The ground state properties of liquid ????????3 in the presence of magnetic field have been investigated. In our calculations, we have employed a variational many-body formalism using the Lennard-Jones and Aziz inter-atomic potentials. For this system, we have also computed the magnetization in magnetic fields up to 200 T. Our results show no ferromagnetic phase transition induced by the magnetic field. Here, a comparison has also been made between the results of the Lennard-Jones and Aziz potentials.
