The stimulated emission from an atom interacting with radiation in non-equilibrium state is considered. The stochastic limit, applied to the non-relativistic Hamiltonian describing the interaction, shows that the state of atoms, driven by some non-equilibrium state of the field approaches a stationary state which can continuously emit photon, unlike the case with an equilibrium state.Einstein applied Planck's radiation theory to describe the equilibrium state between a atom and field [1]. He perceived that such an equilibrium state can be realized through the detailed balance condition, i.e. the balance in each mode between spontaneous and "stimulated emission", i.e. the emission from the atom stimulated by the field. Einstein's investigation can be said to give the clearest insight into the origin of Planck's radiation because, with this notion, we can understand the Planck's law on the density of states of the photons from an equilibrium field, i.e.On the other hand, with the development of technology, a controlled emission with a controlled stimulating field has been realized in experimental situation, for example, a laser system. A laser is often described in terms of stimulated emission from an equilibrium state at negative temperature [2]. However the concept of the negative temperature can't be accepted literally, but rather as an expediency to understand an inverse population state of the atoms which can emit photons. More precisely, a laser should be considered as a stimulated emission due to a non-equilibrium state of a field. In this letter we propose a way to understand such kind of stimulated emissions from non-equilibrium states, without introducing any phenomenological expediency like a negative temperature.We apply the stochastic limit [3] to the non-relativistic QED Hamiltonian and derive two types of equations: one is the so-called rate equation for the atom and the other is an equation describing the time evolution of the number of photons. In addition, based on these equations, we discuss the stimulated emission from the atom interacting with some non-equilibrium field. The state of an atom driven by the non-equilibrium state of the field approaches a stationary state which can continuously emit photon, unlike the case of the equilibrium field. The conditions of the non-equilibrium state of the field for such phenomena is also made clear.We shall consider an atom interacting with the EM-filed described with the standard non-relativistic QED Hamiltonianwhere