{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:6LJCH44VKNTOUAHJ6HNBASYYE2","short_pith_number":"pith:6LJCH44V","canonical_record":{"source":{"id":"1311.4263","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-11-18T04:38:08Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"c97907656e0aac7ea614ecd5d79e0fb1b5000b763caa68812d007022b4db6845","abstract_canon_sha256":"3908a22990dbe2fcc3168844cb35be6403ad30961a0b6351a50f5a40ccdc8c30"},"schema_version":"1.0"},"canonical_sha256":"f2d223f3955366ea00e9f1da104b18268153f5945c2714d1056dacc4d4052a03","source":{"kind":"arxiv","id":"1311.4263","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1311.4263","created_at":"2026-05-18T02:57:26Z"},{"alias_kind":"arxiv_version","alias_value":"1311.4263v1","created_at":"2026-05-18T02:57:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.4263","created_at":"2026-05-18T02:57:26Z"},{"alias_kind":"pith_short_12","alias_value":"6LJCH44VKNTO","created_at":"2026-05-18T12:27:36Z"},{"alias_kind":"pith_short_16","alias_value":"6LJCH44VKNTOUAHJ","created_at":"2026-05-18T12:27:36Z"},{"alias_kind":"pith_short_8","alias_value":"6LJCH44V","created_at":"2026-05-18T12:27:36Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:6LJCH44VKNTOUAHJ6HNBASYYE2","target":"record","payload":{"canonical_record":{"source":{"id":"1311.4263","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-11-18T04:38:08Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"c97907656e0aac7ea614ecd5d79e0fb1b5000b763caa68812d007022b4db6845","abstract_canon_sha256":"3908a22990dbe2fcc3168844cb35be6403ad30961a0b6351a50f5a40ccdc8c30"},"schema_version":"1.0"},"canonical_sha256":"f2d223f3955366ea00e9f1da104b18268153f5945c2714d1056dacc4d4052a03","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:57:26.285790Z","signature_b64":"2tZVqCU7jnGATNmbosCbl0DxYNEoZJBl319zIhra1sWh51yOj91R60zHXvKFKBL4C3HqaSHFNyEs0PYmFYQlCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f2d223f3955366ea00e9f1da104b18268153f5945c2714d1056dacc4d4052a03","last_reissued_at":"2026-05-18T02:57:26.285188Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:57:26.285188Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1311.4263","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":"2026-05-18T02:57:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YK5UewfhmtigU3kh5aQU2jqH/cdOgt+/LMlXDATjBIhZ/ZkLy3lvn3odx8uzyN8Rnib8FgzSnkcYstZg97WEAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T04:29:04.928883Z"},"content_sha256":"4edfb78901b76219f3cfa5bd9c6d0fd5d41f9bb5cc83565f329aa3b73ee6b80b","schema_version":"1.0","event_id":"sha256:4edfb78901b76219f3cfa5bd9c6d0fd5d41f9bb5cc83565f329aa3b73ee6b80b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:6LJCH44VKNTOUAHJ6HNBASYYE2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Orbital magnetization of insulating perovskite transition-metal oxides with the net ferromagnetic moment in the ground state","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"I. V. Solovyev, S. A. Nikolaev","submitted_at":"2013-11-18T04:38:08Z","abstract_excerpt":"Modern theory of the orbital magnetization is applied to the series of insulating perovskite transition metal oxides (orthorhombic YTiO$_3$, LaMnO$_3$, and YVO$_3$, as well as monoclinic YVO$_3$), carrying a net ferromagnetic (FM) moment in the ground state. For these purposes, we use an effective Hubbard-type model, derived from the first-principles electronic-structure calculations and describing the behavior of magnetically active states near the Fermi level. The solution of this model in the mean-field Hartree-Fock approximation with the relativistic spin-orbit coupling typically gives us "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.4263","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":"2026-05-18T02:57:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tfJC2QneS1nf8JH8IdPVNlurIhTeSRLI1DFwqdhHIYaLZEJTDKXMnkXz/h4kxQtche5IS9I5ZDiq1Xo3A5xbDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T04:29:04.929223Z"},"content_sha256":"e35315b209b4b235836764614514f0799de16cb46bfb99eaf12052cd15d44549","schema_version":"1.0","event_id":"sha256:e35315b209b4b235836764614514f0799de16cb46bfb99eaf12052cd15d44549"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6LJCH44VKNTOUAHJ6HNBASYYE2/bundle.json","state_url":"https://pith.science/pith/6LJCH44VKNTOUAHJ6HNBASYYE2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6LJCH44VKNTOUAHJ6HNBASYYE2/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":"2026-06-01T04:29:04Z","links":{"resolver":"https://pith.science/pith/6LJCH44VKNTOUAHJ6HNBASYYE2","bundle":"https://pith.science/pith/6LJCH44VKNTOUAHJ6HNBASYYE2/bundle.json","state":"https://pith.science/pith/6LJCH44VKNTOUAHJ6HNBASYYE2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6LJCH44VKNTOUAHJ6HNBASYYE2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:6LJCH44VKNTOUAHJ6HNBASYYE2","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":"3908a22990dbe2fcc3168844cb35be6403ad30961a0b6351a50f5a40ccdc8c30","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-11-18T04:38:08Z","title_canon_sha256":"c97907656e0aac7ea614ecd5d79e0fb1b5000b763caa68812d007022b4db6845"},"schema_version":"1.0","source":{"id":"1311.4263","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1311.4263","created_at":"2026-05-18T02:57:26Z"},{"alias_kind":"arxiv_version","alias_value":"1311.4263v1","created_at":"2026-05-18T02:57:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.4263","created_at":"2026-05-18T02:57:26Z"},{"alias_kind":"pith_short_12","alias_value":"6LJCH44VKNTO","created_at":"2026-05-18T12:27:36Z"},{"alias_kind":"pith_short_16","alias_value":"6LJCH44VKNTOUAHJ","created_at":"2026-05-18T12:27:36Z"},{"alias_kind":"pith_short_8","alias_value":"6LJCH44V","created_at":"2026-05-18T12:27:36Z"}],"graph_snapshots":[{"event_id":"sha256:e35315b209b4b235836764614514f0799de16cb46bfb99eaf12052cd15d44549","target":"graph","created_at":"2026-05-18T02:57:26Z","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":"Modern theory of the orbital magnetization is applied to the series of insulating perovskite transition metal oxides (orthorhombic YTiO$_3$, LaMnO$_3$, and YVO$_3$, as well as monoclinic YVO$_3$), carrying a net ferromagnetic (FM) moment in the ground state. For these purposes, we use an effective Hubbard-type model, derived from the first-principles electronic-structure calculations and describing the behavior of magnetically active states near the Fermi level. The solution of this model in the mean-field Hartree-Fock approximation with the relativistic spin-orbit coupling typically gives us ","authors_text":"I. V. Solovyev, S. A. Nikolaev","cross_cats":["cond-mat.str-el"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-11-18T04:38:08Z","title":"Orbital magnetization of insulating perovskite transition-metal oxides with the net ferromagnetic moment in the ground state"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.4263","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":"sha256:4edfb78901b76219f3cfa5bd9c6d0fd5d41f9bb5cc83565f329aa3b73ee6b80b","target":"record","created_at":"2026-05-18T02:57:26Z","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":"3908a22990dbe2fcc3168844cb35be6403ad30961a0b6351a50f5a40ccdc8c30","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-11-18T04:38:08Z","title_canon_sha256":"c97907656e0aac7ea614ecd5d79e0fb1b5000b763caa68812d007022b4db6845"},"schema_version":"1.0","source":{"id":"1311.4263","kind":"arxiv","version":1}},"canonical_sha256":"f2d223f3955366ea00e9f1da104b18268153f5945c2714d1056dacc4d4052a03","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f2d223f3955366ea00e9f1da104b18268153f5945c2714d1056dacc4d4052a03","first_computed_at":"2026-05-18T02:57:26.285188Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:57:26.285188Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2tZVqCU7jnGATNmbosCbl0DxYNEoZJBl319zIhra1sWh51yOj91R60zHXvKFKBL4C3HqaSHFNyEs0PYmFYQlCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:57:26.285790Z","signed_message":"canonical_sha256_bytes"},"source_id":"1311.4263","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4edfb78901b76219f3cfa5bd9c6d0fd5d41f9bb5cc83565f329aa3b73ee6b80b","sha256:e35315b209b4b235836764614514f0799de16cb46bfb99eaf12052cd15d44549"],"state_sha256":"1ff3bec9704f295a260b5928cd2bdf6510d62a630b0a4f40cfb556770ce073ca"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"V0RPl0/W7hdJmEZkYlUdA2mRihvp/dXFIzQvUqz3fOhrH+s9qAqPexYA0Kq+8GFrvxLJnieZHCevEeA77qBMDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T04:29:04.931306Z","bundle_sha256":"28cc842754e2167341daf62f2f999cc413d743453dc891be0ac108237abf17e9"}}