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The connection between | r2 | and the size of the hadron is less direct for a particle in which the quarks contribute with opposite signs to the integrand of Eq. 3.20. Indeed, because r2 flips sign under charge conjugation, r2 =0 for a self-conjugate particle, such as π0. However, isospin invariance implies that the size of π0 is equal, up to small corrections, to the size of π±. For an electrically neutral, non-self-conjugate meson Mij̄, the sign of r2 is controlled by the lighter of the qi and q̄j. For example, r2 K0=-(0.077±0.010)fm2, as can be understood from the larger spatial extent of the d compared with the s̄, which results from the property that Mud
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