Q-switched solid state pulsed laser with injection seeding and a gaussian output coupling mirror

Claim 2

In a pulsed laser system having a quantity of solid state light amplifying material positioned within a resonant cavity on an optical axis thereof between first and second mirrors in a manner that laser light oscillates between said mirrors through the light amplifying material, a laser output beam being directed through said second mirror and out of said resonant cavity, an optical arrangement comprising: means including a flashlamp directing a pulse of optical energy to said light amplifying material for exciting said light amplifying material to emit light, Q-switch means positioned along said optical axis between said light amplifying material and one of said first and second mirrors for controllably attenuating said emitted light passing therethrough, means illuminating said light amplifying material with a coherent beam of light from a source external to said resonant cavity for limiting operation of the laser system to a single longitudinal mode of said laser light, said second mirror having a partial reflectivity that varies as a substantially continuous smoothly varying function of radial position across a surface of said mirror, a maximum partial reflectivity occurring substantially coincident with said optical axis at a center of the varying partial reflectivity function, thereby providing partial transmission of laser light therethrough out of said resonant cavity as the pulsed laser output beam, and the relative curvature of said first and second mirrors and the optical characteristics of other elements in the resonant cavity being chosen to cause a diameter of the laser light returning to the second mirror to be greater than the diameter of the light reflected from the second mirror by a magnification ratio that is in excess of substantially 1.3.

Claim 3

The pulsed laser optical arrangement according to claim 1 wherein the partial reflectivity function across said second mirror is such that when Fourier analyzed in terms of spatial frequencies, its spatial frequency spectrum contains substantially no spatial frequencies higher in value than a reciprocal of the transverse size of said reflectivity profile, thereby avoiding high frequency modulation across the output laser beam.

Claim 4

The pulsed laser optical arrangement according to claim 2 wherein said second mirror includes a substrate and a dielectric material layer carried thereby that is characterized by a profile having a maximum thickness at the center of said varying partial reflectivity function and a gradually decreasing thickness at radial positions removed from said center.

Claim 5

The pulsed laser optical arrangement according to claim 1 wherein the partial reflectivity function across said second mirror substantially corresponds to a mathematical Gaussian function.

Claim 6

The pulsed laser optical arrangement according to claim 1 wherein said second mirror includes a substrate and a dielectric material layer carried thereby that is characterized by a profile having a maximum thickness at the center of said varying partial reflectivity function and a gradually decreasing thickness at radial positions removed from said center.

Claim 7

The pulsed laser optical arrangement according to any of claims 1-5 wherein the maximum partial reflectivity of said second mirror is substantially less than 50 percent of the laser light incident thereon, substantially all of the remaining laser light incident thereon being transmitted through said second mirror and out of said resonant cavity as said output laser beam.

Claim 8

The pulsed laser optical arrangement according to any of claims 1-5 wherein the relative curvature of said first and second mirrors and the optical characteristics of other elements in the resonant cavity are additionally chosen to cause said magnification ratio to be within a range of substantially 1.3 to 2.2.

Claim 9

The pulsed laser optical arrangement according to any of claims 1-5 wherein said solid state light amplifying material is in the form of a cylindrically shaped rod having an axis substantially coincident with said resonant cavity axis and having a diameter that is substantially within a range of from 1.5 to 3.0 times the diameter of said second mirror within a circle of uniform reflectivity that is substantially the peak reflectivity divided by a square of the natural logarithm "e".

Claim 10

The pulsed laser optical arrangement according to any of claims 1-5 wherein said solid state light amplifying material is in the form of a cylindrically shaped rod having an axis substantially coincident with said resonant cavity axis and having a cross-sectional radius that is approximately 1.5 times a cross-sectional radius of the laser light beam therein from a peak intensity substantially at said cavity axis to an intensity that is approximately 1/e 2 of its peak intensity.

