CA2073492C - Process for making a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user and a custom phase-conjugated circular mirror made according to the process - Google Patents
Process for making a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user and a custom phase-conjugated circular mirror made according to the processInfo
- Publication number
- CA2073492C CA2073492C CA002073492A CA2073492A CA2073492C CA 2073492 C CA2073492 C CA 2073492C CA 002073492 A CA002073492 A CA 002073492A CA 2073492 A CA2073492 A CA 2073492A CA 2073492 C CA2073492 C CA 2073492C
- Authority
- CA
- Canada
- Prior art keywords
- mirror
- lambda
- phase
- distance
- user
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Fee Related
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/10—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
- H01S3/10076—Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating using optical phase conjugation, e.g. phase conjugate reflection
Abstract
A process for making a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user is provided. The mirror reverses wavefront of one particular input beam ?o(x) determined by the user, the input beam ?o(x) having a given wavelength, the laser resonator including the mirror and an output coupler cooperating with the mirror and separated therefrom by a laser gain medium, the mirror being at a distance L from the output coupler. The process comprises steps of (a) determining the input beam ?o(x) that will suit need of the user; (b) calculating equation of ?L(X) which is a value of the input beam ?o(x) that is propagated through said laser gain medium at distance L; (c) calculating phase .PHI.o(x) of the input beam, which is a phase of the input beam ?o(x) at distance L, the phase .PHI.o(x) determining profile of the custom phase-conjugated mirror; and (d) fabricating the custom phase-conjugated mirror according to the profile determined in step (c), whereby a custom phase-conjugated mirror can be provided to suit the specifications of the user. There is also provided a mirror made according to the above-mentioned method.
Description
2073~92 PROCESS FOR NAKING A CUSTOM PHASE-CONJUGATED CIRCULAR MIRROR
TO BE USED IN A LASER R~ONATOR THAT WILL SUIT
~Yh~l~lCATIONS OF A USER AND A CUSTOM PHASE-CONJUGATED
CIRCULAR MIRROR HADE AcrQRnING TO THE PROCESS
s FIELD OF THE INVENTION
The present invention relates to a process for making a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user, to a process for making a custom laser resonator that will suit specifications of the user, to a custom phase-conjugated circular mirror made according to the above-mentioned process, and to a custom laser resonator made according to the above-mentioned process.
RA~r7~ouND OF THE INVENTION
Known in the art, there is the U.S. patent no.
4,803,694 of Chun-Sheu LEE et al., granted on February 7, 1989, wherein there is described a laser resonator having a cavity for the propagation of a laser beam having a wavefront in which a laser medium is positioned, comprising an aspherical concave mirror means disposed in the cavity facing an optical means for reflecting the expanded wavefront toward the lasing medium and correcting wavefront aberrations induced when the laser beam passes through the laser medium. The geometry of the aspherical concave mirror is defined by a predetermined equation.
This patent does not provide the necessary means or the necessary method steps by which a user can determine specifications from which a custom phase-conjugated circular mirror or a laser resonator including such mirror can be made. ~
Also known in the art, there is the U.S. patents nos. 4,233,571; 4,529,273; 4,715,689; and 4,750,818, describing different conjugated mirrors, and lasers including such mirrors. But none of these patents describes the necessary means or the necessary method steps by which a user can determine specifications from which a conjugated mirror or a laser including such mirror can be made.
OBJECTS OF THE INVENTION
It is an object of the present invention to provide the necessary means or the necessary method steps by which a user can determine specifications from which a custom phase-conjugated circular mirror or a laser resonator including such mirror can be provided.
SUMHARY OF THE INVENTION
According to the present invention, there is provided a process for making a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user, said mirror reversing wavefront of one particular input beam ~O(X) determined by said user, said input beam ~O(x) having a given wavelength, said laser resonator including said mirror and an output coupler cooperating with said mirror and separated therefrom by a laser gain medium, said mirror being at a distance L
from said output coupler, said process comprising steps of:
(a) determining said input beam ~O(X) that will suit need of said user;
(b) calculating equation of ~L ( X ) which is a value of said input beam ~O(x) that is propagated through said laser gain medium at said distance L, where:
~ (x) = (~)/(lB)I ~(~)e(~i~/AB)(A~2 + Dx2)J[(2~x~ B]xd~
o where A, B and D are constants determined by optical elements in said laser gain medium, xO is an integration variable, x is radial distance in transverse direction of propagation, and JO is a Bessel function of zero order;
(c) calculating phase ~O(X) of said input beam, which is a phase of said input beam ~O(x) at said distance L, where:
~L(x) = ¦~L(X)¦ e (2~ O(X) said phase ~O(X) determining profile of said custom phase-conjugated mirror; and (d) fabricating said custom phase-conjugated mirror according to said profile determined in step (c), whereby a custom phase-conjugated mirror can be provided to suit said specifications of said user.
