{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:HGWO6HP7N5YX3RMXCNAYSX4LEV","short_pith_number":"pith:HGWO6HP7","schema_version":"1.0","canonical_sha256":"39acef1dff6f717dc5971341895f8b2578c6e363403678526cf3fe7d61745dbe","source":{"kind":"arxiv","id":"1103.1228","version":1},"attestation_state":"computed","paper":{"title":"High-Spatial-Resolution Monitoring of Strong Magnetic Field using Rb vapor Nanometric-Thin Cell","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"C. Leroy, D. Sarkisyan, G. Hakhumyan, M. Auzinsh, Y. Pashayan-Leroy","submitted_at":"2011-03-07T10:18:58Z","abstract_excerpt":"We have implemented the so-called $\\lambda$-Zeeman technique (LZT) to investigate individual hyperfine transitions between Zeeman sublevels of the Rb atoms in a strong external magnetic field $B$ in the range of $2500 - 5000$ G (recently it was established that LZT is very convenient for the range of $10 - 2500$ G). Atoms are confined in a nanometric thin cell (NTC) with the thickness $L = \\lambda$, where $\\lambda$ is the resonant wavelength 794 nm for Rb $D_1$ line. Narrow velocity selective optical pumping (VSOP) resonances in the transmission spectrum of the NTC are split into several compo"},"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":"1103.1228","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-03-07T10:18:58Z","cross_cats_sorted":[],"title_canon_sha256":"9d2f61a5114bfb7f423c9d661f06b4db6b74050d87c8563c36e7353fd3834c27","abstract_canon_sha256":"5ff3e757ec7ffe3eb1929c9f6ba0f07e798f11df1724a405d00653fd023c62f5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:02:58.987917Z","signature_b64":"sChFn6VPLkFBpAg0+KHWBIF5LV36KGG3vqoay+jqgoZefilA5tNfIQJ2jluupXTDSvb+gu7FflC4W0+ecd6OCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"39acef1dff6f717dc5971341895f8b2578c6e363403678526cf3fe7d61745dbe","last_reissued_at":"2026-05-18T02:02:58.987261Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:02:58.987261Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"High-Spatial-Resolution Monitoring of Strong Magnetic Field using Rb vapor Nanometric-Thin Cell","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"C. Leroy, D. Sarkisyan, G. Hakhumyan, M. Auzinsh, Y. Pashayan-Leroy","submitted_at":"2011-03-07T10:18:58Z","abstract_excerpt":"We have implemented the so-called $\\lambda$-Zeeman technique (LZT) to investigate individual hyperfine transitions between Zeeman sublevels of the Rb atoms in a strong external magnetic field $B$ in the range of $2500 - 5000$ G (recently it was established that LZT is very convenient for the range of $10 - 2500$ G). Atoms are confined in a nanometric thin cell (NTC) with the thickness $L = \\lambda$, where $\\lambda$ is the resonant wavelength 794 nm for Rb $D_1$ line. Narrow velocity selective optical pumping (VSOP) resonances in the transmission spectrum of the NTC are split into several compo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1103.1228","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":"1103.1228","created_at":"2026-05-18T02:02:58.987377+00:00"},{"alias_kind":"arxiv_version","alias_value":"1103.1228v1","created_at":"2026-05-18T02:02:58.987377+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1103.1228","created_at":"2026-05-18T02:02:58.987377+00:00"},{"alias_kind":"pith_short_12","alias_value":"HGWO6HP7N5YX","created_at":"2026-05-18T12:26:30.835961+00:00"},{"alias_kind":"pith_short_16","alias_value":"HGWO6HP7N5YX3RMX","created_at":"2026-05-18T12:26:30.835961+00:00"},{"alias_kind":"pith_short_8","alias_value":"HGWO6HP7","created_at":"2026-05-18T12:26:30.835961+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/HGWO6HP7N5YX3RMXCNAYSX4LEV","json":"https://pith.science/pith/HGWO6HP7N5YX3RMXCNAYSX4LEV.json","graph_json":"https://pith.science/api/pith-number/HGWO6HP7N5YX3RMXCNAYSX4LEV/graph.json","events_json":"https://pith.science/api/pith-number/HGWO6HP7N5YX3RMXCNAYSX4LEV/events.json","paper":"https://pith.science/paper/HGWO6HP7"},"agent_actions":{"view_html":"https://pith.science/pith/HGWO6HP7N5YX3RMXCNAYSX4LEV","download_json":"https://pith.science/pith/HGWO6HP7N5YX3RMXCNAYSX4LEV.json","view_paper":"https://pith.science/paper/HGWO6HP7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1103.1228&json=true","fetch_graph":"https://pith.science/api/pith-number/HGWO6HP7N5YX3RMXCNAYSX4LEV/graph.json","fetch_events":"https://pith.science/api/pith-number/HGWO6HP7N5YX3RMXCNAYSX4LEV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HGWO6HP7N5YX3RMXCNAYSX4LEV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HGWO6HP7N5YX3RMXCNAYSX4LEV/action/storage_attestation","attest_author":"https://pith.science/pith/HGWO6HP7N5YX3RMXCNAYSX4LEV/action/author_attestation","sign_citation":"https://pith.science/pith/HGWO6HP7N5YX3RMXCNAYSX4LEV/action/citation_signature","submit_replication":"https://pith.science/pith/HGWO6HP7N5YX3RMXCNAYSX4LEV/action/replication_record"}},"created_at":"2026-05-18T02:02:58.987377+00:00","updated_at":"2026-05-18T02:02:58.987377+00:00"}