Abstract
If the deuteron were an elementary particle then the triplet np effective range would be approximately ZR(IZ), where R=4.31 F is the usual deuteron radius and Z is the probability of finding the deuteron in a bare elementary-particle state. This formula is model-independent, but has an error of the order of the range mπ1=1.41 F of the np force, so it becomes exact only in the limit of small deuteron binding energy, i.e., Rmπ1. The experimental value of the effective range is not of order R and negative, but rather of order mπ1 and positive, so Z is small or zero and the deuteron is mostly or wholly composite.

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