{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2009:YNY7UJR4R6EXLEKW4KDPCEV56Z","short_pith_number":"pith:YNY7UJR4","canonical_record":{"source":{"id":"0902.0098","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"nucl-th","submitted_at":"2009-02-01T00:48:56Z","cross_cats_sorted":[],"title_canon_sha256":"cd947eb9baeb5c6ef52a87a86bf9c47d26ab3b1780616dd23854380aed581df5","abstract_canon_sha256":"9450c75c72718b73960fe21be3605b383901e0213a65dc1f910f25fcccaef7b1"},"schema_version":"1.0"},"canonical_sha256":"c371fa263c8f89759156e286f112bdf67c756557c1e616f3aba18096a861b61e","source":{"kind":"arxiv","id":"0902.0098","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0902.0098","created_at":"2026-05-18T04:35:05Z"},{"alias_kind":"arxiv_version","alias_value":"0902.0098v1","created_at":"2026-05-18T04:35:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0902.0098","created_at":"2026-05-18T04:35:05Z"},{"alias_kind":"pith_short_12","alias_value":"YNY7UJR4R6EX","created_at":"2026-05-18T12:26:02Z"},{"alias_kind":"pith_short_16","alias_value":"YNY7UJR4R6EXLEKW","created_at":"2026-05-18T12:26:02Z"},{"alias_kind":"pith_short_8","alias_value":"YNY7UJR4","created_at":"2026-05-18T12:26:02Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2009:YNY7UJR4R6EXLEKW4KDPCEV56Z","target":"record","payload":{"canonical_record":{"source":{"id":"0902.0098","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"nucl-th","submitted_at":"2009-02-01T00:48:56Z","cross_cats_sorted":[],"title_canon_sha256":"cd947eb9baeb5c6ef52a87a86bf9c47d26ab3b1780616dd23854380aed581df5","abstract_canon_sha256":"9450c75c72718b73960fe21be3605b383901e0213a65dc1f910f25fcccaef7b1"},"schema_version":"1.0"},"canonical_sha256":"c371fa263c8f89759156e286f112bdf67c756557c1e616f3aba18096a861b61e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:35:05.508682Z","signature_b64":"Pl/jVaz5s8jHXkL/EkL1EphrmIzHuu96uWbh+BRJM3fHcWNBvBWFK3Cu8odiPirtsV4LFLv41e6bGMcEM3nzAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c371fa263c8f89759156e286f112bdf67c756557c1e616f3aba18096a861b61e","last_reissued_at":"2026-05-18T04:35:05.508187Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:35:05.508187Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0902.0098","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":"2026-05-18T04:35:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CLuzNa6Y7AMsxe1fWNrCbA+enR6aNoK0uYJHY57BgfOpwZ2pntmkZLIV71F6NjdFSwUD/SMHDT8nZ67/gczZAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T21:52:26.564738Z"},"content_sha256":"12039a54125272a6f7a68c0eb6755a5ff515b86700de0700a13c83a28954274c","schema_version":"1.0","event_id":"sha256:12039a54125272a6f7a68c0eb6755a5ff515b86700de0700a13c83a28954274c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2009:YNY7UJR4R6EXLEKW4KDPCEV56Z","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Band terminations in density functional theory","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A. V. Afanasjev","submitted_at":"2009-02-01T00:48:56Z","abstract_excerpt":"The analysis of the terminating bands has been performed in the relativistic mean field framework. It was shown that nuclear magnetism provides an additional binding to the energies of the specific configuration and this additional binding increases with spin and has its {\\it maximum} exactly at the terminating state. This suggests that the terminating states can be an interesting probe of the time-odd mean fields {\\it provided that other effects can be reliably isolated.} Unfortunately, a reliable isolation of these effects is not that simple: many terms of the density functional theories con"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0902.0098","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":"2026-05-18T04:35:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xHn7OY9BOsqMKNyTExCPS8Yw2ukK8Ali9DPlBpUZdhWhWeBx0EELQC4MlrwaSWnQSZF7En+k8DYU+FoKdd66Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T21:52:26.565363Z"},"content_sha256":"805051c33aa32938e2d37ceb9884ae921ba60e09a35c347564e6ccf85cec67a4","schema_version":"1.0","event_id":"sha256:805051c33aa32938e2d37ceb9884ae921ba60e09a35c347564e6ccf85cec67a4"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YNY7UJR4R6EXLEKW4KDPCEV56Z/bundle.json","state_url":"https://pith.science/pith/YNY7