Miniaturized self-Q-switched frequency-doubled laser

Claim 2

A laser, comprising: a laser cavity comprising a self-frequency-doubling host material doped with at least two ionic species, where one of said ionic species absorbs energy at one wavelength λ 1 , and emits it at another wavelength λ 2 , larger than λ 1 , said other ionic species having the property that it is a saturable absorber with respect to said first ionic species so that said other ionic species absorbs energy emitted from said first ionic species at wavelength λ 2 and emits energy within said cavity in the form of a series of high-intensity radiation pulses at wavelength λ 2 ; a radiation source optically coupled with said laser cavity to pump said first ionic species so that it emits radiation at wavelength λ 2 , which is then converted to said high-intensity radiation pulses at wavelength λ 2 via said other ionic species; and means for providing feedback to said laser cavity so that it operates as a resonator at wavelength λ 2 to propagate said high-intensity pulses at wavelength λ 2 along its length so that said self-frequency-doubling host material operates to convert said high-intensity pulses at λ 2 into a series of high-intensity pulses at λ 3 , and for transmitting said series of high-intensity pulses at wavelength λ 3 , that is half the wavelength of λ 2 , from said laser cavity so that they are available for use outside of said laser.

Claim 3

The laser of claim 1 further comprising a non-linear crystal positioned to receive said series of high-intensity pulses emitted from said laser at λ 3 and to convert them into a series of pulses at wavelength λ 4 , that is half the wavelength of λ 3 .

Claim 4

The laser of claim 2 wherein said means for providing feedback comprises input mirror means and output mirror means, said input mirror means being flat and highly transmissible at wavelength λ 1 , and also being highly reflective at wavelength λ 2 and at wavelength λ 3 ; said output mirror means being convex and highly reflective at wavelength λ 1 and at wavelength λ 2 , also being highly transmissible at wavelength λ 3 ; and wherein said laser further comprises lens means disposed between said output mirror means and said non-linear crystal whereby said series of high-intensity pulses at λ 3 are brought to focus upon said non-linear crystal.

Claim 5

The laser of claim 2 wherein said non-linear crystal comprises a material which is selected from the group consisting of: beta barium borate (BaB 2 O 4 ) and lithium triborate (LiB 3 O 5 ).

Claim 6

The laser of claim 1 wherein said means for providing feedback comprises input mirror means and output mirror means, said input mirror means being highly transmissible at wavelength λ 1 , and also being highly reflective at wavelength λ 2 and at wavelength λ 3 , and said output mirror means being highly reflective at wavelength λ 1 and at wavelength λ 2 , also being highly transmissible at wavelength λ 3 .

Claim 7

The laser of claim 5 wherein said mirror means are flat and substantially parallel to one another.

Claim 8

The laser of claim 5 wherein λ 1 =807 nm, λ 2 =1.064 μm, and λ 3 =532 nm.

Claim 9

The laser of claim 1 wherein said radiation source comprises a laser diode.

Claim 10

The laser of claim 8 in which λ 1 is 807 to 809 nm.

Claim 11

The laser of claim 1 wherein said self-frequency-doubling host material comprises a material which is selected from the group consisting of: barium sodium niobate (Ba 2 NaNb 5 O 12 ), lithium niobate (LiNbO 3 ), and yttrium aluminum borate (YAl 3 (BO 3 ) 4 ).

Claim 12

The laser of claim 10 in which said self-frequency-doubling host material is in the form of an etalon having a thickness of approximately 0.5 mm.

Claim 13

The laser of claim 1 wherein said first ionic dopant is neodymium (Nd 3+ ).

Claim 14

The laser of claim 1 wherein said second ionic dopant comprises a material which is selected from the group consisting of: tetravalent chromium (Cr 4+ ), trivalent cobalt (Co 3+ ), divalent iron (Fe 2+ ), and trivalent nickel (Ni 3+ ).

Claim 15

The laser of claim 1 wherein each said mirror means comprises a deposition of at least one dielectric layer.

