Single longitudinal mode frequency converted laser

Claim 2

A single longitudinal mode, frequency-converted solid-state laser comprising: an optical pumping means for producing optical pumping radiation; a coupled resonant cavity including a first resonant cavity and a second resonant cavity that share a common partially reflecting mirror; a solid-state laser medium disposed within said first resonant cavity and being optically pumped by said optical pumping radiation, said solid-state laser medium generating a first laser radiation at a first wavelength; an optical wavelength converting means disposed within said second resonant cavity for converting said first laser radiation at said first wavelength into a second laser radiation at a second wavelength; and a temperature controlling means for controlling the temperature of said first resonant cavity and said second resonant cavity, whereby said first resonant cavity and said second resonant cavity are used for oscillating said first laser radiation at said first wavelength.

Claim 3

The laser of claim 1 wherein optical path lengths of said first resonant cavity and of said second resonant cavity are selected such that only one longitudinal mode of said coupled resonant cavity is within the gain bandwidth of said laser medium.

Claim 4

The laser of claim 1 wherein the ratio of an optical path length of said second resonant cavity to an optical path length of said first resonant cavity is about a value selected from the group of 0.5, 1.5, 2.5, 3.5, 4.5, 5.5, 6.5, 7.5, and 8.5.

Claim 5

The laser of claim 1 wherein the ratio of an optical path length of said first resonant cavity to an optical path length of said second resonant cavity is about a value selected from the group of 0.5, 1.5, 2.5, 3.5, 4.5, 5.5, 6.5, 7.5, and 8.5.

Claim 6

The laser of claim 1 wherein optical path lengths of said first resonant cavity and of said second resonant cavity are selected such that the interval of longitudinal modes of said coupled resonant cavity is larger than one half of the gain bandwidth of said solid-state laser medium.

Claim 7

The laser of claim 5 wherein the ratio of said optical path length of said second resonant cavity to said optical path length of said first resonant cavity is about a value selected from the group of 0.5, 1.5 and 2.5.

Claim 8

The laser of claim 1 wherein said solid-state laser medium is a solid that includes at least one element selected from the group of Nd, Ho, Er, Tm, Ti, Cr, Yb, Ce, and rare earth elements.

Claim 9

The laser of claim 1 wherein said solid-state laser medium is made from a material that is selected from the group of Nd:YAG, Nd doped garnets, Nd:glass, Nd:YAP, Nd:YVO 4 , Nd:GdVO 4 , Nd:Sr 5 (PO 4 ) 3 F, Nd:LaSc 3 (BO 3 ) 4 , NAB, NdP 5 O 14 , NdLiPO, NdKPO, Nd:YLF, Nd:Sr 5 (VO 4 ) 3 F, Nd:YAB and Nd:X a Z b (BO 3 ).sub.(a+b), where "X" is one element selected from Al, Y, Sc, and rare earth elements, where "Z" is one element selected from Al, Y, Sc, and rare earth elements and where "a" and "b" are integers or fractions.

Claim 10

The laser of claim 1 wherein said wavelength converting means is selected from the group of KTP, KDP, ADA, ADP, CDA, YAB, BBO, KNbO 3 , LiNbO 3 , LBO, CLBO, LIO and MTiO(XO 4 ), where "M" is at least one of K, Rb, Tl, Cs or NH 4 , and where "X" is at least one of P or As.

Claim 11

The laser of claim 1 wherein said laser produces light at said second wavelength that is one of blue light and green light.

Claim 12

The laser of claim 1 further comprising: an input mirror included as part of said first resonant cavity that substantially reflects said first laser radiation at said first wavelength and transmits resonant said optical pumping radiation; an output mirror included as part of said second resonant cavity that substantially reflects said first laser radiation at said first wavelength and transmits resonant at least some of said second laser radiation at said second wavelength; and wherein said common partially reflecting mirror partially reflects laser radiation at said first wavelength and partially transmits said first laser radiation at said first wavelength.

Claim 13

The laser of claim 11 wherein said input mirror further reflects said second laser radiation at said second wavelength and is formed on an input surface of said solid-state laser medium.

Claim 14

The laser of claim 11 wherein said output mirror is formed on an output surface of said optical wavelength converting means.

