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We find this claim to be invalid if corrected expressions for the contributions of the transition current to G_A^s and G_E^s are used. We show that, instead, it is the lowest-lying uuds\\bar{s} configuration with uuds subsystem of completely s"},"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":"1107.3072","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-07-15T14:24:01Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"ccef131e3e2ecf94e9a62608a8ae7bff5972551c7f3da726b6caa9142b6f2ff4","abstract_canon_sha256":"41bdb6aed6965b82a6845b3c46bb53e61a71ec7e664a0209c61f59016d8e4100"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:05:57.580423Z","signature_b64":"cQrWkxGMYcIuWzzQVesVvKlbDvxSVQthWZoyO5g8YcIpeS6XwWWyYjR9UhqT3NFEZPJWhD+8sxUT4Tdojjg/CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e8bb7749c9a819fb4492237946f93ef00b4ae98642d9c51b06f0ea754c151c15","last_reissued_at":"2026-05-18T04:05:57.579755Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:05:57.579755Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The strangeness form factors of the proton within nonrelativistic constituent quark model revisited","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Alvin Kiswandhi, Hao-Chun Lee, Shin Nan Yang","submitted_at":"2011-07-15T14:24:01Z","abstract_excerpt":"We reexamine, within the nonrelativistic constituent quark model (NRCQM), a recent claim that the current data on the strangeness form factors indicates that the uuds\\bar{s} component in the proton is such that the uuds subsystem has the mixed spatial symmetry [31]_X and flavor spin symmetry [4]_{FS}[22]_F[22]_S, with \\bar{s} in S state (configuration I). We find this claim to be invalid if corrected expressions for the contributions of the transition current to G_A^s and G_E^s are used. 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