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The renormalized charge in noncompact lattice QED with staggered fermions is calculated using simulation data for ( W y ) and (F$) as input. One outcome is that the charge vanishes in the infinite-cutoff limit for all values of the bare charge up to and including the chiral-phasetransition point. The analysis suggests that the scaling region of the latter is describable by an effective action containing Yukawa as well as gauge interactions.

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