Claim 15

The laser of claim 1 further comprising: an input mirror included as part of said first resonant cavity that has a reflectance between 99% and 100% at said first wavelength; and an output mirror included as part of said second resonant cavity that has a reflectance between about 99% and 100% at said first wavelength.

Claim 16

The laser of claim 14 wherein said common partially reflecting mirror has a reflectance between about 3% and 98% at said first wavelength.

Claim 17

The laser of claim 14 wherein said common partially reflecting mirror has a reflectance between about 30% and 70% at said first wavelength.

Claim 18

The laser of claim 14 wherein said common partially reflecting mirror has a reflectance between about 15% and 80% at said first wavelength and is formed on an intermediate surface of said optical wavelength converting means, said intermediate surface of said optical wavelength converting means being adjacent to said solid-state laser medium.

Claim 19

The laser of claim 14 wherein said common partially reflecting mirror has a reflectance between about 15% and 80% at said first wavelength and is formed on an intermediate surface of said solid-state laser medium, said intermediate surface of said solid-state laser medium being adjacent to said optical wavelength converting means.

Claim 20

The laser of claim 14 wherein said common partially reflecting mirror includes an absorption layer.

Claim 21

The laser of claim 14 wherein said common partially reflecting mirror partially reflects said first laser radiation at said first wavelength and partially transmits said first laser radiation at said first wavelength and reflects said second laser radiation at said second wavelength.

Claim 22

The laser of claim 1 wherein said temperature controlling means is used to adjust said temperature of said first and second resonant cavities to produce a single longitudinal mode and said temperature controlling means is also used to adjust said temperature to produce multiple longitudinal modes of said laser, said laser being able to operate in a single or multiple longitudinal modes.

Claim 23

A frequency-doubled solid-state laser comprising: a diode pumping source that produces optical pumping radiation; a coupled resonant cavity including a first resonant cavity, a second resonant cavity and a common partially reflecting mirror shared between said first resonant cavity and said second resonant cavity, said first resonant cavity being defined by an input mirror and said common partially reflecting mirror, said second resonant cavity being defined by an output mirror and said common partially reflecting mirror; a solid-state laser medium disposed within said first resonant cavity and being optically pumped by said optical pumping radiation, said solid-state laser medium generating a first laser radiation at a first wavelength in a single transverse mode; an optical wavelength converting means disposed within said second resonant cavity that converts said first laser radiation at said first wavelength into a second laser radiation at a second wavelength, said common partially reflecting mirror being formed on an intermediate surface of one of said solid-state laser medium and said optical wavelength converting means; and temperature controlling means for controlling temperatures of said first and second resonant cavities, wherein said first resonant cavity and said second resonant cavity are used for oscillating said first laser radiation at said first wavelength and wherein said common partially reflecting mirror partially reflects laser radiation at said first wavelength and partially transmits said first laser radiation at said first wavelength.

Claim 24

A frequency-doubled solid-state laser comprising: a diode pumping source that produces optical pumping radiation; a coupled resonant cavity including a first resonant cavity, a second resonant cavity and a common partially reflecting mirror shared between said first resonant cavity and said second resonant cavity, said first resonant cavity being defined by an input mirror and said common partially reflecting mirror, said second resonant cavity being defined by an output mirror and said common partially reflecting mirror; a solid-state laser medium disposed within said first resonant cavity and being optically pumped by said optical pumping radiation, said solid-state laser medium generating a first laser radiation at a first wavelength in a single transverse mode; an optical wavelength converting means disposed within said second resonant cavity that converts said first laser radiation at said first wavelength into a second laser radiation at a second wavelength, said common partially reflecting mirror being formed on an intermediate surface of one of said solid-state laser medium and said optical wavelength converting means; and temperature controlling means for controlling temperatures of said first and second resonant cavities, wherein said first resonant cavity and said second resonant cavity are used for oscillating said first laser radiation at said first wavelength and wherein said common partially reflecting mirror partially reflects laser radiation at said first wavelength and partially transmits said first laser radiation at said first wavelength.

Claim 25

The laser of claim 22 wherein said optical wavelength converting means is a second harmonic generator that converts said first laser radiation at said first wavelength into the second harmonic laser radiation of said first laser radiation.

Claim 26

The laser of claim 22 wherein optical path lengths of said first resonant cavity and of said second resonant cavity are selected to provide a single longitudinal mode laser oscillating in said coupled resonant cavity.

