{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:HGQN4CHLD5FTA4Q7D2JMMMG5XE","short_pith_number":"pith:HGQN4CHL","schema_version":"1.0","canonical_sha256":"39a0de08eb1f4b30721f1e92c630ddb90a6ed89a02f9bed35e863b5fcaea19cb","source":{"kind":"arxiv","id":"1207.1754","version":1},"attestation_state":"computed","paper":{"title":"Analytical description of spin-Rabi oscillation controlled electronic transitions rates between weakly coupled pairs of paramagnetic states with S=1/2","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"C. Boehme, M. E. Raikh, R. Glenn, W. J. Baker","submitted_at":"2012-07-07T01:57:49Z","abstract_excerpt":"We report on an analytical description of spin-dependent electronic transition rates which are controlled by a radiation induced spin-Rabi oscillation of weakly spin-exchange and spin-dipolar coupled paramagnetic states (S=1/2). The oscillation components (the Fourier content) of the net transition rates within spin-pair ensembles are derived for randomly distributed spin resonances with account of a possible correlation between the two distributions that correspond to the two individual pair partners. The results presented here show that when electrically or optically detected Rabi spectrosco"},"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":"1207.1754","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2012-07-07T01:57:49Z","cross_cats_sorted":[],"title_canon_sha256":"c00707db0329e0261691372e82ae89f04d15f2c8011772abea472dc98b7bcc0a","abstract_canon_sha256":"8daa939266ea609dca517b6fd9b71cf0141990abdc0363063c43d4c9c46b872f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:27:23.104484Z","signature_b64":"ddsNEkYFrulWaLnQ/lw5jmXVSnjm0zKH5oDzKo36c450PZWmBi3Q61rRRAC9Qe43Mp8JhnIXO/xFw7Dz2aiLDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"39a0de08eb1f4b30721f1e92c630ddb90a6ed89a02f9bed35e863b5fcaea19cb","last_reissued_at":"2026-05-18T03:27:23.103737Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:27:23.103737Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Analytical description of spin-Rabi oscillation controlled electronic transitions rates between weakly coupled pairs of paramagnetic states with S=1/2","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"C. Boehme, M. E. Raikh, R. Glenn, W. J. Baker","submitted_at":"2012-07-07T01:57:49Z","abstract_excerpt":"We report on an analytical description of spin-dependent electronic transition rates which are controlled by a radiation induced spin-Rabi oscillation of weakly spin-exchange and spin-dipolar coupled paramagnetic states (S=1/2). The oscillation components (the Fourier content) of the net transition rates within spin-pair ensembles are derived for randomly distributed spin resonances with account of a possible correlation between the two distributions that correspond to the two individual pair partners. The results presented here show that when electrically or optically detected Rabi spectrosco"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.1754","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":"1207.1754","created_at":"2026-05-18T03:27:23.103859+00:00"},{"alias_kind":"arxiv_version","alias_value":"1207.1754v1","created_at":"2026-05-18T03:27:23.103859+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.1754","created_at":"2026-05-18T03:27:23.103859+00:00"},{"alias_kind":"pith_short_12","alias_value":"HGQN4CHLD5FT","created_at":"2026-05-18T12:27:09.501522+00:00"},{"alias_kind":"pith_short_16","alias_value":"HGQN4CHLD5FTA4Q7","created_at":"2026-05-18T12:27:09.501522+00:00"},{"alias_kind":"pith_short_8","alias_value":"HGQN4CHL","created_at":"2026-05-18T12:27:09.501522+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/HGQN4CHLD5FTA4Q7D2JMMMG5XE","json":"https://pith.science/pith/HGQN4CHLD5FTA4Q7D2JMMMG5XE.json","graph_json":"https://pith.science/api/pith-number/HGQN4CHLD5FTA4Q7D2JMMMG5XE/graph.json","events_json":"https://pith.science/api/pith-number/HGQN4CHLD5FTA4Q7D2JMMMG5XE/events.json","paper":"https://pith.science/paper/HGQN4CHL"},"agent_actions":{"view_html":"https://pith.science/pith/HGQN4CHLD5FTA4Q7D2JMMMG5XE","download_json":"https://pith.science/pith/HGQN4CHLD5FTA4Q7D2JMMMG5XE.json","view_paper":"https://pith.science/paper/HGQN4CHL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1207.1754&json=true","fetch_graph":"https://pith.science/api/pith-number/HGQN4CHLD5FTA4Q7D2JMMMG5XE/graph.json","fetch_events":"https://pith.science/api/pith-number/HGQN4CHLD5FTA4Q7D2JMMMG5XE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HGQN4CHLD5FTA4Q7D2JMMMG5XE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HGQN4CHLD5FTA4Q7D2JMMMG5XE/action/storage_attestation","attest_author":"https://pith.science/pith/HGQN4CHLD5FTA4Q7D2JMMMG5XE/action/author_attestation","sign_citation":"https://pith.science/pith/HGQN4CHLD5FTA4Q7D2JMMMG5XE/action/citation_signature","submit_replication":"https://pith.science/pith/HGQN4CHLD5FTA4Q7D2JMMMG5XE/action/replication_record"}},"created_at":"2026-05-18T03:27:23.103859+00:00","updated_at":"2026-05-18T03:27:23.103859+00:00"}