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[16] This number of excess pions is far smaller than the ∼0.2 obtained earlier [11]. Much of the difference is caused by the absence of Δ effects in our one-boson-exchange formulation and the presence of such, computed with a hard form factor in Ref. [11]. Recent electron-scattering data [V. V. Frolov et al., Phys. Rev. Lett. 82, 45 (1999)] show that the electromagnetic NΔ transition form factor falls rapidly with increasing momentum transfer, so that it could be more appropriate to use a soft form factor. Thus including no nuclear Δ's may be a better approximation than including huge amounts.
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[26] Previous work required momentum missing by nucleons to be carried only by excess nuclear pions, and this condition yields the momentum sum rule. However, vector mesons can carry a significant fraction of the nuclear plus momentum [G. A. Miller, Phys. Rev. C 56, R8 (1997)] so that the momentum sum rule need not be satisfied by nucleons and pions.
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