{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:6AKUDOLUDYE5QJ6PW6GBLXNHAJ","short_pith_number":"pith:6AKUDOLU","schema_version":"1.0","canonical_sha256":"f01541b9741e09d827cfb78c15dda7026152c8210f80b86bc828675e69eb9ddd","source":{"kind":"arxiv","id":"1701.07659","version":1},"attestation_state":"computed","paper":{"title":"Ab initio calculations for non-strange and strange few-baryon systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Winfried Leidemann","submitted_at":"2017-01-26T11:24:30Z","abstract_excerpt":"Concerning the non-strange particle systems the low-energy excitation spectra of the three- and four-body helium isotopes are studied. Objects of the study are the astrophysical $S$-factor $S_{12}$ of the radiative proton deuteron capture $d(p,\\gamma)^3$He and the width of the $^4$He isoscalar monopole resonance.Both observables are calculated using the Lorentz integral transform (LIT) method. The LIT equations are solved via expansions of the LIT states on a specifically modified hyperspherical harmonics (HH) basis. It is illustrated that at low energies such a modification allows to work wit"},"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":"1701.07659","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-01-26T11:24:30Z","cross_cats_sorted":[],"title_canon_sha256":"bc82fa6b5dfda5e2e244862e2fca6a1e34bb3a20a69b5ee4a3291f0bea1d9147","abstract_canon_sha256":"30b68a522f98507c39367d67757f84ccd193f44d893c920859365c717e08840e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:19:31.031151Z","signature_b64":"W/xBxlaXBREmJPK2CTLwUoN8HK9PTUREwG9ekBnNS+M0u5OW3xQrbma1WUvHL9o7IxDQeis9VMUdGMBlBGKyAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f01541b9741e09d827cfb78c15dda7026152c8210f80b86bc828675e69eb9ddd","last_reissued_at":"2026-05-18T00:19:31.030607Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:19:31.030607Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Ab initio calculations for non-strange and strange few-baryon systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Winfried Leidemann","submitted_at":"2017-01-26T11:24:30Z","abstract_excerpt":"Concerning the non-strange particle systems the low-energy excitation spectra of the three- and four-body helium isotopes are studied. Objects of the study are the astrophysical $S$-factor $S_{12}$ of the radiative proton deuteron capture $d(p,\\gamma)^3$He and the width of the $^4$He isoscalar monopole resonance.Both observables are calculated using the Lorentz integral transform (LIT) method. The LIT equations are solved via expansions of the LIT states on a specifically modified hyperspherical harmonics (HH) basis. It is illustrated that at low energies such a modification allows to work wit"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.07659","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":"1701.07659","created_at":"2026-05-18T00:19:31.030685+00:00"},{"alias_kind":"arxiv_version","alias_value":"1701.07659v1","created_at":"2026-05-18T00:19:31.030685+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.07659","created_at":"2026-05-18T00:19:31.030685+00:00"},{"alias_kind":"pith_short_12","alias_value":"6AKUDOLUDYE5","created_at":"2026-05-18T12:31:03.183658+00:00"},{"alias_kind":"pith_short_16","alias_value":"6AKUDOLUDYE5QJ6P","created_at":"2026-05-18T12:31:03.183658+00:00"},{"alias_kind":"pith_short_8","alias_value":"6AKUDOLU","created_at":"2026-05-18T12:31:03.183658+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/6AKUDOLUDYE5QJ6PW6GBLXNHAJ","json":"https://pith.science/pith/6AKUDOLUDYE5QJ6PW6GBLXNHAJ.json","graph_json":"https://pith.science/api/pith-number/6AKUDOLUDYE5QJ6PW6GBLXNHAJ/graph.json","events_json":"https://pith.science/api/pith-number/6AKUDOLUDYE5QJ6PW6GBLXNHAJ/events.json","paper":"https://pith.science/paper/6AKUDOLU"},"agent_actions":{"view_html":"https://pith.science/pith/6AKUDOLUDYE5QJ6PW6GBLXNHAJ","download_json":"https://pith.science/pith/6AKUDOLUDYE5QJ6PW6GBLXNHAJ.json","view_paper":"https://pith.science/paper/6AKUDOLU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1701.07659&json=true","fetch_graph":"https://pith.science/api/pith-number/6AKUDOLUDYE5QJ6PW6GBLXNHAJ/graph.json","fetch_events":"https://pith.science/api/pith-number/6AKUDOLUDYE5QJ6PW6GBLXNHAJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6AKUDOLUDYE5QJ6PW6GBLXNHAJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6AKUDOLUDYE5QJ6PW6GBLXNHAJ/action/storage_attestation","attest_author":"https://pith.science/pith/6AKUDOLUDYE5QJ6PW6GBLXNHAJ/action/author_attestation","sign_citation":"https://pith.science/pith/6AKUDOLUDYE5QJ6PW6GBLXNHAJ/action/citation_signature","submit_replication":"https://pith.science/pith/6AKUDOLUDYE5QJ6PW6GBLXNHAJ/action/replication_record"}},"created_at":"2026-05-18T00:19:31.030685+00:00","updated_at":"2026-05-18T00:19:31.030685+00:00"}