Laser diode end pumped Nd:YAG single mode laser
AssigneeLightwave Electronics Corporation
InventorsDavid G. Scerbak, Leonard P. Pearson
Life of this patent
Estimating the term…
Abstract
A diode pumped Nd:YAG laser is disclosed. The YAG rod is coated on its ends to define an optical resonator containing the YAG rod. The YAG rod is made sufficiently short, i.e., 1 mm, so that it will support only two axial resonant (lasing) modes. The rod is transversely stressed to polarize the two original modes and to excite a third lasing mode orthogonally polarized to the first two modes. The third mode is separated from the first two modes to provide stable, single mode TEM.sub.001 output. The transverse stress is applied by means of a spring clamp made of a material, Be-Cu, having a low temperature coefficient.
Claims15
In a method for producing single-mode, linearly polarized, coherent radiation at optical wavelengths, the steps of:
- generating a beam of coherent optical pumping radiation from a diode laser;
- directing the beam of optical pumping radiation through a solid member of generally non-birefingent lasant material to optically pump said member of lasant material and to provide a gain bandwidth having a characteristic peaked gain curve;
- disposing said member of lasant material within an optical resonator having an optical axis passing through the member of lasant material for exciting a plurality of resonant axial modes of said optical resonator with coherent optical radiation at a plurality of optical wavelengths;
- dimensioning the optical path length of the optical resonator to be sufficiently short such that essentially only two adjacent non-polarized optical resonant axial modes of said resonator will lase when centered in frequency on opposite sides of the peak of the gain curve within the optical resonator containing the optically pumped member of lasant material;
- and
- stressing the member of lasant material to produce therein a stress with a predominant component transverse to the optical axis of the optical resonator to produce a stress related birefringence of said lasant material causing linear polarization of the two excited axial modes of the optical resonator along an axis normal to the direction of the stress in the member of lasant material and to produce a third excited axial mode of optical resonance of said optical resonator, said third mode of resonance being linearly polarized parallel to the direction of the applied stress and having a resonant optical wavelength inbetween the optical wavelengths of said first two excited optical resonant modes, whereby the energy of the third excited optical mode can be separated by a polarization sensitive device from the energy of the first two excited optical modes to produce a single-mode linearly polarized output.
In a laser apparatus for producing single-mode linearly polarized, coherent radiation at optical wavelengths:
- a laser diode for generating a beam of coherent optical pumping radiation;
- an optical resonator having an optical axis therein;
- a solid member of generally non-birefringent lasant material disposed within said optical resonator on the optical axis of said resonator;
- means for directing the beam of optical pumping radiation into said solid member of lasant material as disposed within said optical resonator for optically pumping same to produce an optical gain bandwidth having a characteristic peaked gain curve and for exciting a plurality of resonant axial modes of said optical resonator with coherent, optical radiation at a plurality of optical wavelengths;
- said optical resonator being dimensioned to be sufficiently short such that the optical path length within said optical resonator and through said solid member of lasant material is such that essentially only two non-polarized adjacent optically resonant, axial modes of said resonator will lase when centered in frequency on opposite sides of the peak of the gain curve within the optical resonator containing said optically pumped member of lasant material;
- and
- means for stressing said member of lasant material to produce therein a stress with a predominant component transverse to the optical axis of said optical resonator to produce a stress related birefringence of said lasant material causing linear polarization of the two excited axial modes of said optical resonator along an axis normal to the direction of the stress in said member of lasant material and to produce a third excited axial mode of optical resonance of said optical resonator, said third mode of resonance being linearly polarized parallel to the direction of the applied stress and having a resonant optical wavelength inbetween the optical wavelengths of said first two excited optical resonant modes, whereby the energy of the third excited optical resonant mode can be separated by a polarization sensitive device from the energy of the first two excited optical modes to produce a single-mode, linearly polarized output.
In a laser apparatus for producing linearly polarized coherent radiation at optical wavelengths:
- means for generating a beam of coherent optical pumping radiation;
- an optical resonator having an optical axis therein;
- a solid member of generally non-birefringent lasant material disposed within said optical resonator on the optical axis of said resonator;
- means for directing the beam of optical pumping radiation into said solid member of lasant material as disposed within said optical resonator for optically pumping said solid member of lasant material;
- clamp means for stressing said member of lasant material to produce therein a stress related birefringence;
- and
- said clamp means including means for contacting one side of said solid member of lasant material along a pair of parallel relatively closely spaced lines of contact and including means for contacting said solid member of lasant material along a third line of contact generally diametrically opposed to said first two lines of contact and said third line of contact being generally parallel to said first two lines of contact, whereby the lasant material is transversely stressed to produce the stress-related birefringence therein.
Dependencies are inferred from the claim text.