{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:MIBIHBS3XBVEWHFCTYYPMNSQEV","short_pith_number":"pith:MIBIHBS3","schema_version":"1.0","canonical_sha256":"620283865bb86a4b1ca29e30f6365025735982fcccf8b4a30d284a6039bd4bdb","source":{"kind":"arxiv","id":"1805.00073","version":6},"attestation_state":"computed","paper":{"title":"Photoionization of Xe and Rn from the relativistic random-phase theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Chang-Jian Tang, Chen-Kai Qiao, Gang Jiang, Hsin-Chang Chi, Keh-Ning Huang, Ming-Chien Hsu, Shin-Ted Lin, Xu-Gen Zheng","submitted_at":"2018-04-30T19:33:46Z","abstract_excerpt":"Photoionization cross section $\\sigma_{n\\kappa}$, asymmetry parameter $\\beta_{n\\kappa}$, and polarization parameters $\\xi_{n\\kappa}$, $\\eta_{n\\kappa}$, $\\zeta_{n\\kappa}$ of Xe and Rn are calculated in the fully relativistic formalism. To deal with the relativistic and correlation effects, we adopt the relativistic random-phase theory with channel couplings among different subshells. Energy ranges for giant \\emph{d}-resonance regions are especially considered."},"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":"1805.00073","kind":"arxiv","version":6},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2018-04-30T19:33:46Z","cross_cats_sorted":[],"title_canon_sha256":"867ccd05bb58170cc1766406d119b37f2f8e27535743af105f47c9980237f4bc","abstract_canon_sha256":"e507da6958baf87866608c03dc33839a68c171af918eef4ffcc3ffe6ad5ff940"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:29:26.765601Z","signature_b64":"/3eEgdJs16qIUVJvGRu8z3fYH+bZamrnzNIFKi/nlm/xsG4pc0ZYB0isL/OuwNxF4jG3nh39aQhZdilw14ckCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"620283865bb86a4b1ca29e30f6365025735982fcccf8b4a30d284a6039bd4bdb","last_reissued_at":"2026-07-05T00:29:26.765170Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:29:26.765170Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Photoionization of Xe and Rn from the relativistic random-phase theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Chang-Jian Tang, Chen-Kai Qiao, Gang Jiang, Hsin-Chang Chi, Keh-Ning Huang, Ming-Chien Hsu, Shin-Ted Lin, Xu-Gen Zheng","submitted_at":"2018-04-30T19:33:46Z","abstract_excerpt":"Photoionization cross section $\\sigma_{n\\kappa}$, asymmetry parameter $\\beta_{n\\kappa}$, and polarization parameters $\\xi_{n\\kappa}$, $\\eta_{n\\kappa}$, $\\zeta_{n\\kappa}$ of Xe and Rn are calculated in the fully relativistic formalism. To deal with the relativistic and correlation effects, we adopt the relativistic random-phase theory with channel couplings among different subshells. Energy ranges for giant \\emph{d}-resonance regions are especially considered."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.00073","kind":"arxiv","version":6},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1805.00073/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"1805.00073","created_at":"2026-07-05T00:29:26.765231+00:00"},{"alias_kind":"arxiv_version","alias_value":"1805.00073v6","created_at":"2026-07-05T00:29:26.765231+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.00073","created_at":"2026-07-05T00:29:26.765231+00:00"},{"alias_kind":"pith_short_12","alias_value":"MIBIHBS3XBVE","created_at":"2026-07-05T00:29:26.765231+00:00"},{"alias_kind":"pith_short_16","alias_value":"MIBIHBS3XBVEWHFC","created_at":"2026-07-05T00:29:26.765231+00:00"},{"alias_kind":"pith_short_8","alias_value":"MIBIHBS3","created_at":"2026-07-05T00:29:26.765231+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/MIBIHBS3XBVEWHFCTYYPMNSQEV","json":"https://pith.science/pith/MIBIHBS3XBVEWHFCTYYPMNSQEV.json","graph_json":"https://pith.science/api/pith-number/MIBIHBS3XBVEWHFCTYYPMNSQEV/graph.json","events_json":"https://pith.science/api/pith-number/MIBIHBS3XBVEWHFCTYYPMNSQEV/events.json","paper":"https://pith.science/paper/MIBIHBS3"},"agent_actions":{"view_html":"https://pith.science/pith/MIBIHBS3XBVEWHFCTYYPMNSQEV","download_json":"https://pith.science/pith/MIBIHBS3XBVEWHFCTYYPMNSQEV.json","view_paper":"https://pith.science/paper/MIBIHBS3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1805.00073&json=true","fetch_graph":"https://pith.science/api/pith-number/MIBIHBS3XBVEWHFCTYYPMNSQEV/graph.json","fetch_events":"https://pith.science/api/pith-number/MIBIHBS3XBVEWHFCTYYPMNSQEV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MIBIHBS3XBVEWHFCTYYPMNSQEV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MIBIHBS3XBVEWHFCTYYPMNSQEV/action/storage_attestation","attest_author":"https://pith.science/pith/MIBIHBS3XBVEWHFCTYYPMNSQEV/action/author_attestation","sign_citation":"https://pith.science/pith/MIBIHBS3XBVEWHFCTYYPMNSQEV/action/citation_signature","submit_replication":"https://pith.science/pith/MIBIHBS3XBVEWHFCTYYPMNSQEV/action/replication_record"}},"created_at":"2026-07-05T00:29:26.765231+00:00","updated_at":"2026-07-05T00:29:26.765231+00:00"}