{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:CHTBYZJGTJGR22M76OPDLV73Q3","short_pith_number":"pith:CHTBYZJG","schema_version":"1.0","canonical_sha256":"11e61c65269a4d1d699ff39e35d7fb86f99cd1b1f5891075ab8edd0e1785796b","source":{"kind":"arxiv","id":"1101.2106","version":1},"attestation_state":"computed","paper":{"title":"General integral relations for the description of scattering states using the hyperspherical adiabatic basis","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"physics.atm-clus","authors_text":"A. Kievsky, C. Romero-Redondo, CSIC, E. Garrido (IEM, Italy), Madrid), M. Viviani (INFN, P. Barletta (University College London, Pisa, UK)","submitted_at":"2011-01-11T12:00:41Z","abstract_excerpt":"In this work we investigate 1+2 reactions within the framework of the hyperspherical adiabatic expansion method. To this aim two integral relations, derived from the Kohn variational principle, are used. A detailed derivation of these relations is shown. The expressions derived are general, not restricted to relative $s$ partial waves, and with applicability in multichannel reactions. The convergence of the ${\\cal K}$-matrix in terms of the adiabatic potentials is investigated. Together with a simple model case used as a test for the method, we show results for the collision of a $^4$He atom o"},"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":"1101.2106","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atm-clus","submitted_at":"2011-01-11T12:00:41Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"c87171b420b56ee7722a8c435b11683130c71eb344765d04608ea00fcb05a6d4","abstract_canon_sha256":"ae98838448f0673e3be2023a1b4848aee7c45041f53681fbf713f8286003095a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:58:51.563434Z","signature_b64":"s6s3zUUxGDKA67EFDaQYyyWW1KbPBNqowsNxJ0HeszUSNXpGxttqeuwHUOtLWMRelw8UZ/kOm/NtYEjcFPk9Cw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"11e61c65269a4d1d699ff39e35d7fb86f99cd1b1f5891075ab8edd0e1785796b","last_reissued_at":"2026-05-18T03:58:51.562694Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:58:51.562694Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"General integral relations for the description of scattering states using the hyperspherical adiabatic basis","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"physics.atm-clus","authors_text":"A. Kievsky, C. Romero-Redondo, CSIC, E. Garrido (IEM, Italy), Madrid), M. Viviani (INFN, P. Barletta (University College London, Pisa, UK)","submitted_at":"2011-01-11T12:00:41Z","abstract_excerpt":"In this work we investigate 1+2 reactions within the framework of the hyperspherical adiabatic expansion method. To this aim two integral relations, derived from the Kohn variational principle, are used. A detailed derivation of these relations is shown. The expressions derived are general, not restricted to relative $s$ partial waves, and with applicability in multichannel reactions. The convergence of the ${\\cal K}$-matrix in terms of the adiabatic potentials is investigated. Together with a simple model case used as a test for the method, we show results for the collision of a $^4$He atom o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1101.2106","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"1101.2106","created_at":"2026-05-18T03:58:51.562792+00:00"},{"alias_kind":"arxiv_version","alias_value":"1101.2106v1","created_at":"2026-05-18T03:58:51.562792+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1101.2106","created_at":"2026-05-18T03:58:51.562792+00:00"},{"alias_kind":"pith_short_12","alias_value":"CHTBYZJGTJGR","created_at":"2026-05-18T12:26:26.731475+00:00"},{"alias_kind":"pith_short_16","alias_value":"CHTBYZJGTJGR22M7","created_at":"2026-05-18T12:26:26.731475+00:00"},{"alias_kind":"pith_short_8","alias_value":"CHTBYZJG","created_at":"2026-05-18T12:26:26.731475+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/CHTBYZJGTJGR22M76OPDLV73Q3","json":"https://pith.science/pith/CHTBYZJGTJGR22M76OPDLV73Q3.json","graph_json":"https://pith.science/api/pith-number/CHTBYZJGTJGR22M76OPDLV73Q3/graph.json","events_json":"https://pith.science/api/pith-number/CHTBYZJGTJGR22M76OPDLV73Q3/events.json","paper":"https://pith.science/paper/CHTBYZJG"},"agent_actions":{"view_html":"https://pith.science/pith/CHTBYZJGTJGR22M76OPDLV73Q3","download_json":"https://pith.science/pith/CHTBYZJGTJGR22M76OPDLV73Q3.json","view_paper":"https://pith.science/paper/CHTBYZJG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1101.2106&json=true","fetch_graph":"https://pith.science/api/pith-number/CHTBYZJGTJGR22M76OPDLV73Q3/graph.json","fetch_events":"https://pith.science/api/pith-number/CHTBYZJGTJGR22M76OPDLV73Q3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CHTBYZJGTJGR22M76OPDLV73Q3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CHTBYZJGTJGR22M76OPDLV73Q3/action/storage_attestation","attest_author":"https://pith.science/pith/CHTBYZJGTJGR22M76OPDLV73Q3/action/author_attestation","sign_citation":"https://pith.science/pith/CHTBYZJGTJGR22M76OPDLV73Q3/action/citation_signature","submit_replication":"https://pith.science/pith/CHTBYZJGTJGR22M76OPDLV73Q3/action/replication_record"}},"created_at":"2026-05-18T03:58:51.562792+00:00","updated_at":"2026-05-18T03:58:51.562792+00:00"}