{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:HQYYLVEAM3L6DZZPYGSOQRKJC5","short_pith_number":"pith:HQYYLVEA","schema_version":"1.0","canonical_sha256":"3c3185d48066d7e1e72fc1a4e84549177f2ee80be4f41c468779083fbaec6e24","source":{"kind":"arxiv","id":"1612.08959","version":2},"attestation_state":"computed","paper":{"title":"Radiative 3He-alpha reaction in Halo Effective Field Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.SR","hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"Akshay Vaghani, Gautam Rupak, Renato Higa","submitted_at":"2016-12-28T19:35:18Z","abstract_excerpt":"In this work we study the radiative capture of ${\\rm {}^3He}$ on ${\\rm {}^4He}$ within the halo effective field theory (EFT) framework. At leading order the capture amplitude comprises the initial state $s$-wave strong and Coulomb interactions summed to all orders. At the same order in the expansion, leading two-body currents contribute as well. We find delicate cancelations between the various contributions, and the two-body current contributions can be replaced by appropriately enhancing the asymptotic normalizations of the $^7$Be ground and first excited state wave functions. The next-to-le"},"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":"1612.08959","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-12-28T19:35:18Z","cross_cats_sorted":["astro-ph.SR","hep-ph","nucl-ex"],"title_canon_sha256":"56e88cbcfc640bd762be9df0e62e8b8c28a1bed01572a7d3d6a63dbf2e47235f","abstract_canon_sha256":"166b9db77d7c624b9228c4de92f81b6da45d898fed99db27a6343a2f505f5f57"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:14:57.228383Z","signature_b64":"vaiWl5GdYtve45AwuRvt/Use6ZTEbXPndpPiIPyfUm1ZloTSPrREL83drteuTBNyxyks/6EiAE2ETcGJIoslBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3c3185d48066d7e1e72fc1a4e84549177f2ee80be4f41c468779083fbaec6e24","last_reissued_at":"2026-05-18T00:14:57.227818Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:14:57.227818Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Radiative 3He-alpha reaction in Halo Effective Field Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.SR","hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"Akshay Vaghani, Gautam Rupak, Renato Higa","submitted_at":"2016-12-28T19:35:18Z","abstract_excerpt":"In this work we study the radiative capture of ${\\rm {}^3He}$ on ${\\rm {}^4He}$ within the halo effective field theory (EFT) framework. At leading order the capture amplitude comprises the initial state $s$-wave strong and Coulomb interactions summed to all orders. At the same order in the expansion, leading two-body currents contribute as well. We find delicate cancelations between the various contributions, and the two-body current contributions can be replaced by appropriately enhancing the asymptotic normalizations of the $^7$Be ground and first excited state wave functions. The next-to-le"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1612.08959","kind":"arxiv","version":2},"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":"1612.08959","created_at":"2026-05-18T00:14:57.227913+00:00"},{"alias_kind":"arxiv_version","alias_value":"1612.08959v2","created_at":"2026-05-18T00:14:57.227913+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1612.08959","created_at":"2026-05-18T00:14:57.227913+00:00"},{"alias_kind":"pith_short_12","alias_value":"HQYYLVEAM3L6","created_at":"2026-05-18T12:30:19.053100+00:00"},{"alias_kind":"pith_short_16","alias_value":"HQYYLVEAM3L6DZZP","created_at":"2026-05-18T12:30:19.053100+00:00"},{"alias_kind":"pith_short_8","alias_value":"HQYYLVEA","created_at":"2026-05-18T12:30:19.053100+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/HQYYLVEAM3L6DZZPYGSOQRKJC5","json":"https://pith.science/pith/HQYYLVEAM3L6DZZPYGSOQRKJC5.json","graph_json":"https://pith.science/api/pith-number/HQYYLVEAM3L6DZZPYGSOQRKJC5/graph.json","events_json":"https://pith.science/api/pith-number/HQYYLVEAM3L6DZZPYGSOQRKJC5/events.json","paper":"https://pith.science/paper/HQYYLVEA"},"agent_actions":{"view_html":"https://pith.science/pith/HQYYLVEAM3L6DZZPYGSOQRKJC5","download_json":"https://pith.science/pith/HQYYLVEAM3L6DZZPYGSOQRKJC5.json","view_paper":"https://pith.science/paper/HQYYLVEA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1612.08959&json=true","fetch_graph":"https://pith.science/api/pith-number/HQYYLVEAM3L6DZZPYGSOQRKJC5/graph.json","fetch_events":"https://pith.science/api/pith-number/HQYYLVEAM3L6DZZPYGSOQRKJC5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HQYYLVEAM3L6DZZPYGSOQRKJC5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HQYYLVEAM3L6DZZPYGSOQRKJC5/action/storage_attestation","attest_author":"https://pith.science/pith/HQYYLVEAM3L6DZZPYGSOQRKJC5/action/author_attestation","sign_citation":"https://pith.science/pith/HQYYLVEAM3L6DZZPYGSOQRKJC5/action/citation_signature","submit_replication":"https://pith.science/pith/HQYYLVEAM3L6DZZPYGSOQRKJC5/action/replication_record"}},"created_at":"2026-05-18T00:14:57.227913+00:00","updated_at":"2026-05-18T00:14:57.227913+00:00"}