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Both octet and decuplet degrees of freedom are included. We formulate a chiral expansion at the kinematic point $Q^2=-(M_{B_1}-M_{B_2})^2$, which can be conveniently accessed in lattice QCD. The two unknown low-energy constants at this point are constrained by lattice QCD simulation results for the $\\Sigma^-\\rightarrow n$ and $\\Xi^0\\rightarrow \\Sigma^+$ transition form factors. Hence we determ"},"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":"1508.06923","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2015-08-27T16:20:08Z","cross_cats_sorted":["hep-lat","hep-th"],"title_canon_sha256":"47cd2e1aca152be0f4f533bcaad0ae4755af05ba1551722a59caf80805cf1ffb","abstract_canon_sha256":"133e3e9624580a2b8eb4d06cde648d75ed9a069ef526ee6dd2b286d9e867b1b5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:28:46.585486Z","signature_b64":"vqKYhD/Rpi2RQDV6KTgiNY4oCl1YWdlFE/zn0bOs8q5R54y+K8ab5OCsMtVfWRe8P4G6FkbB/VZ7YzmIWuvdDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"96e5c54343194870875a3681964199f3eba7c8e7135c33927c35eb0d588b74e7","last_reissued_at":"2026-05-18T01:28:46.584881Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:28:46.584881Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"SU(3) breaking in hyperon transition vector form factors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"nucl-th","authors_text":"A.N. Cooke, A.W. Thomas, G. Schierholz, J.M. Zanotti, P.E.L. Rakow, P.E. Shanahan, R.D. Young, R. Horsley, Y. Nakamura","submitted_at":"2015-08-27T16:20:08Z","abstract_excerpt":"We present a calculation of the SU(3)-breaking corrections to the hyperon transition vector form factors to $\\mathcal{O}(p^4)$ in heavy baryon chiral perturbation theory with finite-range regularisation. Both octet and decuplet degrees of freedom are included. We formulate a chiral expansion at the kinematic point $Q^2=-(M_{B_1}-M_{B_2})^2$, which can be conveniently accessed in lattice QCD. The two unknown low-energy constants at this point are constrained by lattice QCD simulation results for the $\\Sigma^-\\rightarrow n$ and $\\Xi^0\\rightarrow \\Sigma^+$ transition form factors. 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