De-tuned distributed feedback laser diode
A semiconductor laser that includes a feedback laser section and an amplifier section. The feedback laser section generates a laser beam that has a maximum intensity at a first wavelength. The amplifier section amplifies the laser beam into a high powered beam. The amplifier section is constructed to have a peak optical gain located at a second wavelength that is offset from the first wavelength. Offsetting the wavelength generated in the feedback laser section from the peak gain wavelength of the amplifier section will result in an output beam that has a much broader linewidth that the feedback section alone. The broader linewidth is relatively stable even when part of the light reflects back into the semiconductor laser.
1. A semiconductor laser, comprising:
a feedback laser section that generates a laser beam with a maximum intensity at a first wavelength; and,
an amplifier section that is externally coupled to said feedback laser section to amplify the laser beam and has a peak optical gain at a second wavelength that is offset from the first wavelength to broaden a line width of said laser beam, said amplifier section having a pair of tapered edges.
2. The semiconductor laser of claim 1 , wherein said feedback laser section includes a diffraction grating.
3. The semiconductor laser of claim 1 , wherein said feedback laser section includes a distributed feedback diffraction grating.
4. The semiconductor laser of claim 1 , wherein said feedback laser section includes a distributed Bragg reflector.
5. A semiconductor laser, comprising:
first means for generating a laser beam with a maximum intensity at a first wavelength; and,
second means for amplifying the laser beam, said second means having a peak optical gain at a second wavelength that is offset from the first wavelength to broaden a line width of said laser beam said second means including a pair of tapered edges.
6. The semiconductor laser of claim 5 , wherein said first means includes a diffraction grating.
7. The semiconductor laser of claim 5 , wherein said first means includes a distributed feedback diffraction grating.
8. The semiconductor laser of claim 5 , wherein said first means includes a distributed Bragg reflector.
9. A method for operating a semiconductor laser, comprising:
generating a laser beam with a maximum intensity at a first wavelength within a feedback laser section; and,
amplifying the laser beam with an amplifier section that is external to said feedback laser section and has a pair of tapered edges, the amplifier section has a peak optical gain at a second wavelength that is offset from the first wavelength to broaden a line width of the laser beam.
10. The method of claim 9 , wherein the first wavelength is defined by the grating period of a diffraction grating.