Also according to the present invention, there is provided a process for making a custom laser resonator that will suit specifications of a user, said laser including a phase conjugated circular mirror which reverses wavefront of one particular input beam ~O(x) determined by said user, said input beam ~O(X) having a given wavelength, said laser resonator including an output coupler cooperating with said mirror and separated therefrom by a laser gain medium, said mirror being at a distance L from said output coupler, said process comprising steps of:
(a) determining said input beam ~O(X) that will suit need of said user;
(b) calculating equation of ~L(X) which is a value of said input beam ~O(X) that is propagated through said laser gain medium at said distance L, where:
L( ) (i2~)/(AB)l ~0(xo)e(~ B)(Axo2 + DX2)J[(2 )/
where A, B and D are constants determined by optical elements in said laser gain medium, xO is an integration variable, x is radial distance in transverse direction of propagation, and JO is a Bessel function of zero order;
(c) calculating phase ~O(X) of said input beam, which is a phase of said input beam ~O(X) at said distance L, where:
~L(x) = I~L(X)I e (2~/A) ~O(X) said phase ~O(X) determining profile of said custom phase-conjugated mirror; and (d) fabricating said custom phase-conjugated mirror according to said profile determined in step (c), whereby a custom laser resonator can be provided to suit said specifications of said user.
Also according to the present invention, there is provided a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user, said mirror reversing wavefront of one particular input beam YO(X) determined by said user, said input beam (X) having a given wavelength, said laser resonator including said mirror and an output coupler cooperating with said mirror and separated therefrom by a laser gain medium, said mirror being at a distance L from said output coupler, said mirror having a profile determined by ~O(X) where:
~L(x) = ¦~L(X)¦ e i(2~/~) ~O(X) where:
() (i2~)l(AB)l ~0(xo)e(-i~lAB)(~2 + Dxl)J[(2 20~734g2 where A, B and D are constants determined by optical elements in said laser gain medium, xO is an integration variable, x is radial distance in transverse direction of propagation, and JO is a Bessel function of zero order:
whereby a custom phase-conjugated mirror can be provided to suit said specifications of said user.
Also according to the present invention, there is provided a custom laser resonator that will suit specifications of a user, said laser including a phase conjugated circular mirror which reverses wavefront of one particular input beam ~O(X) determined by said user, said input beam ~O(X) having a given wavelength, said laser resonator including an output coupler cooperating with said mirror and separated therefrom by a laser gain medium, said mirror being at a distance L from said output coupler, said mirror having a profile determined by ~O(X) where:
~L( X) = ¦ ~L(X) ¦ e (2~/~) ~O(X) where:
00 . 2 2 ~L(X) (i2~)/(AB)l ~o(xo)e(-l~lAB)(Axo + Dx)J[(2 )/A
0 .
where A, B and D are constants determined by optical elements in said laser gain medium, xO is an integration variable, x is radial distance in transverse direction of propagation, and JO is a Bessel function of zero order;
whereby a custom laser resonator can be provided to suit said specifications of said user.
The objects, advantages and other features of the present invention will become more apparent upon reading of the following non restrictive description of preferred embodiment thereof, given for the purpose of exemplification only with reference to the accompanying drawings.
2073~92 BRIEF DESCRIPTION OF THE DRAWINGS
Figure 1 is a schematic diagram illustrating the relation between a specified input beam ~O(X) with respect to a custom phase-conjugated mirror;
Figure 2 is a schematic diagram illustrating a custom phase-conjugated mirror laser resonator;
Figure 3 is a schematic diagram illustrating a laser resonator made according to the present invention;
Figure 4 is a diagram illustrating ~O(X) with respect to x for a given mirror; and Figure 5 is a diagram illustrating ~O(X) with respect to x for another given mirror.
DETATT.~n DESCRIPTION OF TH~ DRAWINGS
Referring now to Figure 1, there is shown a schematic diagram illustrating the relation between a specified input beam ~O(x)~ a laser gain medium including an optical system 2, a custom phase-conjugated mirror 4 and the distance L. The process for making a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications o~ a user will be described by means of Figure 1. The mirror 4 reverses wavefront of one particular input beam ~O(X) determined by the user. The input beam ~O(X) has a given wavelength A. The laser resonator includes the mirror 4 and an output coupler (not shown in this Figure 1) cooperating with the mirror 4 and separate therefrom by a laser gain medium including optical elements 2. The mirror 4 is at a distance L from the output coupler (shown in Figure 2). The process comprises steps of (a) determining the input beam ~O(X) that will suit need of the user; (b) calculating equation of ~L(x) which is a value of the input beam ~O(X) that is propagated through the laser gain medium at the distance L, where:
2073~92 ~ (x) = (i2~)t(~B)¦ ~(x)e(~i~/AB)(A~2 + DX2)J[(2~xx)/~B]xdx where A, B and D are constants determined by the optical elements 2 in the laser gain medium, xO is an integration variable, x is radial distance in transverse direction of propagation, and JO is a Bessel function of zero order; (c) calculating phase ~O(X) of the input beam, which is a phase of the input beam ~O(x) at the distance L, where:
~L(x) = ¦~L(X)¦ e i(2~/A) ~O(X) the phase ~O(X) determining profile of the custom phase-conjugated mirror; and (d) fabricating the custom phase-conjugated mirror according to the profile determined in step (c), whereby a custom phase-conjugated mirror can be provided to suit the specifications of the user.
