Abstract
The baryon-antibaryon contributions to the K20K10 mass difference are studied in an extended fermion-loop model as a further consistency test of a current-current quark model. It is found that contributions arising from the parity-conserving weak Hamiltonian phenomenologically constructed of one-baryon octet matrix elements are negligible compared to the crude estimate of the K10 mass shift, Δ(mK10)=(2τs)cotδ00(mK2). Although the contribution to the K20 mass shift arising from the parity-violating weak Hamiltonian via an S-wave effective meson-baryon-baryon interaction turns out to be comparable to Δ(mK10) and negative, the extended loop model is not incompatible with present theoretical understanding of the K20K10 mass difference.