Nonlinear optical crystal optimized for ytterbium laser host wavelengths
View Patent ↗A material for harmonic generation has been made by substitutional changes to the crystal LaCa 4 (BO 3 ) 3 also known as LaCOB in the form Re1 x Re2 y Re3 z Ca 4 (B0 3 ) 3 O where Re1 and Re2, (rare earth ion 1 and rare earth ion 2) are selected from the group consisting of Sc, Yttrium, La, Ce, Pr, Nd, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb, and Lu; Re3 is Lanthanum; and x+y+z=1.
1. A laser apparatus, comprising:
a laser gain medium,
an excitation means coupled with the gain medium for pumping the gain medium,
a cavity forming means surrounding the gain medium to form a resonate laser cavity,
a harmonic generator capable of doubling the frequency of said radiation, said harmonic generator being a crystal having the general chemical formula Re1 x Re2 y Ca 4 (BO 3 ) 3 O, wherein Re1 is Gd and Re2 is Lanthanum; and x ranges from greater than 0 to about 0.7, y=1−x, and x+v=1; and wherein said Re1 and Re2, are manipulated in a predetermined fashion during the growth process of the crystal so as to modify the principle birefringence plane of said crystal and enable noncritical phase-matching for harmonic generation, and
an energy extraction means in the cavity forming means to remove laser energy from the cavity.
2. The apparatus of claim 1 , wherein the laser gain medium further comprises a Ytterbium doped laser gain medium having an emission wavelength between about 1030 nm and about 1047 nm.
3. The apparatus of claim 1 , wherein the laser gain medium further comprises a Ytterbium doped laser gain medium having an emission wavelength between about 970 nm and about 985 nm.
4. The apparatus of claim 1 , wherein the crystal is an intracavity device and adapted within a laser cavity to multiply the frequency of said radiation.
5. The apparatus of claim 2 , wherein said Ytterbium doped laser gain medium is a material selected from Yb:SFAP, Yb:YAG, YbAG, Yb:glass, and Yb:SiO 2 .
6. The apparatus of claim 1 , wherein the crystal is external to a laser cavity and adapted to multiply the frequency of the radiation.
7. The apparatus of claim 1 , wherein the crystal is substantially noncritically phasematched.