Background
Laser models have been developed for the past five decades and can be classified in large categories under the headings: "quantum mechanical models", "statistical models", "electrodynamical models" (so-called Maxwell-Bloch), "heuristic models" (typically rate-equations-based).
All have their merits and aim at answering specific questions -- for instance, statistical models provide information on fluctuations, while heuristic models aim at predicting laser behaviour with minimal effort (for applications).
Nanolasers have proven to be rather impervious to effective modeling. Rate-equations-based ones tend to provide wrong or ineffectual answers due to the strong role played by fluctuations, while more fundamental models require a substantial amount of work, difficult to carry out far from the thermodynamic limit.
This way, we have constructed a laser automaton which computes the evolution of the laser's intracavity photon number (spontaneous or stimulated) together with the population evolution.
This procedure is fast (1 ns of experimental time predicted in a few seconds of computing time), and provides the following information:
intrinsic fluctuations -- with no additional hypotheses;
probabilistic computation of the power output;
simulation of the detection process;
knowledge of off-axis spontaneous emission;
knowledge of on-axis spontaneous photons;
knowledge of stimulated photons (the last two can be added).
This detailed information allows for the computation of steady states, but also for fluctuations, correlations, etc.
[1] G.P. Puccioni and G.L. Lippi, Stochastic Simulator for modeling the transition to lasing, Optics Express 23 (3), 2369 (2015).
Stochastic Simulator
We have developed a Stochastic Simulator [1], which numerically predicts the behaviour of a laser starting from a semi-classical description of the physical processes (rather than their analytical representation). The computer is given the probabilistic rules pertaining to the absorption (by a two-level system), spontaneous and stimulated emission, as well as the probabilities for photon reflection and transmission by the laser cavity.