{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:AN7B47KVJMGSCK4KWZJ7J2FP4T","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":"dd80418ebe6376b2e677ff8c3ec137c3cc358815a4b3e3aa60d54458922444e4","cross_cats_sorted":["physics.comp-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-03-26T11:31:56Z","title_canon_sha256":"f2745c42e55272eb73b8f0cec4dfa4193ad5744786df9eb1dbc59dbab437ecc4"},"schema_version":"1.0","source":{"id":"1303.6439","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.6439","created_at":"2026-05-18T02:27:19Z"},{"alias_kind":"arxiv_version","alias_value":"1303.6439v2","created_at":"2026-05-18T02:27:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.6439","created_at":"2026-05-18T02:27:19Z"},{"alias_kind":"pith_short_12","alias_value":"AN7B47KVJMGS","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_16","alias_value":"AN7B47KVJMGSCK4K","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_8","alias_value":"AN7B47KV","created_at":"2026-05-18T12:27:38Z"}],"graph_snapshots":[{"event_id":"sha256:f3dee3f66d24feda767c5d034682e341aeb7beb8820a30e233c5dfb18d93ceec","target":"graph","created_at":"2026-05-18T02:27:19Z","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 complex scaling method, which consists in continuing spatial coordinates into the complex plane, is a well-established method that allows to compute resonant eigenfunctions of the time-independent Schroedinger operator. Whenever it is desirable to apply the complex scaling to investigate resonances in physical systems defined on numerical discrete grids, the most direct approach relies on the application of a similarity transformation to the original, unscaled Hamiltonian. We show that such an approach can be conveniently implemented in the Daubechies wavelet basis set, featuring a very pr","authors_text":"Alessandro Cerioni, Ivan Duchemin, Luigi Genovese, Thierry Deutsch","cross_cats":["physics.comp-ph","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-03-26T11:31:56Z","title":"Accurate Complex Scaling of Three Dimensional Numerical Potentials"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.6439","kind":"arxiv","version":2},"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":"sha256:38276a406d90b490e103d934fd80788d45d9d6ac35dc56d1bb10c1029fe52640","target":"record","created_at":"2026-05-18T02:27:19Z","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":"dd80418ebe6376b2e677ff8c3ec137c3cc358815a4b3e3aa60d54458922444e4","cross_cats_sorted":["physics.comp-ph","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2013-03-26T11:31:56Z","title_canon_sha256":"f2745c42e55272eb73b8f0cec4dfa4193ad5744786df9eb1dbc59dbab437ecc4"},"schema_version":"1.0","source":{"id":"1303.6439","kind":"arxiv","version":2}},"canonical_sha256":"037e1e7d554b0d212b8ab653f4e8afe4cb297acdbbbeaa5631df35e8d3b0efa4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"037e1e7d554b0d212b8ab653f4e8afe4cb297acdbbbeaa5631df35e8d3b0efa4","first_computed_at":"2026-05-18T02:27:19.107759Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:27:19.107759Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"tVIr97MugRbFEdzBVPJ54udgnWGIECI0iMt6tyAERlR/Sx6Tgcr/fc4OEMc5TazJvA/Cw5OjnH9qkgLPdZrmBg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:27:19.108482Z","signed_message":"canonical_sha256_bytes"},"source_id":"1303.6439","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:38276a406d90b490e103d934fd80788d45d9d6ac35dc56d1bb10c1029fe52640","sha256:f3dee3f66d24feda767c5d034682e341aeb7beb8820a30e233c5dfb18d93ceec"],"state_sha256":"b70f0b05a0c9fa20e5fe509a253a383d5a44df34dc1ed0ef5a87119d9b11b0be"}