Laser diodes with phase conjugate feedback

Laser diodes with phase conjugate feedback Laser diodes with phase conjugate feedback

26.11.2014 Views

Risø National Laboratory Four-wave mixing operation in high power diodes 0 L The nonlinear polarization is given by P= ε χ( N) E nc where χ( N) =− ( β+i)g(N) , g(N)=a(N-N 0) ω Z R=R 1 Z=0 R=0 Gain and refractive index gratings A 1 A 3 Semiconductor amplifier A 2 Electrode 0 Z=L dA1 * * =−α0A1− γ( AA 1 4 + A2A3) A4 (1A) dz * dA2 * * * * =+ α0A2 − γ( AA 1 4 + A2A3) A3 (1B) dz dA3 * * =+ α0A3+ γ( AA 1 4 + A2A3) A2 (1C) dz * dA4 * * * * =− α0A4 + γ( AA 1 4 + A2A3) A1 (1D) dz (1 − iβ ) g0 α0 =− is the effective gain 2(1 + P ) P 0 = E 0 P s 2 0 0 is the average intercavity pump intensity 2C γ=-i α0 is the coupling factor 1+ P Paul Michael Petersen, Laser Diodes with External Feedback (tutorial)

Risø National Laboratory DFWM in diodes using total internal reflection 0 Gain and refractive index gratings A 1 High reflective coating Z=0 Semiconductor amplifier Electrode L Z A 3 A 2 Z=L Antireflection coating Spatial- and temporal filtering Output beam M Paul Michael Petersen, Laser Diodes with External Feedback (tutorial)

Risø National Laboratory<br />

Four-wave mixing operation in high power <strong>diodes</strong><br />

0<br />

L<br />

The nonlinear polarization is given by P=<br />

ε χ( N)<br />

E<br />

nc<br />

where χ( N) =− ( β+i)g(N) , g(N)=a(N-N<br />

0)<br />

ω<br />

Z<br />

R=R 1 Z=0<br />

R=0<br />

Gain and refractive<br />

index gratings<br />

A 1<br />

A 3<br />

Semiconductor<br />

amplifier<br />

A 2<br />

Electrode<br />

0<br />

Z=L<br />

dA1<br />

* *<br />

=−α0A1− γ( AA<br />

1 4<br />

+ A2A3) A4<br />

(1A)<br />

dz<br />

*<br />

dA2<br />

* * * *<br />

=+ α0A2 − γ( AA<br />

1 4<br />

+ A2A3) A3<br />

(1B)<br />

dz<br />

dA3<br />

* *<br />

=+ α0A3+ γ( AA<br />

1 4<br />

+ A2A3) A2<br />

(1C)<br />

dz<br />

*<br />

dA4<br />

* * * *<br />

=− α0A4 + γ( AA<br />

1 4<br />

+ A2A3) A1<br />

(1D)<br />

dz<br />

(1 − iβ<br />

) g0<br />

α0<br />

=− is the effective gain<br />

2(1 + P )<br />

P<br />

0<br />

=<br />

E<br />

0<br />

P<br />

s<br />

2<br />

0<br />

0<br />

is the average intercavity pump intensity<br />

2C<br />

γ=-i α0<br />

is the coupling factor<br />

1+<br />

P<br />

Paul Michael Petersen, <strong>Laser</strong> Diodes <strong>with</strong> External Feedback (tutorial)

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