Constraint on KK compositeness of the a 0 (980) and f 0 (980) resonances from their mixing intensity Structure of the a0(980) and f0 (980) resonances is investigated with the a0(980)-f0(980) mixing intensity from the viewpoint of compositeness, which corresponds to the amount of two-body states composing resonances as well as bound states. For this purpose we first formulate the a0(980)-f0(980) mixing intensity as the ratio of two partial decay widths of a parent particle, in the same manner as the recent analysis in BES experiments. Calculating the a0(980)-f0(980) mixing intensity with the existing Flatte parameters from experiments, we find that many combinations of the a0(980) and f0(980) Flatte parameters can reproduce the experimental value of the a0(980)-f0(980) mixing intensity by BES. Next, from the same Flatte parameters we also calculate the KK compositeness for a0(980) and f0(980). Although the compositeness with the correct normalization becomes complex in general for resonance states, we find that the Flatte parameters for f0(980) imply large absolute value of the KK compositeness and the parameters for a0(980) lead to small but nonnegligible absolute value of the KK compositeness. Then, connecting the mixing intensity and the KK compositeness via the a0(980)-and f0(980)-KK coupling constants, we establish a relation between them. As a result, a small mixing intensity indicates a small value of the product of the KK compositeness for the a0(980) and f0 (980) resonances. Moreover, the experimental value of the a0(980)-f0(980) mixing intensity implies that the a0(980) and f0 (980) resonances cannot be simultaneously KK molecular states.