Fig. 4.32 Solution of the laser differential equation for EMF strength (4.83): at representation in
the form of S E n
ð Þ ¼ E n = 1 þ T 1n G 00 E
2
n
À
Á
for the scaled value T 1n G 00 ¼ 0.01 k 0 ¼ T 1n G 00 ¼ 0.125,
2πν 0n ¼ 1, 1=T
0
OF
À
Á ¼ 0:1 for different values of the DC component of scaled pumping K ¼ 0.1 (a),
0.3 (b), 3.4 (c), 5.4 (d). Initial conditions at the above-mentioned equation solution are the
4.7 Solution of Nonlinear DE of Second Order for the Laser
195