{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:CEMEF2DUR36M2BEVPP5AYRX2IC","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":"9ca44277addfcf42337351236a81d4ee0b9b589bc22295d5df4cc10d4e09a952","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-08-18T19:05:21Z","title_canon_sha256":"10ec4cc7b2c69a10ad5728073a82496d51b18f0a051e761943a306df4cd21fb8"},"schema_version":"1.0","source":{"id":"1508.04411","kind":"arxiv","version":15}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1508.04411","created_at":"2026-05-18T01:17:11Z"},{"alias_kind":"arxiv_version","alias_value":"1508.04411v15","created_at":"2026-05-18T01:17:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.04411","created_at":"2026-05-18T01:17:11Z"},{"alias_kind":"pith_short_12","alias_value":"CEMEF2DUR36M","created_at":"2026-05-18T12:29:14Z"},{"alias_kind":"pith_short_16","alias_value":"CEMEF2DUR36M2BEV","created_at":"2026-05-18T12:29:14Z"},{"alias_kind":"pith_short_8","alias_value":"CEMEF2DU","created_at":"2026-05-18T12:29:14Z"}],"graph_snapshots":[{"event_id":"sha256:32f407fdf5373a12edce30cc06710ea0ec1d4a0a6545258213b301a116e2a31c","target":"graph","created_at":"2026-05-18T01:17:11Z","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":"The RSE Born Approximation is a new scattering formula in Physics, it allows the calculation of strong scattering at all frequencies via the Fourier transform of the scattering potential and Resonant-states. In this paper I apply the RSE Born Approximation to Schrodinger's equation. The resonant-states of the system can be calculated using the recently discovered RSE perturbation theory and correctly normalised to appear in spectral Green's functions via the flux-volume normalisation. In the limit of an infinite number of resonant states being used in the RSE Born Approximation basis the appro","authors_text":"M. B. Doost","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-08-18T19:05:21Z","title":"Resonant-state expansion Born Approximation with a correct eigen-mode normalisation applied to Schrodinger's equation or general wave equations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.04411","kind":"arxiv","version":15},"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:f23ccd9ba45311fbf7d644ddaf517978ffc7e0b71bee8691fc6f8e11af3cdd16","target":"record","created_at":"2026-05-18T01:17:11Z","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":"9ca44277addfcf42337351236a81d4ee0b9b589bc22295d5df4cc10d4e09a952","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-08-18T19:05:21Z","title_canon_sha256":"10ec4cc7b2c69a10ad5728073a82496d51b18f0a051e761943a306df4cd21fb8"},"schema_version":"1.0","source":{"id":"1508.04411","kind":"arxiv","version":15}},"canonical_sha256":"111842e8748efccd04957bfa0c46fa409899f14870f487d5acb8b39033de7760","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"111842e8748efccd04957bfa0c46fa409899f14870f487d5acb8b39033de7760","first_computed_at":"2026-05-18T01:17:11.606048Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:17:11.606048Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"fN9RJbjYCg6MC4Gc/fZ9M/f54SPHQ7dSBLymzvinap/zyKnPcBN4vPN9nyJCBawpPoMSFNUyEfvXuRkH+Q4fCA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:17:11.606769Z","signed_message":"canonical_sha256_bytes"},"source_id":"1508.04411","source_kind":"arxiv","source_version":15}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f23ccd9ba45311fbf7d644ddaf517978ffc7e0b71bee8691fc6f8e11af3cdd16","sha256:32f407fdf5373a12edce30cc06710ea0ec1d4a0a6545258213b301a116e2a31c"],"state_sha256":"90a2e0bdbc8e3184d8e7060ee2112d77ae043761a43f1918946283a93d4304a5"}