Claim 16

A laser, comprising: a laser cavity comprising a self-frequency-doubling host material doped with trivalent neodymium ions (Nd 3+ ) and tetravalent chromium ions (Cr 4+ ), where said neodymium ions absorb energy at 807 nm and emits energy at wavelength 1.064 μm, and said tetravalent chromium ions act as saturable absorbers with respect to said neodymium ions so that energy emitted from said neodymium ions are absorbed by said chromium ions and further, that said chromium ions emit energy in the form of high-intensity radiation pulses at wavelength 1.064 μm; a laser diode, operating at a wavelength of 807 to 809 nm, optically coupled with said laser cavity to pump said neodymium ions so that said neodymium ions emit radiation at wavelength 1.064 μm which is then converted to said high-intensity radiation pulses at wavelength 1.064 μm via said chromium ions; and means for providing feedback to said laser cavity so that it operates as a resonator at wavelength 1.064 μm to propagate said high-intensity pulses at wavelength 1.064 μm along its length so that said self-frequency-doubling host material operates to convert said high-intensity pulses at 1.064 μm into a series of high-intensity pulses at 532 nm and for transmitting said series of high-intensity pulses at wavelength 532 nm from said laser cavity so that they are available for use outside of said laser.

Claim 17

A laser, comprising: a laser cavity comprising a self-frequency-doubling host material doped with trivalent neodymium ions (Nd 3+ ) and tetravalent chromium ions (Cr 4+ ), where said neodymium ions absorb energy at 807 nm and emits energy at wavelength 1.064 μm, and said tetravalent chromium ions act as saturable absorbers with respect to said neodymium ions so that energy emitted from said neodymium ions are absorbed by said chromium ions and further, that said chromium ions emit energy in the form of high-intensity radiation pulses at wavelength 1.064 μm; a laser diode, operating at a wavelength of 807 to 809 nm, optically coupled with said laser cavity to pump said neodymium ions so that said neodymium ions emit radiation at wavelength 1.064 μm which is then converted to said high-intensity radiation pulses at wavelength 1.064 μm via said chromium ions; and means for providing feedback to said laser cavity so that it operates as a resonator at wavelength 1.064 μm to propagate said high-intensity pulses at wavelength 1.064 μm along its length so that said self-frequency-doubling host material operates to convert said high-intensity pulses at 1.064 μm into a series of high-intensity pulses at 532 nm and for transmitting said series of high-intensity pulses at wavelength 532 nm from said laser cavity so that they are available for use outside of said laser.

Claim 18

The laser of claim 15 further comprising a non-linear crystal positioned to receive said series of high-intensity pulses emitted from said laser at wavelength 532 nm and to convert them into a series of pulses at wavelength 266 nm.

Claim 19

The laser of claim 16 wherein said means for providing feedback comprises input mirror means and output mirror means, said input mirror means being flat and highly transmissible at wavelength 807 to 809 nm, and also being highly reflective at wavelengths 1.064 μm and 532 nm; said output mirror means being convex and highly reflective at wavelength 807 to 809 nm and at wavelength 1.064 μm, also being highly transmissible at wavelength 532 nm; and wherein said laser further comprises lens means disposed between said output mirror means and said non-linear crystal whereby the said series of high-intensity pulses at wavelength 532 nm are brought to focus upon said non-linear crystal.

Claim 20

The laser of claim 16 wherein said means for providing feedback comprises input mirror means and output mirror means, said input mirror means being flat and highly transmissible at wavelength 807 to 809 nm, and also being highly reflective at wavelengths 1.064 μm and 532 nm; said output mirror means being convex and highly reflective at wavelength 807 to 809 nm and at wavelength 1.064 μm, also being highly transmissible at wavelength 532 nm; and wherein said laser further comprises lens means disposed between said output mirror means and said non-linear crystal whereby said series of high-intensity pulses at 532 nm are brought to focus upon said non-linear crystal.

Claim 21

The laser of claim 16 in which said self-frequency-doubling host material is in the form of an etalon having a thickness of approximately 0.5 min.

Claim 22

The laser of claim 15 wherein said means for providing feedback comprises input mirror means and output mirror means, said input mirror means being highly transmissible at wavelength 807 to 809 nm, and also being highly reflective at wavelengths 1.064 μm and 532 nm; said output mirror means being highly reflective at wavelength 807 to 809 nm and at wavelength 1.064 μm, also being highly transmissible at wavelength 532 nm; and said mirror means further being flat and essentially parallel to one another.

