We perform a five-body calculation for pentaquark (q(4)(q) over bar) state of A(1405) as well as the three-body calculations for the ground state baryons and the A(1405), and two-body calculations for mesons. The hamiltonian, which reproduces reasonably well the energies of ground state baryons (N, Lambda, Sigma, Xi and Delta) and mesons (pi, K, rho, K*), includes kinetic energy of semi-relativistic form, linear confinement potential, and the simplest form of color-magnetic interaction with Gaussian form factor. Flavor symmetry breaking (m(s) > M-u,M- d) is taken into account. The energy calculated for (q(4)(q) over bar) state of Lambda(1405) is lower than the energy for the (q(3)) state. The present result suggests that the Lambda(1405) is a pentaquark-dominated state if the color-magnetic potential plays a leading role of the quark-quark and quark-antiquark interactions.