Claim 27

The laser of claim 22 wherein the ratio of an optical path length of said second resonant cavity to an optical path length of said first resonant cavity is about a value selected from the group of 0.5, 1.5, 2.5, and 3.5.

Claim 28

The laser of claim 22 wherein the ratio of an optical path length of said first resonant cavity to an optical path length of said second resonant cavity is about a value selected from the group of 0.5, 1.5, 2.5, and 3.5.

Claim 29

A frequency-converted coupled resonant cavity used in a solid-state laser comprising: a first resonant cavity having a first optical path length and including a solid-state laser medium used for generating a first laser radiation at a first wavelength; a second resonant cavity having a second optical path length and including an optical wavelength converting means for converting said first laser radiation at said first wavelength into a second laser radiation at a second wavelength, wherein the ratio of said second optical path length to said first optical path length is about a value selected from the group of 0.5, 1.5, 2.5, 3.5, 4.5, 5.5, 6.5, 7.5, and 8.5; and a common partially reflecting mirror shared between said first resonant cavity and said second resonant cavity, said common partially reflecting mirror partially reflecting said first laser radiation at said first wavelength and partially transmitting said first laser radiation at said first wavelength.

Claim 30

A frequency-converted coupled resonant cavity used in a solid-state laser comprising: a first resonant cavity having a first optical path length and including a solid-state laser medium used for generating a first laser radiation at a first wavelength; a second resonant cavity having a second optical path length and including an optical wavelength converting means for converting said first laser radiation at said first wavelength into a second laser radiation at a second wavelength, wherein the ratio of said second optical path length to said first optical path length is about a value selected from the group of 0.5, 1.5, 2.5, 3.5, 4.5, 5.5, 6.5, 7.5, and 8.5; and a common partially reflecting mirror shared between said first resonant cavity and said second resonant cavity, said common partially reflecting mirror partially reflecting said first laser radiation at said first wavelength and partially transmitting said first laser radiation at said first wavelength.

Claim 31

The coupled resonant cavity of claim 27 wherein said common partially reflecting mirror has a reflectance between about 15% and 80% at said first wavelength.

Claim 32

The coupled resonant cavity of claim 27 wherein said common partially reflecting mirror has a reflectance between about 25% and 70% at said first wavelength.

Claim 33

The coupled resonant cavity of claim 27 wherein the ratio of said second optical path length to said first optical path length is about a value selected from the group of 0.5, 0.75, 1.5 and 2.

Claim 34

The coupled resonant cavity of claim 27 further comprising: temperature controlling means for controlling the temperature of said first resonant cavity and of said second resonant cavity.

Claim 35

A coupled resonant cavity used in a single longitudinal mode frequency-converted solid-state laser comprising: a first resonant cavity having a first optical path length and including a solid-state laser medium used for generating a first laser radiation at a first wavelength; a second resonant cavity having a second optical path length and including an optical wavelength converting means for converting said first laser radiation at said first wavelength into a second laser radiation at a second wavelength, wherein the ratio of said second optical path length to said first optical path length is such that said laser operates in a single longitudinal mode; and a common partially reflecting mirror shared between said first resonant cavity and said second resonant cavity, said common partially reflecting mirror partially reflecting said first laser radiation at said first wavelength and partially transmitting said first laser radiation at said first wavelength.

Claim 36

A coupled resonant cavity used in a single longitudinal mode frequency-converted solid-state laser comprising: a first resonant cavity having a first optical path length and including a solid-state laser medium used for generating a first laser radiation at a first wavelength; a second resonant cavity having a second optical path length and including an optical wavelength converting means for converting said first laser radiation at said first wavelength into a second laser radiation at a second wavelength, wherein the ratio of said second optical path length to said first optical path length is such that said laser operates in a single longitudinal mode; and a common partially reflecting mirror shared between said first resonant cavity and said second resonant cavity, said common partially reflecting mirror partially reflecting said first laser radiation at said first wavelength and partially transmitting said first laser radiation at said first wavelength.

Claim 37

The coupled resonant cavity of claim 32 wherein said first resonant cavity produces a plurality of first longitudinal modes having a first interval, wherein said second resonant cavity produces a plurality of second longitudinal modes having a second interval, and wherein said coupled cavity produces a plurality of coupled longitudinal modes having a coupled interval such that said coupled interval is the least common multiple of said first interval and said second interval whereby said laser operates in a single longitudinal mode.

