Suppression of relaxation oscillations in flashpumped, two-micron tunable solid state lasers

Claim 2

A solid state laser comprising: a laser cavity defined by a first reflective element and an output coupler reflective element to form a reflective path therebetween; a laser crystal disposed in said laser cavity, said laser crystal having a host material doped with preselected activator ions sufficient to produce a laser emission at a laser transition wavelength in a range of wavelengths between about 1.9 microns and about 2.1 microns when said laser crystal is optically excited to produce said laser emission; means for optically exciting said laser crystal to produce a pulse of laser emission in said range of wavelengths; means disposed in said laser cavity between said laser crystal and one of said reflective elements for tuning said laser emission to a desired laser transition wavelength in said range of wavelengths; first means oriented at Brewster's angle in said reflective path in said laser cavity for suppressing oscillation of undesired wavelengths within said laser cavity; and second means disposed in said reflective path for suppressing laser spiking in said laser cavity to enable said laser to emit through said output coupler reflective element a smooth, long pulse of laser emission without spiking at said desired laser transition wavelength.

Claim 3

The laser of claim 1 wherein said second means includes: a nonlinear crystal disposed in said reflective path for generating second harmonics of said desired laser transition wavelength to suppress laser spiking at said desired laser transition wavelength in said laser cavity; and means for tilting said nonlinear crystal to a proper phasematching angle for maximum second harmonic generation.

Claim 4

The laser of claim 2 wherein: said nonlinear crystal is a lithium iodate crystal.

Claim 5

The laser of claim 1 further including: aperture means disposed in said reflective path in said laser cavity for allowing said laser to operate only at the lowest order spatial transverse mode of the desired laser transition wavelength in said range of wavelengths.

Claim 6

The laser of claim 4 wherein said aperture means includes: an opaque element containing a hole disposed in said reflective path for only passing the lowest order spatial transverse mode of the desired laser transition wavelength therethrough.

Claim 7

The laser of claim 1 wherein said first means includes: at least one optical plate oriented at Brewster's angle on each side of said tuning means to suppress the oscillation of undesired laser transition wavelengths within said laser cavity, said at least one optical plate being transparent to laser emission over said range of wavelengths.

Claim 8

The laser of claim 1 wherein said first means includes: first and second sets of optical plates oriented at Brewster's angle and respectively disposed on opposite sides of said tuning means to suppress the oscillation of undesired wavelengths within said laser cavity, said optical plates being transparent to laser emission over said range of wavelengths.

Claim 9

The laser of claim 7 wherein: said optical plates are comprised of material selected from the group consisting of calcium fluoride, fused silica and barium fluoride.

Claim 10

The laser of claim 1 wherein said first means comprises: Brewster-cut end faces on said laser crystal.

Claim 11

The laser of claim 1 wherein: said laser crystal has Brewster-cut end faces for further suppressing the oscillation of undesired laser transition wavelengths within said laser cavity.

Claim 12

The laser of claim 1 wherein said tuning means includes: a tuning element; and means for rotating said tuning element about its optic axis to tune said laser emission to a different laser transition wavelength within said range of wavelengths.

Claim 13

The laser of claim 11 wherein said second means includes: a nonlinear crystal disposed in said reflective path for generating second harmonics of said desired laser transition wavelength to suppress laser spiking at said desired laser transition wavelength in said laser cavity; and means for tilting said nonlinear crystal to a proper phasematching angle for maximum second harmonic generation.

Claim 14

The laser of claim 12 wherein: said nonlinear crystal is a lithium iodate crystal.

Claim 15

The laser of claim 11 wherein said tuning element includes: a stack of birefringent plates oriented at Brewster's angle to the direction of propagation of said laser emission.

Claim 16

The laser of claim 14 wherein: said birefringent plates have predetermined thicknesses, with the thicker ones of said birefringent plates having integer multiples of the thickness of the thinnest said birefringent plate.

