<p dir="ltr">These figures illustrate the the process of detailed balance in terms of elementary transitions.</p><p dir="ltr">Figure 1, illustrates the idea of using a composite Hilbert space to describe the time-evolution of a system. The first Hilbert space represents the original system at the current moment in time. The second copy in the tensor product represents the system at the next moment in time.</p><p dir="ltr">Figure 2, illustrates the use of pure states kappa<sub>(i</sub><sub>,j</sub><sub>)</sub> on the composite system as elementary transitions in the classical case. Here kappa<sub>(i</sub><sub>,j)</sub> represents the transition from the pure state i to the pure state j. The term kappa<sub>(j,i)</sub> represents the reverse elementary transition from j to i<sub><em> </em></sub><i>.</i></p><p dir="ltr">Figure 3, illustrates that for a system satisfying elementary transition detailed balance (ETDB), each elementary transition kappa<sub>alpha</sub> will necessarily have a corresponding reverse elementary transition R(kappa<sub>alpha</sub>). Likewise, the term kappa<sub>beta</sub> = R(kappa<sub>alpha</sub>) will have a corresponding reverse, namely R(kappa<sub>beta</sub>) = kappa<sub>alpha</sub>. This takes into account that the operator R is its own inverse.</p>