Abstract

The strange-quark vector current form factors of the nucleon are analyzed within the framework of dispersion relations. Particular attention is paid to contributions made by KKˉK\bar{K} intermediate states to the form factor spectral functions. It is shown that, when the KKˉ→NNˉK\bar{K}\to N\bar{N} amplitude is evaluated in the Born approximation, the KKˉK\bar{K} contributions are identical to those arising from a one-loop calculation and entail a serious violation of unitarity. The mean square strangeness radius and magnetic moment are evaluated by imposing unitarity bounds on the kaon-nucleon partial wave amplitudes. The impact of including the kaon's form factor in the dispersion integrals is also evaluated.

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