{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:SSU7P6ZEV2LXTPNLIY5SVEBLN2","short_pith_number":"pith:SSU7P6ZE","schema_version":"1.0","canonical_sha256":"94a9f7fb24ae9779bdab463b2a902b6ea4744463d6ad0d57d4302a6ecc0d8249","source":{"kind":"arxiv","id":"1412.2012","version":1},"attestation_state":"computed","paper":{"title":"Electron Paramagnetic Resonance of Mn in Bi$_2$Se$_3$ Topological Insulator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Agnieszka Wolos, Andrzej Hruban, Andrzej Materna, Aneta Drabinska, Magdalena Romaniec, Maria Kaminska, Miroslaw Piersa, Ryszard Diduszko, Stanislawa G. Strzelecka","submitted_at":"2014-12-05T14:42:17Z","abstract_excerpt":"Electron paramagnetic resonance was used to investigate Mn impurity in Bi$_2$Se$_3$ topological insulator grown by the vertical Bridgman method. Mn in high-spin S = 5/2, Mn$^2$$^+$ configuration, was detected regardless of the conductivity type of the host material. This means that Mn$^2$$^+$(d$^5$) energy level is located within the valence band, and Mn$^1$$^+$(d$^6$) energy level is outside the energy gap of Bi$_2$Se$_3$. The electron paramagnetic resonance spectrum of Mn$^2$$^+$ in Bi$_2$Se$_3$ is characterized by the isotropic g-factor |g| = 1.91 and large axial parameter D = -4.20 GHz x h"},"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":"1412.2012","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2014-12-05T14:42:17Z","cross_cats_sorted":[],"title_canon_sha256":"2f5feaf99e81abc99d4b10ee0c8a1b728beedef1297cd80b027f323f4ce8a019","abstract_canon_sha256":"a9f486c11c83f8f8fdac48b51e43dc6c481f61139bcd12664729b5d92174f792"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:32:05.552576Z","signature_b64":"1VandCIhRnbzvOOZOVX/E4wUW94WU/VAFzGiRUJW+skRYnpbT1wf6jl3aPp0Yy3c6f1BuHZkd9nEhmsytA1mAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"94a9f7fb24ae9779bdab463b2a902b6ea4744463d6ad0d57d4302a6ecc0d8249","last_reissued_at":"2026-05-18T02:32:05.552164Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:32:05.552164Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electron Paramagnetic Resonance of Mn in Bi$_2$Se$_3$ Topological Insulator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Agnieszka Wolos, Andrzej Hruban, Andrzej Materna, Aneta Drabinska, Magdalena Romaniec, Maria Kaminska, Miroslaw Piersa, Ryszard Diduszko, Stanislawa G. Strzelecka","submitted_at":"2014-12-05T14:42:17Z","abstract_excerpt":"Electron paramagnetic resonance was used to investigate Mn impurity in Bi$_2$Se$_3$ topological insulator grown by the vertical Bridgman method. Mn in high-spin S = 5/2, Mn$^2$$^+$ configuration, was detected regardless of the conductivity type of the host material. This means that Mn$^2$$^+$(d$^5$) energy level is located within the valence band, and Mn$^1$$^+$(d$^6$) energy level is outside the energy gap of Bi$_2$Se$_3$. The electron paramagnetic resonance spectrum of Mn$^2$$^+$ in Bi$_2$Se$_3$ is characterized by the isotropic g-factor |g| = 1.91 and large axial parameter D = -4.20 GHz x h"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.2012","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":"1412.2012","created_at":"2026-05-18T02:32:05.552224+00:00"},{"alias_kind":"arxiv_version","alias_value":"1412.2012v1","created_at":"2026-05-18T02:32:05.552224+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.2012","created_at":"2026-05-18T02:32:05.552224+00:00"},{"alias_kind":"pith_short_12","alias_value":"SSU7P6ZEV2LX","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_16","alias_value":"SSU7P6ZEV2LXTPNL","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_8","alias_value":"SSU7P6ZE","created_at":"2026-05-18T12:28:49.207871+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/SSU7P6ZEV2LXTPNLIY5SVEBLN2","json":"https://pith.science/pith/SSU7P6ZEV2LXTPNLIY5SVEBLN2.json","graph_json":"https://pith.science/api/pith-number/SSU7P6ZEV2LXTPNLIY5SVEBLN2/graph.json","events_json":"https://pith.science/api/pith-number/SSU7P6ZEV2LXTPNLIY5SVEBLN2/events.json","paper":"https://pith.science/paper/SSU7P6ZE"},"agent_actions":{"view_html":"https://pith.science/pith/SSU7P6ZEV2LXTPNLIY5SVEBLN2","download_json":"https://pith.science/pith/SSU7P6ZEV2LXTPNLIY5SVEBLN2.json","view_paper":"https://pith.science/paper/SSU7P6ZE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1412.2012&json=true","fetch_graph":"https://pith.science/api/pith-number/SSU7P6ZEV2LXTPNLIY5SVEBLN2/graph.json","fetch_events":"https://pith.science/api/pith-number/SSU7P6ZEV2LXTPNLIY5SVEBLN2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SSU7P6ZEV2LXTPNLIY5SVEBLN2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SSU7P6ZEV2LXTPNLIY5SVEBLN2/action/storage_attestation","attest_author":"https://pith.science/pith/SSU7P6ZEV2LXTPNLIY5SVEBLN2/action/author_attestation","sign_citation":"https://pith.science/pith/SSU7P6ZEV2LXTPNLIY5SVEBLN2/action/citation_signature","submit_replication":"https://pith.science/pith/SSU7P6ZEV2LXTPNLIY5SVEBLN2/action/replication_record"}},"created_at":"2026-05-18T02:32:05.552224+00:00","updated_at":"2026-05-18T02:32:05.552224+00:00"}