Consider a perturbation that oscillates sinusoidally in time. This is usually called a harmonic perturbation. Thus,
where is, in general, a function of position, momentum, and spin operators.
Let us initiate the system in the eigenstate of the unperturbed Hamiltonian, , and switch on the harmonic perturbation at . It follows from Equation (796) that
This formula is analogous to Equation (803), provided that
Thus, it follows from the analysis of Section 8.6 that the transition probability is only appreciable in the limit if
Clearly, (855) corresponds to the first term on the right-hand side of Equation (851), and (856) corresponds to the second term. The former term describes a process by which the system gives up energy to the perturbing field, while making a transition to a final state whose energy level is less than that of the initial state by . This process is known as stimulated emission. The latter term describes a process by which the system gains energy from the perturbing field, while making a transition to a final state whose energy level exceeds that of the initial state by . This process is known as absorption. In both cases, the total energy (i.e., that of the system plus the perturbing field) is conserved.
By analogy with Equation (816),
Equation (857) specifies the transition rate for stimulated emission, whereas Equation (858) gives the transition rate for absorption. These equations are more usually written
It is clear from Equations (852)-(853) that . It follows from Equations (857)-(858) that
In other words, the rate of stimulated emission, divided by the density of final states for stimulated emission, equals the rate of absorption, divided by the density of final states for absorption. This result, which expresses a fundamental symmetry between absorption and stimulated emission, is known as detailed balancing, and is very important in statistical mechanics.
- Richard Fitzpatrick (Professor of Physics, The University of Texas at Austin)