{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:DQJIJOLS6WM62N62KTXVSI3CD4","short_pith_number":"pith:DQJIJOLS","schema_version":"1.0","canonical_sha256":"1c1284b972f599ed37da54ef5923621f0af191d79c4600abba51f319e3b09e16","source":{"kind":"arxiv","id":"1101.2290","version":1},"attestation_state":"computed","paper":{"title":"Constraints on the axion-electron coupling for solar axions produced by Compton process and bremsstrahlung","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.SR","hep-ph"],"primary_cat":"hep-ex","authors_text":"A.S. Kayunov, A.V. Derbin, D.A. Semenov, E.V. Unzhakov, V.N. Muratova","submitted_at":"2011-01-12T08:10:16Z","abstract_excerpt":"The search for solar axions produced by Compton ($\\gamma+e^-\\rightarrow e^-+A$) and bremsstrahlung-like ($e^-+Z \\rightarrow Z+e^-+A$) processes has been performed. The axion flux in the both cases depends on the axion-electron coupling constant. The resonant excitation of low-lying nuclear level of $^{169}\\rm{Tm}$ was looked for: $A+^{169}$Tm $\\rightarrow ^{169}$Tm$^*$ $\\rightarrow ^{169}$Tm $+ \\gamma$ (8.41 keV). The Si(Li) detector and $^{169}$Tm target installed inside the low-background setup were used to detect 8.41 keV $\\gamma$-rays. As a result, a new model independent restriction on th"},"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":"1101.2290","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2011-01-12T08:10:16Z","cross_cats_sorted":["astro-ph.SR","hep-ph"],"title_canon_sha256":"27fa1d4e14792d5f0636a50c9bbbc30de55be73e19a3eb37be1210eb7794d046","abstract_canon_sha256":"240f96e4c8b7cfdcb7930e1c48a15b57f243a9f83e97c5053ee3ac1f3541d7a8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:27:57.825828Z","signature_b64":"vl6E6c2JemhISQ/tf/o0TLthnbXJircecNl7yEcPMg0X4DE2QuQ4H0H60APoWEyO4Zv4xmNhHa5LEwcCpFsHCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1c1284b972f599ed37da54ef5923621f0af191d79c4600abba51f319e3b09e16","last_reissued_at":"2026-05-18T04:27:57.825141Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:27:57.825141Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Constraints on the axion-electron coupling for solar axions produced by Compton process and bremsstrahlung","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.SR","hep-ph"],"primary_cat":"hep-ex","authors_text":"A.S. Kayunov, A.V. Derbin, D.A. Semenov, E.V. Unzhakov, V.N. Muratova","submitted_at":"2011-01-12T08:10:16Z","abstract_excerpt":"The search for solar axions produced by Compton ($\\gamma+e^-\\rightarrow e^-+A$) and bremsstrahlung-like ($e^-+Z \\rightarrow Z+e^-+A$) processes has been performed. The axion flux in the both cases depends on the axion-electron coupling constant. The resonant excitation of low-lying nuclear level of $^{169}\\rm{Tm}$ was looked for: $A+^{169}$Tm $\\rightarrow ^{169}$Tm$^*$ $\\rightarrow ^{169}$Tm $+ \\gamma$ (8.41 keV). The Si(Li) detector and $^{169}$Tm target installed inside the low-background setup were used to detect 8.41 keV $\\gamma$-rays. As a result, a new model independent restriction on th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1101.2290","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":"1101.2290","created_at":"2026-05-18T04:27:57.825241+00:00"},{"alias_kind":"arxiv_version","alias_value":"1101.2290v1","created_at":"2026-05-18T04:27:57.825241+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1101.2290","created_at":"2026-05-18T04:27:57.825241+00:00"},{"alias_kind":"pith_short_12","alias_value":"DQJIJOLS6WM6","created_at":"2026-05-18T12:26:26.731475+00:00"},{"alias_kind":"pith_short_16","alias_value":"DQJIJOLS6WM62N62","created_at":"2026-05-18T12:26:26.731475+00:00"},{"alias_kind":"pith_short_8","alias_value":"DQJIJOLS","created_at":"2026-05-18T12:26:26.731475+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/DQJIJOLS6WM62N62KTXVSI3CD4","json":"https://pith.science/pith/DQJIJOLS6WM62N62KTXVSI3CD4.json","graph_json":"https://pith.science/api/pith-number/DQJIJOLS6WM62N62KTXVSI3CD4/graph.json","events_json":"https://pith.science/api/pith-number/DQJIJOLS6WM62N62KTXVSI3CD4/events.json","paper":"https://pith.science/paper/DQJIJOLS"},"agent_actions":{"view_html":"https://pith.science/pith/DQJIJOLS6WM62N62KTXVSI3CD4","download_json":"https://pith.science/pith/DQJIJOLS6WM62N62KTXVSI3CD4.json","view_paper":"https://pith.science/paper/DQJIJOLS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1101.2290&json=true","fetch_graph":"https://pith.science/api/pith-number/DQJIJOLS6WM62N62KTXVSI3CD4/graph.json","fetch_events":"https://pith.science/api/pith-number/DQJIJOLS6WM62N62KTXVSI3CD4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DQJIJOLS6WM62N62KTXVSI3CD4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DQJIJOLS6WM62N62KTXVSI3CD4/action/storage_attestation","attest_author":"https://pith.science/pith/DQJIJOLS6WM62N62KTXVSI3CD4/action/author_attestation","sign_citation":"https://pith.science/pith/DQJIJOLS6WM62N62KTXVSI3CD4/action/citation_signature","submit_replication":"https://pith.science/pith/DQJIJOLS6WM62N62KTXVSI3CD4/action/replication_record"}},"created_at":"2026-05-18T04:27:57.825241+00:00","updated_at":"2026-05-18T04:27:57.825241+00:00"}