{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:2VST54PZSLDCPFHGNF2UM6HXYX","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":"28150e2d4a03fc4606d31255c540b3dd4eed289afe17714dcc4133a41907ea10","cross_cats_sorted":["nucl-th","physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2015-01-16T15:24:17Z","title_canon_sha256":"6b6cf2fa9b7a5b38038c25d0e60981a18549235e72a9ff74abe03a69716a4fdc"},"schema_version":"1.0","source":{"id":"1501.04011","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1501.04011","created_at":"2026-05-18T02:03:34Z"},{"alias_kind":"arxiv_version","alias_value":"1501.04011v2","created_at":"2026-05-18T02:03:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.04011","created_at":"2026-05-18T02:03:34Z"},{"alias_kind":"pith_short_12","alias_value":"2VST54PZSLDC","created_at":"2026-05-18T12:29:02Z"},{"alias_kind":"pith_short_16","alias_value":"2VST54PZSLDCPFHG","created_at":"2026-05-18T12:29:02Z"},{"alias_kind":"pith_short_8","alias_value":"2VST54PZ","created_at":"2026-05-18T12:29:02Z"}],"graph_snapshots":[{"event_id":"sha256:543975ad3a5dcc05067a4c1b67bba9ba3d4c13f86b0811a7845e3c9d61eb5320","target":"graph","created_at":"2026-05-18T02:03:34Z","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":"A complete and consistent inversion technique is proposed to derive an accurate interaction potential from an effective-range function for a given partial wave in the neutral case. First, the effective-range function is Taylor or Pad\\'e expanded, which allows high precision fitting of the experimental scattering phase shifts with a minimal number of parameters on a large energy range. Second, the corresponding poles of the scattering matrix are extracted in the complex wave-number plane. Third, the interaction potential is constructed with supersymmetric transformations of the radial Schr\\\"odi","authors_text":"Bikashkali Midya, Jean-Marc Sparenberg, J\\'er\\'emie Evrard, O. L. Ram\\'irez Su\\'arez, Sylvain Abramowicz","cross_cats":["nucl-th","physics.atom-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2015-01-16T15:24:17Z","title":"Supersymmetric inversion of effective-range expansions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.04011","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:b56918054f1843fcb6563b974b4d6334ea0daeda5f30dd8b2471c359f1d68600","target":"record","created_at":"2026-05-18T02:03:34Z","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":"28150e2d4a03fc4606d31255c540b3dd4eed289afe17714dcc4133a41907ea10","cross_cats_sorted":["nucl-th","physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2015-01-16T15:24:17Z","title_canon_sha256":"6b6cf2fa9b7a5b38038c25d0e60981a18549235e72a9ff74abe03a69716a4fdc"},"schema_version":"1.0","source":{"id":"1501.04011","kind":"arxiv","version":2}},"canonical_sha256":"d5653ef1f992c62794e669754678f7c5e819b7bd110e5255da858ab45b27347b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d5653ef1f992c62794e669754678f7c5e819b7bd110e5255da858ab45b27347b","first_computed_at":"2026-05-18T02:03:34.613382Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:03:34.613382Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PlAbARUJyMRGFsy4+vZ/dqmvni31GFAxtjCLNrbWkHdiqGJeak5WwaIAiPRCMO9P737snGHc7iVm4DtNULSEDg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:03:34.614131Z","signed_message":"canonical_sha256_bytes"},"source_id":"1501.04011","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b56918054f1843fcb6563b974b4d6334ea0daeda5f30dd8b2471c359f1d68600","sha256:543975ad3a5dcc05067a4c1b67bba9ba3d4c13f86b0811a7845e3c9d61eb5320"],"state_sha256":"196f78cff8d89ce7d482c4d05b4e859bc5308f19e39ac2b357403ae917b8d62c"}