Laser diode end pumped Nd:YAG single mode laser

Claim 2

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.

Claim 3

The method of claim 1 including the step of directing the beam of optical pumping radiation into the member of lasant material along an axis generally collinear with the optical axis of the optical resonator containing the member of lasant material, whereby conversion efficiency is increased.

Claim 4

The method of claim 1 including the step of making the member of solid lasant material of a material selected from the group consisting of Nd:YAG and Nd:doped glass.

Claim 5

The method of claim 1 including the step of: directing energy of the first two and the third excited resonant modes of the optical resonator into a polarization sensitive separator for separating the energy of the first two resonant modes from that of the third resonant mode.

Claim 6

The method of claim 1 wherein the step of stressing the solid member of lasant material includes a step of adjusting the stress so that the wavelength of the third resonant mode is generally midway between the wavelengths of the first two excited resonant modes.

Claim 7

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.

Claim 8

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.

Claim 9

The laser apparatus of claim 6 wherein said means for directing the beam of optical pumping radiation into the member of lasant material directs the beam of pumping radiation along an axis generally collinear with the optical axis of the optical resonator containing said member of lasant material, whereby the conversion efficiency of the laser apparatus is increased.

Claim 10

The laser apparatus of claim 6 wherein the member of solid lasant material is selected from the group consisting of Nd:YAG and Nd:doped glass.

Claim 11

The laser apparatus of claim 6 including polarization sensitive separator means disposed to receive energy of the first two and third excited resonant modes of said optical resonator for separating the energy of the first two resonant modes from that of the third resonant mode.

Claim 12

The laser apparatus of claim 6 wherein said means for stressing said solid member of lasant material includes means for adjusting the stress so that the wavelength of the third resonant mode can be adjusted to be generally midway between the wavelengths of the first two excited resonant modes.

Claim 13

The laser apparatus of claim 6 wherein said means for stressing said member of lasant material includes a clamp structure, said clamp structure being made of beryllium copper such that the stress exerted on the member of solid lasant material is rendered generally insensitive to temperature fluctuations.

Claim 14

The laser apparatus of claim 6 wherein said optical resonator has a length along its optical axis less than two millimeters.

Claim 15

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.

Claim 16

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.

Claim 17

The apparatus of claim 13 wherein said clamping means includes a first bore therein to coaxially receive said solid lasant material and said clamping means including a relief bore parallel to and intersecting with said first bore such that the intersecting corners of the first bore and said relief bore define said first and second parallel lines of contact with said solid lasant material.

Claim 18

The apparatus of claim 14 wherein said clamp means includes a cantilever portion disposed substantially tangent to said first bore and bearing along a line of tangency on said solid member of lasant material for defining said third line of contact and for applying the stress to said solid member of lasant material.