Motivated by the homometallic intertwining double-chain ferrimagnets A 3 Cu 3 ͑PO 4 ͒ 4 ͑A =Ca,Sr,Pb͒, we investigate the low-energy structure of their model Hamiltonian H = ͚ n ͓J 1 ͑S n:1 + S n:3 ͒ + J 2 ͑S n+1:1 + S n−1:3 ͔͒ · S n:2 , where S n:l stands for the Cu 2+ ion spin labeled l in the nth trimer unit, with particular emphasis on the range of bond alternation 0 Ͻ J 2 / J 1 Ͻ 1. Although the spin-wave theory, whether up to O͑S 1 ͒ or up to O͑S 0 ͒, claims that there exists a flatband in the excitation spectrum regardless of bond alternation, a perturbational treatment, as well as the exact diagonalization of the Hamiltonian, reveals its weak but nonvanishing momentum dispersion unless J 2 = J 1 or J 2 = 0. Quantum Monte Carlo calculations of the static structure factor further convince us of the low-lying excitation mechanism, elucidating similarities and differences between the present system and alternating-spin linear-chain ferrimagnets.