{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:R7ORNQEXVY2OGOVMJL2BFA6ZTM","short_pith_number":"pith:R7ORNQEX","schema_version":"1.0","canonical_sha256":"8fdd16c097ae34e33aac4af41283d99b237769cb994cd0890fab311b52827a8b","source":{"kind":"arxiv","id":"1108.3292","version":1},"attestation_state":"computed","paper":{"title":"Asymptotic normalization of mirror states and the effect of couplings","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"F. M. Nunes, L. J. Titus, P. Capel","submitted_at":"2011-08-16T17:32:13Z","abstract_excerpt":"Assuming that the ratio between asymptotic normalization coefficients of mirror states is model independent, charge symmetry can be used to indirectly extract astrophysically relevant proton capture reactions on proton-rich nuclei based on information on stable isotopes. The assumption has been tested for light nuclei within the microscopic cluster model. In this work we explore the Hamiltonian independence of the ratio between asymptotic normalization coefficients of mirror states when deformation and core excitation is introduced in the system. For this purpose we consider a phenomenological"},"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":"1108.3292","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-08-16T17:32:13Z","cross_cats_sorted":[],"title_canon_sha256":"3c6a0408194bf86181d11b5aa6294d65cea64ce00ea8d85bc43ce41ddbf813cd","abstract_canon_sha256":"dd1626616a92fd06b55259f27ab9034e7ee517e5ac48c514fae790094049bded"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:00:53.185286Z","signature_b64":"rHT/wDlOfETmyUlQsV8A/v5rcX4H+Bjw6SVI2S4JaXlZkC+l88d3HiNosgndHA3B9W+qB9yvKNW83H2ClaPoCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8fdd16c097ae34e33aac4af41283d99b237769cb994cd0890fab311b52827a8b","last_reissued_at":"2026-05-18T02:00:53.184516Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:00:53.184516Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Asymptotic normalization of mirror states and the effect of couplings","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"F. M. Nunes, L. J. Titus, P. Capel","submitted_at":"2011-08-16T17:32:13Z","abstract_excerpt":"Assuming that the ratio between asymptotic normalization coefficients of mirror states is model independent, charge symmetry can be used to indirectly extract astrophysically relevant proton capture reactions on proton-rich nuclei based on information on stable isotopes. The assumption has been tested for light nuclei within the microscopic cluster model. In this work we explore the Hamiltonian independence of the ratio between asymptotic normalization coefficients of mirror states when deformation and core excitation is introduced in the system. For this purpose we consider a phenomenological"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1108.3292","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":"1108.3292","created_at":"2026-05-18T02:00:53.184639+00:00"},{"alias_kind":"arxiv_version","alias_value":"1108.3292v1","created_at":"2026-05-18T02:00:53.184639+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1108.3292","created_at":"2026-05-18T02:00:53.184639+00:00"},{"alias_kind":"pith_short_12","alias_value":"R7ORNQEXVY2O","created_at":"2026-05-18T12:26:41.206345+00:00"},{"alias_kind":"pith_short_16","alias_value":"R7ORNQEXVY2OGOVM","created_at":"2026-05-18T12:26:41.206345+00:00"},{"alias_kind":"pith_short_8","alias_value":"R7ORNQEX","created_at":"2026-05-18T12:26:41.206345+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/R7ORNQEXVY2OGOVMJL2BFA6ZTM","json":"https://pith.science/pith/R7ORNQEXVY2OGOVMJL2BFA6ZTM.json","graph_json":"https://pith.science/api/pith-number/R7ORNQEXVY2OGOVMJL2BFA6ZTM/graph.json","events_json":"https://pith.science/api/pith-number/R7ORNQEXVY2OGOVMJL2BFA6ZTM/events.json","paper":"https://pith.science/paper/R7ORNQEX"},"agent_actions":{"view_html":"https://pith.science/pith/R7ORNQEXVY2OGOVMJL2BFA6ZTM","download_json":"https://pith.science/pith/R7ORNQEXVY2OGOVMJL2BFA6ZTM.json","view_paper":"https://pith.science/paper/R7ORNQEX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1108.3292&json=true","fetch_graph":"https://pith.science/api/pith-number/R7ORNQEXVY2OGOVMJL2BFA6ZTM/graph.json","fetch_events":"https://pith.science/api/pith-number/R7ORNQEXVY2OGOVMJL2BFA6ZTM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/R7ORNQEXVY2OGOVMJL2BFA6ZTM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/R7ORNQEXVY2OGOVMJL2BFA6ZTM/action/storage_attestation","attest_author":"https://pith.science/pith/R7ORNQEXVY2OGOVMJL2BFA6ZTM/action/author_attestation","sign_citation":"https://pith.science/pith/R7ORNQEXVY2OGOVMJL2BFA6ZTM/action/citation_signature","submit_replication":"https://pith.science/pith/R7ORNQEXVY2OGOVMJL2BFA6ZTM/action/replication_record"}},"created_at":"2026-05-18T02:00:53.184639+00:00","updated_at":"2026-05-18T02:00:53.184639+00:00"}