An isotropic tensor has unchanged components under every proper orthogonal change of basis: for every . Orthogonality gives , so the Kronecker delta is isotropic. The determinant identity gives , so the Levi-Civita symbol is isotropic too. If reflections are included, this last object is a pseudotensor: it changes sign. The question's isotropy convention therefore refers to proper rotations.
For the sphere moment , change variables to . Rotations preserve the sphere and its area measure; inserting the component transformation proves that is an isotropic tensor. For the second moment, half-turns about coordinate axes kill the off-diagonal components, while rotations interchanging axes make the diagonal entries equal. Thus it is a multiple . Contracting the indices gives . Odd moments vanish by , including the third moment. The supplied general fourth-rank form and symmetry under every permutation of the four indices make its three coefficients equal. A double contraction then gives . ThusTo explain the weighted volume integrals, put ; its bilinear square is , without complex conjugation. Separating radial and angular factors givesFor the angular factor is . For it is zero by oddness. For it is . Therefore all three requested integrals vanish, assuming the radial integrals exist. More generally the null-vector cancellation of radial moments follows from rotation about the third axis, which multiplies the integral by without otherwise changing it.
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