Claim 23

The laser of claim 15 wherein said self-frequency-doubling host material comprises a material which is selected from the group consisting of: barium sodium niobate (Ba 2 NaNb 5 O 12 ), lithium niobate (LiNbO 3 ), and yttrium aluminum borate (YAl 3 (BO 3 ) 4 ).

Claim 24

The laser of claim 15 wherein said mirror means are flat and substantially parallel to one another.

Claim 25

A laser, comprising: a laser cavity comprising a self-frequency-doubling host material doped with neodymium ions (Nd 3+ ) and tetravalent chromium ions (Cr 4+ ), where said neodymium ions absorb energy at 807 nm and emits energy at wavelength 1.064 μm, and said tetravalent chromium ions acting as saturable absorbers so that energy emitted from said neodymium ions are absorbed by said chromium ions, and further, that said chromium ions emit energy in the form of high-intensity radiation pulses at wavelength 1.064 μm; a laser diode, operating at a wavelength of 807 to 809 nm, optically coupled with said laser cavity to pump said neodymium ions so that said neodymium ions emit radiation at wavelength 1.064 μm which is then converted to said high-intensity radiation pulses at wavelength 1.064 μm via said chromium ions; input mirror means and output mirror means, said input mirror means being highly transmissible at wavelength 807 to 809 nm, and also being highly reflective at wavelengths 1.064 μm and 532 nm, said output mirror means being highly reflective at wavelength 807 to 809 nm and at wavelength 1.064 μm, also being highly transmissible at wavelength 532 nm, so that said laser cavity operates as a resonator at wavelength 1.064 μm to propagate said high-intensity pulses at wavelength 1.064 μm along its length so that said self-frequency-doubling host material operates to convert said high-intensity pulses at 1.064 μm into said series of high-intensity pulses at 532 nm and for transmitting said series of high-intensity pulses at wavelength 532 nm from said laser cavity; and a non-linear crystal positioned to receive said series of high-intensity pulses emitted from said laser at wavelength 532 nm and to convert them into a series of pulses at wavelength 266 nm.

Claim 26

A laser, comprising: a laser cavity comprising a self-frequency-doubling host material doped with neodymium ions (Nd 3+ ) and tetravalent chromium ions (Cr 4+ ), where said neodymium ions absorb energy at 807 nm and emits energy at wavelength 1.064 μm, and said tetravalent chromium ions acting as saturable absorbers so that energy emitted from said neodymium ions are absorbed by said chromium ions, and further, that said chromium ions emit energy in the form of high-intensity radiation pulses at wavelength 1.064 μm; a laser diode, operating at a wavelength of 807 to 809 nm, optically coupled with said laser cavity to pump said neodymium ions so that said neodymium ions emit radiation at wavelength 1.064 μm which is then converted to said high-intensity radiation pulses at wavelength 1.064 μm via said chromium ions; input mirror means and output mirror means, said input mirror means being highly transmissible at wavelength 807 to 809 nm, and also being highly reflective at wavelengths 1.064 μm and 532 nm, said output mirror means being highly reflective at wavelength 807 to 809 nm and at wavelength 1.064 μm, also being highly transmissible at wavelength 532 nm, so that said laser cavity operates as a resonator at wavelength 1.064 μm to propagate said high-intensity pulses at wavelength 1.064 μm along its length so that said self-frequency-doubling host material operates to convert said high-intensity pulses at 1.064 μm into said series of high-intensity pulses at 532 nm and for transmitting said series of high-intensity pulses at wavelength 532 nm from said laser cavity; and a non-linear crystal positioned to receive said series of high-intensity pulses emitted from said laser at wavelength 532 nm and to convert them into a series of pulses at wavelength 266 nm.

Claim 27

The laser of claim 23 where said non-linear crystal comprises a crystal of beta barium borate (BaB 2 O 4 ).

Claim 28

The laser of claim 23 where said non-linear crystal comprises a crystal of lithium triborate (LiB 3 O 5 ).

Claim 29

The laser of claim 23 further comprising lens means disposed between said output mirror means and said non-linear crystal whereby the said series of high-intensity pulses at wavelength 532 nm are brought to focus upon said non-linear crystal.