{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:Z3QJKACDJ2QD67SSJ5MKZU7WUQ","short_pith_number":"pith:Z3QJKACD","schema_version":"1.0","canonical_sha256":"cee09500434ea03f7e524f58acd3f6a4086bddd4db49d25a30816c39980d4dad","source":{"kind":"arxiv","id":"1311.1499","version":1},"attestation_state":"computed","paper":{"title":"Anomalies in radiation-collisional kinetics of Rydberg atoms induced by the effects of dynamical chaos and the double Stark resonance","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"astro-ph.SR","authors_text":"A.A. Mihajlov, A.N. Klyucharev, N.N. Bezuglov, V.A. Sreckovic","submitted_at":"2013-11-05T21:15:30Z","abstract_excerpt":"Radiative and collisional constants of excited atoms contain the matrix elements of the dipole transitions and when they are blocked one can expect occurring a number of interesting phenomena in radiation-collisional kinetics. In recent astrophysical studies of IR emission spectra it was revealed a gap in the radiation emitted by Rydberg atoms ($RA$) with values of the principal quantum number of $n\\approx10$. Under the presence of external electric fields a rearrangement of $RA$ emission spectra is possible to associate with manifestations of the Stark effect. The threshold for electric field"},"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":"1311.1499","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.SR","submitted_at":"2013-11-05T21:15:30Z","cross_cats_sorted":["physics.atom-ph"],"title_canon_sha256":"cc4c9877271d1792e347ee3ecd9146a72f14f007438741e3e71d588c9acbc110","abstract_canon_sha256":"16985407f0f7890230dfbe8ac8196f5c311f4f43804174c4f1cd873fa498fb6c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:07:43.999811Z","signature_b64":"QD/M2PDQ6okUZA6PIEnEcIAxUI+VQDds5ITK5gFS3ttdrtr8aueuWaPwhDt4cX04FXbR5+7tW22Hks1CvnkxBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cee09500434ea03f7e524f58acd3f6a4086bddd4db49d25a30816c39980d4dad","last_reissued_at":"2026-05-18T03:07:43.999191Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:07:43.999191Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anomalies in radiation-collisional kinetics of Rydberg atoms induced by the effects of dynamical chaos and the double Stark resonance","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"astro-ph.SR","authors_text":"A.A. Mihajlov, A.N. Klyucharev, N.N. Bezuglov, V.A. Sreckovic","submitted_at":"2013-11-05T21:15:30Z","abstract_excerpt":"Radiative and collisional constants of excited atoms contain the matrix elements of the dipole transitions and when they are blocked one can expect occurring a number of interesting phenomena in radiation-collisional kinetics. In recent astrophysical studies of IR emission spectra it was revealed a gap in the radiation emitted by Rydberg atoms ($RA$) with values of the principal quantum number of $n\\approx10$. Under the presence of external electric fields a rearrangement of $RA$ emission spectra is possible to associate with manifestations of the Stark effect. The threshold for electric field"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.1499","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":"1311.1499","created_at":"2026-05-18T03:07:43.999287+00:00"},{"alias_kind":"arxiv_version","alias_value":"1311.1499v1","created_at":"2026-05-18T03:07:43.999287+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.1499","created_at":"2026-05-18T03:07:43.999287+00:00"},{"alias_kind":"pith_short_12","alias_value":"Z3QJKACDJ2QD","created_at":"2026-05-18T12:28:09.283467+00:00"},{"alias_kind":"pith_short_16","alias_value":"Z3QJKACDJ2QD67SS","created_at":"2026-05-18T12:28:09.283467+00:00"},{"alias_kind":"pith_short_8","alias_value":"Z3QJKACD","created_at":"2026-05-18T12:28:09.283467+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/Z3QJKACDJ2QD67SSJ5MKZU7WUQ","json":"https://pith.science/pith/Z3QJKACDJ2QD67SSJ5MKZU7WUQ.json","graph_json":"https://pith.science/api/pith-number/Z3QJKACDJ2QD67SSJ5MKZU7WUQ/graph.json","events_json":"https://pith.science/api/pith-number/Z3QJKACDJ2QD67SSJ5MKZU7WUQ/events.json","paper":"https://pith.science/paper/Z3QJKACD"},"agent_actions":{"view_html":"https://pith.science/pith/Z3QJKACDJ2QD67SSJ5MKZU7WUQ","download_json":"https://pith.science/pith/Z3QJKACDJ2QD67SSJ5MKZU7WUQ.json","view_paper":"https://pith.science/paper/Z3QJKACD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1311.1499&json=true","fetch_graph":"https://pith.science/api/pith-number/Z3QJKACDJ2QD67SSJ5MKZU7WUQ/graph.json","fetch_events":"https://pith.science/api/pith-number/Z3QJKACDJ2QD67SSJ5MKZU7WUQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Z3QJKACDJ2QD67SSJ5MKZU7WUQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Z3QJKACDJ2QD67SSJ5MKZU7WUQ/action/storage_attestation","attest_author":"https://pith.science/pith/Z3QJKACDJ2QD67SSJ5MKZU7WUQ/action/author_attestation","sign_citation":"https://pith.science/pith/Z3QJKACDJ2QD67SSJ5MKZU7WUQ/action/citation_signature","submit_replication":"https://pith.science/pith/Z3QJKACDJ2QD67SSJ5MKZU7WUQ/action/replication_record"}},"created_at":"2026-05-18T03:07:43.999287+00:00","updated_at":"2026-05-18T03:07:43.999287+00:00"}