{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:QGY23GIY35TL5FRLAKENGNHNGK","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"a232aaace3b29a0fc7afc9bc4782d6bc3ca5fdd04a134c2ade349702f3ce2d81","cross_cats_sorted":["cond-mat.mtrl-sci","nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2011-02-18T10:08:16Z","title_canon_sha256":"b3ecca903cbe11af585a05a459bde17983953f535c3aecc853d1ba84061a8c0a"},"schema_version":"1.0","source":{"id":"1102.3799","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1102.3799","created_at":"2026-05-18T04:26:22Z"},{"alias_kind":"arxiv_version","alias_value":"1102.3799v1","created_at":"2026-05-18T04:26:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1102.3799","created_at":"2026-05-18T04:26:22Z"},{"alias_kind":"pith_short_12","alias_value":"QGY23GIY35TL","created_at":"2026-05-18T12:26:39Z"},{"alias_kind":"pith_short_16","alias_value":"QGY23GIY35TL5FRL","created_at":"2026-05-18T12:26:39Z"},{"alias_kind":"pith_short_8","alias_value":"QGY23GIY","created_at":"2026-05-18T12:26:39Z"}],"graph_snapshots":[{"event_id":"sha256:7b7577dcc158d8f40fc5ffff4c9afc1e8448f7cd44e3512d0ce5fbae040db111","target":"graph","created_at":"2026-05-18T04:26:22Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"Non-proportional response of the scintillation yield of NaI:Tl was measured using highly monochromatic synchrotron irradiation ranging from 9 to 100 keV. Special attention is paid to the X-ray escape peaks. They provide us additional information about non-proportional response in the range 0.9 to 12 keV. A rapid variation of the non-proportional response curve is observed near the Iodine K-electron binding energy. A dense sampling of data is performed around this energy and that data are used to apply a method, which we call K-dip spectroscopy. This method allows us to derive the electron resp","authors_text":"I.V. Khodyuk, P.A. Rodnyi, P. Dorenbos","cross_cats":["cond-mat.mtrl-sci","nucl-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2011-02-18T10:08:16Z","title":"Non-proportional scintillation response of NaI:Tl to low energy X-ray photons and electrons"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1102.3799","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:c975c59857af32bb22ba7b205e8c123db66f50eeacefbd48883b4dd08cda9852","target":"record","created_at":"2026-05-18T04:26:22Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"a232aaace3b29a0fc7afc9bc4782d6bc3ca5fdd04a134c2ade349702f3ce2d81","cross_cats_sorted":["cond-mat.mtrl-sci","nucl-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2011-02-18T10:08:16Z","title_canon_sha256":"b3ecca903cbe11af585a05a459bde17983953f535c3aecc853d1ba84061a8c0a"},"schema_version":"1.0","source":{"id":"1102.3799","kind":"arxiv","version":1}},"canonical_sha256":"81b1ad9918df66be962b0288d334ed32a1cd8534cf19efe0242e41a2f2479b76","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"81b1ad9918df66be962b0288d334ed32a1cd8534cf19efe0242e41a2f2479b76","first_computed_at":"2026-05-18T04:26:22.558731Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:26:22.558731Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"kSupxIY43/lB91PNjAP+kDnLtm16f9vVKCTAiao+ulP46XWJful/1FkAgjHQgSzMM1cOcyLn84b/pm86x0pGCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T04:26:22.559131Z","signed_message":"canonical_sha256_bytes"},"source_id":"1102.3799","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c975c59857af32bb22ba7b205e8c123db66f50eeacefbd48883b4dd08cda9852","sha256:7b7577dcc158d8f40fc5ffff4c9afc1e8448f7cd44e3512d0ce5fbae040db111"],"state_sha256":"57e79daaa15e750abfbcc5cc74acf104f8c19ec9f8d1d79f02ea06bd2c1395ea"}