Claim 17

The laser of claim 11 wherein said tuning element includes: at least one birefringent plate oriented at Brewster's angle to the direction of propagation of said laser emission.

Claim 18

The laser of claim 16 wherein: said at least one birefringent plate has substantially flat and substantially parallel first and second surfaces.

Claim 19

The laser of claim 17 wherein: said at least one birefringent plate is comprised of a material selected from the group consisting of sapphire and quartz, and said at least one birefringent plate is disposed in said laser cavity at the Brewster angle substantially between the normal to said first surface of said at least one birefringent plate and the path of said laser emission from said laser crystal.

Claim 20

The laser of claim 2 wherein said second means includes: a nonlinear crystal disposed in said reflective path for generating second harmonics of said desired laser transition wavelength to suppress laser spiking at said desired laser transition wavelength in said laser cavity; and means for tilting said nonlinear crystal to a proper phasematching angle for maximum second harmonic generation.

Claim 21

The laser of claim 19 wherein: said nonlinear crystal is a lithium iodate crystal.

Claim 22

The laser of claim 19 wherein: said tuning means includes a tuning element comprised of a stack of birefringent plates oriented at Brewster's angle to the direction of propagation of said laser emission, each of said birefringent plates having an optic axis which lies in the plane of that birefringent plate and is aligned in parallel with each of the other said optic axes; and means for rotating said tuning element about an axis normal to said optic axes to tune said laser emission to a different wavelength within said range of wavelengths; and said aperture means includes an opaque element containing a hole in said reflective path for only passing the lowest order spatial transverse mode of said desired laseer transition wavelength therethrough.

Claim 23

The laser of claim 21 wherein: said birefringent plates have predetermined thicknesses, with the thicker said birefringent plates having integer multiples of the thickness of the thinnest said birefringent plate.

Claim 24

The laser of claim 21 wherein said first means includes: a plurality of optical plates oriented at Brewster's angle and selectively disposed between preselected adjacent birefringent plates in said tuning element to suppress the oscillation of undesired laser transition wavelengths within said laser cavity, said optical plates being transparent to laser emission over said range of wavelengths.

Claim 25

The laser of claim 23 wherein: said optical plates are comprised of a material selected from the group consisting of calcium fluoride, fused silica and barium fluoride.

Claim 26

The laser of claim 23 wherein: said birefringent plates have predetermined thicknesses, with the thicker said birefringent plates having integer multiples of the thickness of the thinnest said birefringent plate.

Claim 27

The laser of claim 21 wherein: said first means includes first and second sets of optical plates oriented at Brewster's angle and respectively disposed on opposite sides of said stack of birefringent plates to suppress the oscillation of undesired wavelengths within said laser cavity, said optical plates being transparent to laser emissions over said range of wavelengths.

Claim 28

The laser of claim 26 wherein: said birefringent plates have predetermined thicknesses, with the thicker said birefringent plates having integer multiples of the thickness of the thinnest said birefringent plate.

Claim 29

The laser of claim 1 wherein: said preselected activator ions in said host material comprise a dopant of Tm 3+ ions; and said host material further includes a dopant of Cr 3+ sensitizer ions.

Claim 30

The laser of claim 28 wherein: said host material is selected from the group consisting of YAG, YSGG, GSGG, GSAG, YSAG, YAlO, GGG, YGG, LLGG, and mixtures thereof; said dopant of Cr 3+ ions has an effective percent concentration of between about 0.3% and about 3%; and said dopant of Tm 3+ ions has an effective percent concentration of between about 2% and about 12%.

Claim 31

The laser of claim 28 wherein: said host material is selected from the group consisting of YAG, YSAG, YSGG and GSGG; said dopant of Cr 3+ ions has an effective percent concentration of between about 0.3% and about 1.5%; and said dopant of Tm 3+ ions has an effective percent concentration of between about 4.5% and about 7.5%.

