Numeric solution to the laser rate equations - An example

Steady State Solution

A numeric solution to the rate equations can easily be obtained under steady state conditions as all parameters can be calculated from the carrier density in a straight forward way.

Starting from a set of values for the carrier density one first calculates the gain at each of those densities. If the gain is linear with the carrier density the gain is obtained from:

We will use this expression in this example. Other expressions for the gain can be used as well.

The rate equation for the photon density can be solved yielding:

from which the photon density corresponding to each value of the carrier density can be calculated. The output power of the laser at the mirror with reflectivity R1 is then obtained using: Finally one finds the current through the laser from: The P-I curve of the laser can now be plotted, simply by plotting the values of the output power as a function of the values of the laser current. Show below is the P-I curve on a linear and semi-logarithmic scale for a typical GaAs/AlGaAs edge-emitting single-quantum-well laser. The values for all the laser parameters and the material constants are summarized in the table.

Laser and material parameters
Cavity lengthL300 mm
Laser widthW3 mm
Laser areaA = L x W9 x 10-6 cm2
Non-radiative recombination timetnr100 ns
Bimolecular recombination constantb5 x 10-5 cm2/s
Auger recombination constantc6.25 x 10-18 cm4/s
Group velocityvgr9 x 109 cm/s
Confinement factorG0.02
Differential gain1.23 x 10-9 cm
Transparency carrier densityNtr1.23 x 1012 cm-2
Spontaneous emission factorb10-5
Photon lifetimetph2.58 ps
Mirror #1 reflectivityR10.3
Mirror #2 reflectivityR10.3
Photon energyhn1.49 eV
Lasing wavelengthl830 nm
Waveguide lossesa3 1/cm
Calculated values
Threshold carrier densityN02.99 x 1012 cm-2
Threshold currentIth0.68 mA
Modal gain at thresholdg(N0)43 1/cm
Differential efficiency0.47 mW/mA

rateeq.xls - lasrate.gif


rateeq.xls - lasrate1.gif