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While the sensitivity of the total width to $B_\\Lambda$ is small, the partial widths for decays into individual final states and the experimentally measured ratio $R=\\Gamma_{^3\\textrm{He}}/\\left(\\Gamma_{^3 \\text{He}}+\\Gamma_{pd}\\right)$ show a strong dependence. For the standard value $B_\\Lambda=(0.13\\pm 0.05)$ MeV, we find"},"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":"2007.10122","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2020-07-20T14:02:20Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"e5923d44b0384b5ee41b877bbedf2a41dad6911c0983d26000fa5388de6647c4","abstract_canon_sha256":"4423d3e23000547ec62883ace0fc422e0480509e8ce8cc70a8c18c0dbb24d3de"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:58:31.060583Z","signature_b64":"LHCerYNKM0fv1jG8OiDeyUin5UDuFwKXbp3UsLb75B11jcUPNCB1ezjNVI6u9Q+V3kxvnTUncRPlRqQj7HPRCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f9d4bd0c1da32bb5406844966aaef942688727b3665a4f69b6ff5ffc5f60f3d6","last_reissued_at":"2026-07-05T01:58:31.060082Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:58:31.060082Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Lifetime of the hypertriton","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"F. 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