UJR4R6EXLEKW4KDPCEV56Z/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YNY7UJR4R6EXLEKW4KDPCEV56Z/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":"2026-05-26T21:52:26Z","links":{"resolver":"https://pith.science/pith/YNY7UJR4R6EXLEKW4KDPCEV56Z","bundle":"https://pith.science/pith/YNY7UJR4R6EXLEKW4KDPCEV56Z/bundle.json","state":"https://pith.science/pith/YNY7UJR4R6EXLEKW4KDPCEV56Z/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YNY7UJR4R6EXLEKW4KDPCEV56Z/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2009:YNY7UJR4R6EXLEKW4KDPCEV56Z","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":"9450c75c72718b73960fe21be3605b383901e0213a65dc1f910f25fcccaef7b1","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"nucl-th","submitted_at":"2009-02-01T00:48:56Z","title_canon_sha256":"cd947eb9baeb5c6ef52a87a86bf9c47d26ab3b1780616dd23854380aed581df5"},"schema_version":"1.0","source":{"id":"0902.0098","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0902.0098","created_at":"2026-05-18T04:35:05Z"},{"alias_kind":"arxiv_version","alias_value":"0902.0098v1","created_at":"2026-05-18T04:35:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0902.0098","created_at":"2026-05-18T04:35:05Z"},{"alias_kind":"pith_short_12","alias_value":"YNY7UJR4R6EX","created_at":"2026-05-18T12:26:02Z"},{"alias_kind":"pith_short_16","alias_value":"YNY7UJR4R6EXLEKW","created_at":"2026-05-18T12:26:02Z"},{"alias_kind":"pith_short_8","alias_value":"YNY7UJR4","created_at":"2026-05-18T12:26:02Z"}],"graph_snapshots":[{"event_id":"sha256:805051c33aa32938e2d37ceb9884ae921ba60e09a35c347564e6ccf85cec67a4","target":"graph","created_at":"2026-05-18T04:35:05Z","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":"The analysis of the terminating bands has been performed in the relativistic mean field framework. It was shown that nuclear magnetism provides an additional binding to the energies of the specific configuration and this additional binding increases with spin and has its {\\it maximum} exactly at the terminating state. This suggests that the terminating states can be an interesting probe of the time-odd mean fields {\\it provided that other effects can be reliably isolated.} Unfortunately, a reliable isolation of these effects is not that simple: many terms of the density functional theories con","authors_text":"A. V. Afanasjev","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"nucl-th","submitted_at":"2009-02-01T00:48:56Z","title":"Band terminations in density functional theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0902.0098","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":"sha256:12039a54125272a6f7a68c0eb6755a5ff515b86700de0700a13c83a28954274c","target":"record","created_at":"2026-05-18T04:35:05Z","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":"9450c75c72718b73960fe21be3605b383901e0213a65dc1f910f25fcccaef7b1","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"nucl-th","submitted_at":"2009-02-01T00:48:56Z","title_canon_sha256":"cd947eb9baeb5c6ef52a87a86bf9c47d26ab3b1780616dd23854380aed581df5"},"schema_version":"1.0","source":{"id":"0902.0098","kind":"arxiv","version":1}},"canonical_sha256":"c371fa263c8f89759156e286f112bdf67c756557c1e616f3aba18096a861b61e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c371fa263c8f89759156e286f112bdf67c756557c1e616f3aba18096a861b61e","first_computed_at":"2026-05-18T04:35:05.508187Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:35:05.508187Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Pl/jVaz5s8jHXkL/EkL1EphrmIzHuu96uWbh+BRJM3fHcWNBvBWFK3Cu8odiPirtsV4LFLv41e6bGMcEM3nzAg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:35:05.508682Z","signed_message":"canonical_sha256_bytes"},"source_id":"0902.0098","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:12039a54125272a6f7a68c0eb6755a5ff515b86700de0700a13c83a28954274c","sha256:805051c33aa32938e2d37ceb9884ae921ba60e09a35c347564e6ccf85cec67a4"],"state_sha256":"48f52f2465e2941e0c4d0e70dc53067013784ad3ff246ff598740349198940c5"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PQASA3c5cw7+UVgDgAH3f/ipsEJYqneHBPOuQZ6jSLmSU2dOujdZKVm+8qJovFfNzgP7ZXl3dI/EvKOuCnQTCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T21:52:26.567936Z","bundle_sha256":"e77b613ab3973eebc38275df8d53cbd175e6f7f639cad8e2b6854e2ead40e73a"}}