Claim 38

The coupled resonant cavity of claim 33 further comprising: temperature controlling means for controlling the temperature of said first resonant cavity and of said second resonant cavity.

Claim 39

The coupled resonant cavity of claim 32 further comprising: temperature controlling means for controlling the temperature of said first resonant cavity and of said second resonant cavity.

Claim 40

The coupled resonant cavity of claim 32 wherein said optical path lengths of said first resonant cavity and of said second resonant cavity are selected such that the interval of longitudinal modes of said coupled resonant cavity is larger than one-half of the gain bandwidth of said solid-state laser medium.

Claim 41

The coupled resonant cavity of claim 36 further comprising: temperature controlling means for controlling the temperature of said first resonant cavity and of said second resonant cavity.

Claim 42

A coupled resonant cavity used in a single longitudinal mode frequency-converted solid-state laser comprising: a first resonant cavity having a first optical path length and including a solid-state laser medium used for generating a first laser radiation at a first wavelength; a second resonant cavity having a second optical path length and including an optical wavelength converting means for converting said first laser radiation at said first wavelength into a second laser radiation at a second wavelength, wherein the ratio of said second optical path length to said first optical path length is such that said laser operates in a single longitudinal mode; and temperature controlling means for controlling the temperature of said first resonant cavity and of said second resonant cavity to adjust said first and second optical path lengths.

Claim 43

A coupled resonant cavity used in a single longitudinal mode frequency-converted solid-state laser comprising: a first resonant cavity having a first optical path length and including a solid-state laser medium used for generating a first laser radiation at a first wavelength; a second resonant cavity having a second optical path length and including an optical wavelength converting means for converting said first laser radiation at said first wavelength into a second laser radiation at a second wavelength, wherein the ratio of said second optical path length to said first optical path length is such that said laser operates in a single longitudinal mode; and temperature controlling means for controlling the temperature of said first resonant cavity and of said second resonant cavity to adjust said first and second optical path lengths.

Claim 44

A single longitudinal mode, frequency-converted solid-state laser comprising: an optical pumping source that produces optical pumping radiation; a laser resonant cavity including a first resonant cavity and a second resonant cavity that share a common partially reflecting mirror, said laser resonant cavity receiving said optical pumping radiation; a solid-state laser medium disposed within said laser resonant cavity and being optically pumped by said optical pumping radiation, said solid-state laser medium generating a first laser radiation at a first wavelength; an optical wavelength converting means disposed within said laser resonant cavity for converting said first laser radiation at said first wavelength into a second laser radiation at a second wavelength; and a temperature controller for controlling the temperature of said first resonant cavity and said second resonant cavity, wherein said first resonant cavity and said second resonant cavity are used for oscillating said first laser radiation at said first wavelength and wherein optical path lengths of said first resonant cavity and of said second resonant cavity are selected such that only one longitudinal mode of said laser resonant cavity is within the gain bandwidth of said laser medium.

Claim 45

A single longitudinal mode, frequency-converted solid-state laser comprising: an optical pumping source that produces optical pumping radiation; a laser resonant cavity including a first resonant cavity and a second resonant cavity that share a common partially reflecting mirror, said laser resonant cavity receiving said optical pumping radiation; a solid-state laser medium disposed within said laser resonant cavity and being optically pumped by said optical pumping radiation, said solid-state laser medium generating a first laser radiation at a first wavelength; an optical wavelength converting means disposed within said laser resonant cavity for converting said first laser radiation at said first wavelength into a second laser radiation at a second wavelength; and a temperature controller for controlling the temperature of said first resonant cavity and said second resonant cavity, wherein said first resonant cavity and said second resonant cavity are used for oscillating said first laser radiation at said first wavelength and wherein optical path lengths of said first resonant cavity and of said second resonant cavity are selected such that only one longitudinal mode of said laser resonant cavity is within the gain bandwidth of said laser medium.

Claim 46

A single longitudinal mode, frequency-converted solid-state laser as recited in claim 39 wherein said laser resonant cavity is a coupled resonant cavity and wherein said solid-state laser medium is disposed within said first resonant cavity and wherein said optical wavelength converting means is disposed within said second resonant cavity.