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:
(le4a)The rate equation for the photon density can be solved yielding:
(le4)
(le3)
(le5)
| Laser and material parameters | ||
| Cavity length | L | 300 mm |
| Laser width | W | 3 mm |
| Laser area | A = L x W | 9 x 10-6 cm2 |
| Non-radiative recombination time | tnr | 100 ns |
| Bimolecular recombination constant | b | 5 x 10-5 cm2/s |
| Auger recombination constant | c | 6.25 x 10-18 cm4/s |
| Group velocity | vgr | 9 x 109 cm/s |
| Confinement factor | G | 0.02 |
| Differential gain | ![]() | 1.23 x 10-9 cm |
| Transparency carrier density | Ntr | 1.23 x 1012 cm-2 |
| Spontaneous emission factor | b | 10-5 |
| Photon lifetime | tph | 2.58 ps |
| Mirror #1 reflectivity | R1 | 0.3 |
| Mirror #2 reflectivity | R1 | 0.3 |
| Photon energy | hn | 1.49 eV |
| Lasing wavelength | l | 830 nm |
| Waveguide losses | a | 3 1/cm |
| Calculated values | ||
| Threshold carrier density | N0 | 2.99 x 1012 cm-2 |
| Threshold current | Ith | 0.68 mA |
| Modal gain at threshold | g(N0) | 43 1/cm |
| Differential efficiency | 0.47 mW/mA |