Abstract
where P denotes the four-momentum of the particle c. The expression (1) can be used only when c is spinless and for higher spins it should be modified appropriately, but in order to avoid inessential complications we shall confine ourselves to the spinless case. In a previous paper4l -to be referred to as I hereafter-it has been shown on the basis of a simple model that limf(~. P) =finite, ~ ... o (3)
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