In this paper we study J-pairing Hamiltonian and find that the sum of eigenvalues of spin I states equals sum of norm matrix elements within the pair basis for four identical particles such as four fermions in a single-j shell or four bosons with spin l. We relate number of states to sum rules of nine-j coefficients. We obtained sum rules for nine-j coefficients (jj)J, (jj)K : I|(jj)J, (jj)K : I and (ll)J, (ll)K : I|(ll)J, (ll)K : I summing over (1) even J and even K, (2) even J and odd K, (3) odd J and odd K, and (4) both even and odd values for J and K, where j is a half integer and l is an integer.