Claim 11

In a pulsed laser system that includes: a resonant cavity bounded by first and second mirrors and having an optical axis therebetween, said cavity being capable of supporting oscillations of laser light therein between said mirrors and directing a portion of the laser light out of the cavity as a pulsed laser output beam, a cylindrically shaped solid state rod of light amplifying material positioned within a resonant cavity and having an axis substantially coincident with said resonant cavity optical axis, a Q-switch positioned intermediate of said rod and one of the first and second mirrors along said optical axis, means for limiting said laser light oscillations within said resonant cavity to substantially a single longitudinal mode, and a flashlamp positioned to illuminate said rod with pulses of excitation radiation, an improvement limiting laser light oscillation within the cavity to substantially a single fundamental transverse mode and producing output laser light of substantially uniform cross-sectional intensity, comprising: said second mirror having a partial reflectivity that varies as a substantially continuous smoothly varying function of radial position across a surface of said mirror, a maximum partial reflectivity occurring substantially coincident with said optical axis at a center of the varying partial reflectivity function, thereby providing partial transmission of laser light therethrough out of said resonant cavity as the pulsed laser output beam, a relative curvature of said first and second mirrors, an optical characteristic of other elements in said cavity and the radially varying partial reflectivity function of the second mirror being such that (1) a diameter of the laser light returning to the second mirror is greater than the diameter of the light reflected from the second mirror by a magnification ratio lying substantially within a range of from 1.3 to 2.2, and (2) said rod has a diameter that is substantially within a range of from 1.5 to 3.0 times the diameter of said second mirror within a circle of uniform reflectivity that is substantially the peak reflectivity divided by a square of the natural logarithm "e", and the maximum partial reflectivity of said second mirror being substantially less than fifty percent and less than substantially the quantity one divided by the square of said magnification ratio, whereby the laser beam oscillating within said resonant cavity is limited to substantially a single fundamental transverse mode of said laser light, and said output beam is characterized by a substantially uniform cross-sectional intensity profile.

Claim 12

In a pulsed laser system that includes: a resonant cavity bounded by first and second mirrors and having an optical axis therebetween, said cavity being capable of supporting oscillations of laser light therein between said mirrors and directing a portion of the laser light out of the cavity as a pulsed laser output beam, a cylindrically shaped solid state rod of light amplifying material positioned within a resonant cavity and having an axis substantially coincident with said resonant cavity optical axis, a Q-switch positioned intermediate of said rod and one of the first and second mirrors along said optical axis, means for limiting said laser light oscillations within said resonant cavity to substantially a single longitudinal mode, and a flashlamp positioned to illuminate said rod with pulses of excitation radiation, an improvement limiting laser light oscillation within the cavity to substantially a single fundamental transverse mode and producing output laser light of substantially uniform cross-sectional intensity, comprising: said second mirror having a partial reflectivity that varies as a substantially continuous smoothly varying function of radial position across a surface of said mirror, a maximum partial reflectivity occurring substantially coincident with said optical axis at a center of the varying partial reflectivity function, thereby providing partial transmission of laser light therethrough out of said resonant cavity as the pulsed laser output beam, a relative curvature of said first and second mirrors, an optical characteristic of other elements in said cavity and the radially varying partial reflectivity function of the second mirror being such that (1) a diameter of the laser light returning to the second mirror is greater than the diameter of the light reflected from the second mirror by a magnification ratio lying substantially within a range of from 1.3 to 2.2, and (2) said rod has a diameter that is substantially within a range of from 1.5 to 3.0 times the diameter of said second mirror within a circle of uniform reflectivity that is substantially the peak reflectivity divided by a square of the natural logarithm "e", and the maximum partial reflectivity of said second mirror being substantially less than fifty percent and less than substantially the quantity one divided by the square of said magnification ratio, whereby the laser beam oscillating within said resonant cavity is limited to substantially a single fundamental transverse mode of said laser light, and said output beam is characterized by a substantially uniform cross-sectional intensity profile.