CA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-23T15:39:19.213366Z","bundle_sha256":"d571b2c6280fc383b0dd6070bb636d62568bd703983b1cfdf63e366e030a65db"}}