Module 8 : Laser- II
Lecture   : Rate equations for Lasers
The emitted photons are confined to a laser cavity to stimulate further emission from the excited atoms. Ruby laser works on the principle of a three level system. The pumping power required for such a system is very high because more than half of the ground state atoms have to be pumped into the upper level to achieve population inversion.
  \includegraphics{laser12.eps}
   
  A few additional points to be noted about the three level system are :
As $ N_m \simeq N_g = N/2$and $ N_m-N_g \ll N$, once the population inversion is achieved, the power required to maintain it is small.
   
$ u\rightarrow m$transition is generally radiationless, the energy being given away to the lattice.
   
As more than half of the atoms are to be raised to the level $ m$, the probability of spontaneous emission is also much higher.
   

Laser transition occurs from the metastable state to the lowest possible state which are well separated. This leads to low efficiency.