{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1998:KMICLCPCRV56LPTVPQ5QKVN5AS","short_pith_number":"pith:KMICLCPC","canonical_record":{"source":{"id":"cond-mat/9811095","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.str-el","submitted_at":"1998-11-06T15:48:09Z","cross_cats_sorted":[],"title_canon_sha256":"2caecfb0ad60d1ca92a4fcc36767ad3b9e830ea16f2fccda5d63453d78d9de4b","abstract_canon_sha256":"0885b35c8644aa006116767542d74744c019c974d61b9b6688838a3b4f71a696"},"schema_version":"1.0"},"canonical_sha256":"53102589e28d7be5be757c3b0555bd04a37d7583e05e0f15369cd2dae88f9940","source":{"kind":"arxiv","id":"cond-mat/9811095","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/9811095","created_at":"2026-05-18T01:07:05Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9811095v1","created_at":"2026-05-18T01:07:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9811095","created_at":"2026-05-18T01:07:05Z"},{"alias_kind":"pith_short_12","alias_value":"KMICLCPCRV56","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_16","alias_value":"KMICLCPCRV56LPTV","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_8","alias_value":"KMICLCPC","created_at":"2026-05-18T12:25:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1998:KMICLCPCRV56LPTVPQ5QKVN5AS","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/9811095","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.str-el","submitted_at":"1998-11-06T15:48:09Z","cross_cats_sorted":[],"title_canon_sha256":"2caecfb0ad60d1ca92a4fcc36767ad3b9e830ea16f2fccda5d63453d78d9de4b","abstract_canon_sha256":"0885b35c8644aa006116767542d74744c019c974d61b9b6688838a3b4f71a696"},"schema_version":"1.0"},"canonical_sha256":"53102589e28d7be5be757c3b0555bd04a37d7583e05e0f15369cd2dae88f9940","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:07:05.181994Z","signature_b64":"LmDRKNBAw65mrMqjFd3nXgkS1VhB7ZLlugw7fkQX5FL8v7+JCiiM7Gg2teK/2Jt/TO1kn9D/IKXM1dgjeGa/CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"53102589e28d7be5be757c3b0555bd04a37d7583e05e0f15369cd2dae88f9940","last_reissued_at":"2026-05-18T01:07:05.181361Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:07:05.181361Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/9811095","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":"2026-05-18T01:07:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DLHMlR5WiVd1103FZok0C+v/BchFzvLdASv6G6/nSkBv19u3zt7J4jVRHaspVg+N5RUxbjjnGtvOgmZlV2knDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T17:26:10.477910Z"},"content_sha256":"be8ccfa363780f19b12b0d4b06dc4f17bcc6281d42c6183f9a0bda5abdd26f31","schema_version":"1.0","event_id":"sha256:be8ccfa363780f19b12b0d4b06dc4f17bcc6281d42c6183f9a0bda5abdd26f31"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1998:KMICLCPCRV56LPTVPQ5QKVN5AS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Combining dynamical mean-field theory and realistic bandstructure of V2O3","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"J. Appel, M. Grodzicki, T. Wolenski","submitted_at":"1998-11-06T15:48:09Z","abstract_excerpt":"Recent neutron scattering experiments on V2O3 show that the magnetic fluctuations on the metallic side of the antiferromagnetic metal-insulator transition are not related to the spin structure of the insulator, but rather to the bandstructure-driven spin-density wave phase of the doped system V(2-y)O3. We calculate these magnetic fluctuations starting from a Slater-Koster bandstructure and incorporating the correlation effects through the dynamical mean-field theory (DMFT). Our results demonstrate that the magnetic properties of the paramagnetic metallic phase are dominated by the Fermi surfac"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9811095","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":"2026-05-18T01:07:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BY7oYPQUUX2ZvR8nXGNx8vY5cVyoNSDtGEpvN/q5gMZ3DarWR6GKlnMMRXuRFp4g0rSbnj3D1sb3dYt4RNgGAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T17:26:10.478528Z"},"content_sha256":"3a7b73978ab1ebc83f105612691abc35f47c09dd19786ab795e545b243ea634d","schema_version":"1.0","event_id":"sha256:3a7b73978ab1ebc83f105612691abc35f47c09dd19786ab795e545b243ea634d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KMICLCPCRV56LPTVPQ5QKVN5AS/bundle.json","state_url":"https://pith.science/pith/KMICLCPCRV56LPTVPQ5QKVN5AS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KMICLCPCRV56LPTVPQ5QKVN5AS/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":"2026-05-29T17:26:10Z","links":{"resolver":"https://pith.science/pith/KMICLCPCRV56LPTVPQ5QKVN5AS","bundle":"https://pith.science/pith/KMICLCPCRV56LPTVPQ5QKVN5AS/bundle.json","state":"https://pith.science/pith/KMICLCPCRV56LPTVPQ5QKVN5AS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KMICLCPCRV56LPTVPQ5QKVN5AS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1998:KMICLCPCRV56LPTVPQ5QKVN5AS","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":"0885b35c8644aa006116767542d74744c019c974d61b9b6688838a3b4f71a696","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat.str-el","submitted_at":"1998-11-06T15:48:09Z","title_canon_sha256":"2caecfb0ad60d1ca92a4fcc36767ad3b9e830ea16f2fccda5d63453d78d9de4b"},"schema_version":"1.0","source":{"id":"cond-mat/9811095","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/9811095","created_at":"2026-05-18T01:07:05Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9811095v1","created_at":"2026-05-18T01:07:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9811095","created_at":"2026-05-18T01:07:05Z"},{"alias_kind":"pith_short_12","alias_value":"KMICLCPCRV56","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_16","alias_value":"KMICLCPCRV56LPTV","created_at":"2026-05-18T12:25:49Z"},{"alias_kind":"pith_short_8","alias_value":"KMICLCPC","created_at":"2026-05-18T12:25:49Z"}],"graph_snapshots":[{"event_id":"sha256:3a7b73978ab1ebc83f105612691abc35f47c09dd19786ab795e545b243ea634d","target":"graph","created_at":"2026-05-18T01:07:05Z","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":"Recent neutron scattering experiments on V2O3 show that the magnetic fluctuations on the metallic side of the antiferromagnetic metal-insulator transition are not related to the spin structure of the insulator, but rather to the bandstructure-driven spin-density wave phase of the doped system V(2-y)O3. We calculate these magnetic fluctuations starting from a Slater-Koster bandstructure and incorporating the correlation effects through the dynamical mean-field theory (DMFT). Our results demonstrate that the magnetic properties of the paramagnetic metallic phase are dominated by the Fermi surfac","authors_text":"J. Appel, M. Grodzicki, T. Wolenski","cross_cats":[],"headline":"","license":"","primary_cat":"cond-mat.str-el","submitted_at":"1998-11-06T15:48:09Z","title":"Combining dynamical mean-field theory and realistic bandstructure of V2O3"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9811095","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:be8ccfa363780f19b12b0d4b06dc4f17bcc6281d42c6183f9a0bda5abdd26f31","target":"record","created_at":"2026-05-18T01:07:05Z","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":"0885b35c8644aa006116767542d74744c019c974d61b9b6688838a3b4f71a696","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat.str-el","submitted_at":"1998-11-06T15:48:09Z","title_canon_sha256":"2caecfb0ad60d1ca92a4fcc36767ad3b9e830ea16f2fccda5d63453d78d9de4b"},"schema_version":"1.0","source":{"id":"cond-mat/9811095","kind":"arxiv","version":1}},"canonical_sha256":"53102589e28d7be5be757c3b0555bd04a37d7583e05e0f15369cd2dae88f9940","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"53102589e28d7be5be757c3b0555bd04a37d7583e05e0f15369cd2dae88f9940","first_computed_at":"2026-05-18T01:07:05.181361Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:07:05.181361Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"LmDRKNBAw65mrMqjFd3nXgkS1VhB7ZLlugw7fkQX5FL8v7+JCiiM7Gg2teK/2Jt/TO1kn9D/IKXM1dgjeGa/CQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:07:05.181994Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/9811095","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:be8ccfa363780f19b12b0d4b06dc4f17bcc6281d42c6183f9a0bda5abdd26f31","sha256:3a7b73978ab1ebc83f105612691abc35f47c09dd19786ab795e545b243ea634d"],"state_sha256":"120d4b437ad946e4f386d3fc17c2f6210ae2a6869ed0da6d6fd12013aea7cbd0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fKlcFwOcUqiawA+w6fEviBZnTK5XNqLL59MTo/6weSneHoD/2kH6joAO2cZkXACke4sbm8DaexoKOYy2ToNIDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T17:26:10.481363Z","bundle_sha256":"c24992939d00dfd1b06fb68c58b9f61b603fa26b5a006dfc7c7495a9526b4cd1"}}