(REx Y1-x Al3 (BO3)4 crystals in electrooptic and nonlinear devices

Claim 2

A nonlinear optical device comprising a crystal having nonlinear optical properties, and means for directing at least one incident beam of electromagnetic radiation into said crystal, whereby electromagnetic radiation emerging from said crystal contains at least one frequency different from the frequency of any incident beam of radiation, said crystal being a single crystal having the formula: (RE).sub.x Y.sub.1-x Al.sub.3 (BO.sub.3).sub.4 wherein 0≦x≦1 and (RE) is a rare-earth element other than Nd and Er.

Claim 3

A nonlinear optical device as in claim 1, wherein x is from 0.02 to 0.95.

Claim 4

A nonlinear optical device as in claim 1, wherein x is from 0.02 to 0.2.

Claim 5

A nonlinear optical device as in claim 1, wherein x is 0.

Claim 6

An electrooptic modulator comprising means for directing a beam of polarized radiation into a birefringent crystal, and means for applying an electric field to said crystal to change birefringence whereby the polarization of radiation emerging from said crystal is changed, wherein said birefringent crystal has the formula: (RE).sub.x Y.sub.1-x Al.sub.3 (BO.sub.3).sub.4 wherein 0≦x≦1 and (RE) is a rare-earth element other than Nd and Er.

Claim 7

An electrooptic modulator comprising means for directing a beam of polarized radiation into a birefringent crystal, and means for applying an electric field to said crystal to change birefringence whereby the polarization of radiation emerging from said crystal is changed, wherein said birefringent crystal has the formula: (RE).sub.x Y.sub.1-x Al.sub.3 (BO.sub.3).sub.4 wherein 0≦x≦1 and (RE) is a rare-earth element other than Nd and Er.

Claim 8

An electrooptic modulator as in claim 5, wherein x is from 0.02 to 0.95.

Claim 9

An electrooptic modulator as in claim 5, wherein x is from 0.02 to 0.2.

Claim 10

An electrooptic modulator as in claim 5, wherein x is 0.

Claim 11

A Q-switched laser with Nd:YAG as gain medium having provided as an intracavity second harmonic generator a single crystal having the formula: (RE).sub.x Y.sub.1-x Al.sub.3 (BO.sub.3).sub.4 wherein 0≦x≦1 and (RE) is a rare-earth element other than Nd and Er.

Claim 12

A Q-switched laser with Nd:YAG as gain medium having provided as an intracavity second harmonic generator a single crystal having the formula: (RE).sub.x Y.sub.1-x Al.sub.3 (BO.sub.3).sub.4 wherein 0≦x≦1 and (RE) is a rare-earth element other than Nd and Er.

Claim 13

A Q-switched laser with Nd:YAG as gain medium having provided as an intracavity second harmonic generator a single crystal as in claim 9, wherein x is from 0.02 to 0.95.

Claim 14

A Q-switched laser with Nd:YAG as gain medium having provided as an intracavity second harmonic generator a single crystal as in claim 9, wherein x is from 0.02 to 0.2.

Claim 15

A Q-switched laser with Nd:YAG as gain medium having provided as an intracavity second harmonic generator a single crystal as in claim 9, wherein x is 0.

Claim 16

A high efficiency, diode pumped compact laser comprising: a neodymium-YAG laser rod having a front end and a back end; a housing including means for holding the neodymium-YAG laser rod in fixed position in the housing with its front end forward; a laser diode for pumping the neodymium-YAG laser rod, having an output frequency sufficiently matched to the rod to pump the rod, secured in the housing behind and in optical alignment with the rod; output coupler means including a mirrored surface forming a front end of a laser cavity; rear mirror means forming a back end of the laser cavity, with the neodymium-YAG rod within the cavity; an intracavity frequency doubler within the laser cavity, positioned to receive the output beam of the laser rod and to halve its wavelength, doubling its frequency; and polarization control means for adjusting and maintaining the polarization of the laser beam to a polarization which optimizes frequency doubling of the laser beam by the frequency doubler, wherein said intracavity frequency doubler is a single crystal having the formula: (RE).sub.x Y.sub.1-x Al.sub.3 (BO.sub.3).sub.4 wherein 0≦x≦1 and (RE) is a rare-earth element other than Nd and Er.

Claim 17

A high efficiency, diode pumped compact laser comprising: a neodymium-YAG laser rod having a front end and a back end; a housing including means for holding the neodymium-YAG laser rod in fixed position in the housing with its front end forward; a laser diode for pumping the neodymium-YAG laser rod, having an output frequency sufficiently matched to the rod to pump the rod, secured in the housing behind and in optical alignment with the rod; output coupler means including a mirrored surface forming a front end of a laser cavity; rear mirror means forming a back end of the laser cavity, with the neodymium-YAG rod within the cavity; an intracavity frequency doubler within the laser cavity, positioned to receive the output beam of the laser rod and to halve its wavelength, doubling its frequency; and polarization control means for adjusting and maintaining the polarization of the laser beam to a polarization which optimizes frequency doubling of the laser beam by the frequency doubler, wherein said intracavity frequency doubler is a single crystal having the formula: (RE).sub.x Y.sub.1-x Al.sub.3 (BO.sub.3).sub.4 wherein 0≦x≦1 and (RE) is a rare-earth element other than Nd and Er.

Claim 18

A high efficiency, diode pumped compact laser as in claim 9, wherein x is from 0.02 to 0.95.

Claim 19

A high efficiency, diode pumped compact laser as in claim 9, wherein x is from 0.02 to 0.2.

Claim 20

A high efficiency, diode pumped compact laser as in claim 9, wherein x is 0.