Here we investigate an optical counterpart of the quantum Hanle effect. By employing the concepts of nonhermitian quantum mechanics 7,8 , we have designed an artificial plasmonic "atom" which has a pair of degenerate resonances that split by 3 broken time-reversal symmetry due to the presence of loss. This is a complete optical analogue of the atomic system where initially degenerate atomic states are split when the time-reversal symmetry is broken by the magnetic field 1 . Twodimensional (2D) arrays of these particles can form a new artificial material (metamaterial) with extremely efficient optical activity.Metamaterials provide vast opportunities to manipulate light beams in an uncommon way 11 , promising a wide range of potential applications such as cloaking 12,13 and perfect lensing 14 based on negative index of refraction. In the optical range, the properties of metamaterials rely on plasmonic effects 11 . In this work we will employ the localized surface plasmon (LSP) resonances supported by metal nanoparticles made of noble metals 15 . These resonances are solely determined by the particle's shape and surrounding environment and can be engineered and tuned to the desired frequency [16][17][18] .The basic scheme of the Hanle effect is represented in Fig. 1(a-b). Linearly polarized light, being a superposition of left and right circular polarizations, excites coherently the p-orbitals of an atom, conserving the total angular momentum. The degeneracy between p-states [ Fig. 1(a)] could be removed by an applied static magnetic field [Fig 1(b)]. The excited p-states evolve in time with slightly dissimilar time constants, adding different phases for opposite circular polarizations and, as a consequence, resulting in polarization-unpreserved light scattering. The polarization of the scattered light depends then on the strength of the magnetic field. The plasmonic "atom level" diagram of our optical analogue is shown in Fig. 1(c-d)