Claim 32

The laser material of claim 28 wherein: said host material is YAG; said dopant of Cr 3+ ions has an effective percent concentration of between about 0.6% and about 0.9%; and said dopant of Tm 3+ ions has an effective percent concentration of between about 5% and about 6%.

Claim 33

The laser of claim 1 wherein: said laser crystal is substantially in the form of a cylindrical laser rod whose long dimension is along the cylinder axis; and said optically exciting means is a pulsed flashlamp having a long dimension along a first axis which is substantially parallel to said cylinder axis of said cylindrical laser rod for enabling said Cr 3+ ions in said cylindrical laser rod to absorb light from said flashlamp along the long dimension of said laser rod.

Claim 34

The laser of claim 32 wherein: said preselected activator ions in said host material comprise a dopant of Tm 3+ ions; and said host material further includes a dopant of Cr 3+ sensitizer ions.

Claim 35

A solid state laser comprising: a laser cavity defined by an input reflective element and an output coupler reflective element to form a reflective optical path therebetween; a laser crystal disposed in said laser cavity, said laser crystal having a host material selected from the group consisting of YAG, YALO, YSAG, YSGG, YGG, GGG, GSAG, GSGG, LLGG and mixtures thereof, said host material being doped with Cr 3+ sensitizer ions and Tm 3+ activator ions sufficient to produce a laser emission at a desired wavelength in a range of wavelengths between about 1.9 microns and about 2.1 microns when said laser crystal is optically excited to produce said laser emission; flashlamp means for exciting said laser crystal to produce a pulsed laser emission in the range of a plurality of wavelengths determined by Stark components in the 3 F 4 to 3 H 6 laser transition in said thulium activator ions when said laser crystal is excited by said exciting means; means disposed in said laser cavity between said laser crystal and one of said reflective elements and oriented at Brewster's angle in said reflective path for tuning said laser emission to any desired one of said plurality of wavelengths within the range between approximately 1.9 microns and approximately 2.1 microns; first means oriented at Brewster's angle in said reflective path on at least one side of said tuning means for suppressing oscillation of undesired wavelengths within said laser cavity and only enabling said desired wavelength to pass out of said output coupler reflective element; and second means disposed in said reflective path for suppressing laser spiking in said laser cavity to enable said laser to emit through said output coupler reflective element a smooth, long pulse of laser emission without spiking at said desired laser transition wavelength.

Claim 36

A solid state laser comprising: a laser cavity defined by an input reflective element and an output coupler reflective element to form a reflective optical path therebetween; a laser crystal disposed in said laser cavity, said laser crystal having a host material selected from the group consisting of YAG, YALO, YSAG, YSGG, YGG, GGG, GSAG, GSGG, LLGG and mixtures thereof, said host material being doped with Cr 3+ sensitizer ions and Tm 3+ activator ions sufficient to produce a laser emission at a desired wavelength in a range of wavelengths between about 1.9 microns and about 2.1 microns when said laser crystal is optically excited to produce said laser emission; flashlamp means for exciting said laser crystal to produce a pulsed laser emission in the range of a plurality of wavelengths determined by Stark components in the 3 F 4 to 3 H 6 laser transition in said thulium activator ions when said laser crystal is excited by said exciting means; means disposed in said laser cavity between said laser crystal and one of said reflective elements and oriented at Brewster's angle in said reflective path for tuning said laser emission to any desired one of said plurality of wavelengths within the range between approximately 1.9 microns and approximately 2.1 microns; first means oriented at Brewster's angle in said reflective path on at least one side of said tuning means for suppressing oscillation of undesired wavelengths within said laser cavity and only enabling said desired wavelength to pass out of said output coupler reflective element; and second means disposed in said reflective path for suppressing laser spiking in said laser cavity to enable said laser to emit through said output coupler reflective element a smooth, long pulse of laser emission without spiking at said desired laser transition wavelength.