When the mirror has a slab geometry, ~(x) can be determined by the following equation:
~L(X) = (i/~B)l/2 1 ~O(xo)e[-i(~/~B) (Axo2 - 2xox + Dx2)] d _~
The phase-conjugated mirror (PCM) is an optical component that reverses the wavefront of an incoming beam.
A custom phase-conjugated mirror (CPCM) is an optical component that reverses wavefront of only one particular beam previously specified by the user.
The design of a CPCM proceeds as follows:
- first, the specified beam ~O(X) is propagated through the optical system 2 till a distance L using, for example, the Huygen-Fresnel integral operator:
~ (x) = (~)/(AB)I ~(X)e(~~ B)(A~2 + DX2)J~(2~xx)/AB]xdx where A is the wavelength of the beam. The above-mentioned equation has been written here for only one transverse dimension x. However, the generalization of two transverse dimensions is immediate;
- second, the phase ~O(X) of this propagated complex beam is extracted according to:
~L(x) = ¦~L(X)¦ e i(2~/A) ~O(X) - third, a mirror is fabricated according to this profile ~O(x) using the appropriate technique for a given wavelength A.
As a consequence of this design procedure, in general, any other beam than the specified one ~O(X), that passes through the same optical system 2 will, after reflection by the CPCM, diverge. Only the specified beam (X) will, after reflection and passage through the same optical system 2, be completely phase-conjugated (reversed), resulting in a nearly exact replica of the specified beam (X) at the same plane z = 0.
This feature can be used to optimize many optical systems. An example is an optical laser resonator.
Referring now to Figure 2, there is shown a schematic diagram illustrating such laser resonator. The laser resonator is an open resonator formed by a reflecting mirror 4 and an output coupler 6 enclosing a laser gain medium including optical components 2. The laser resonator is made here with a CPCM 4 and an output coupler 6 enclosing an optical system 2. According to the theory of CPCM, the specified beam ~O(x) used to design the CPCM Will necessarily be a low loss eigenmode of the resonator when the CPCM 4 has a large enough transverse dimension. This eigenmode will be of the stable type and the resonator can be described by a generalized G parameter related to the beam size (RMS)Wo of the specified beam ~O(X), namely by the following first equation:
WO2 = MZ[ (AL)/~] [G/(1-G)]1/2 where M2 is the beam quality factor.
Appropriate specification of the beam ~O(X) will lead to a large low loss fundamental eigenmode that improves the efficiency of the laser system. The discrimination feature of the laser resonator can be assessed by solving the usual eigen Huygen-Fresnel integral equation on a computer. For the practical situation of short length (L) of the resonator, an approximate differential equation of the eigenmodes ~n(x) can be derived from the following second and third equations:
[ (d21!n)/(dx2) ] + (En--V(x) )~I!n =
where the potential V(x) is proportional to the phase profile of the mirror and is related to the specified beam ~O(X) by:
V(x) = [l/~o(x)][(d2~o)/(dx2)]
These last two equations form a useful tool in order to specify a beam ~O(X) that results in a potential V(x) having a low number of confined eigenmode solutions of the second equation. For example, for ~O(X) = sech x, all the other modes ~n are unconfined resulting in high loss and highly perturbed by diffraction. This resonator has therefore only one transverse confined mode of the stable type and all the other higher modes are of the unstable type (unconfined). Although this differential equation is only approximated, it gives good information that can be confirmed by numerical calculation of the integral equation on the computer.
The fundamental eigenmode of the resonator being of the stable type characterized by a geometrical parameter G, all the optimized parameter relations for thermal lensing compensation do apply by simply changing the geometrical parameter G of the stable resonator by G of the above-mentioned first equation.
The beam ~O(x) used to generate the CPCM was specified onto the output coupler in the previous description of the resonator. However, the beam ~O(X) can be specified at any place inside or outside the resonator and the CPCM be designed by taking into account the extra propagation.
Two super-Gaussian output resonators have been demonstrated for a pulsed TEA-C02 laser and CW-C02 laser using the present design procedure. As shown on Figure 3, the resonator is formed by a CPCM 4 and the output coupler 6 separated by a distance of 2 meters. The value of h is 17 mm. No additional optical elements were located inside the resonator, which means that the constants A and D equal 1, and B = L. The two CPCM profiles were generated according to the procedure described above for a specified output on the coupler ~O(x). Accordingly, for a first design procedure:
~ ( 1 -(x/3)~
where x is in millimeters, the distance L and B are substantially two meters, the constants A and D are 1, and ~ is substantially 10.6 micrometers. The profile of this mirror is shown more specifically on Figure 4.
For a second design procedure, it has been determined that:
~ ( ) _(X/3-5)6 where x is in millimeters, the distance L and B are substantially two meters, the constants A and D are 1, and A is substantially 10.6 micrometers. The profile of this mirror is shown more specifically on Figure 5.
It should be noted that these two resonators have a geometrical parameter G = 0.5. The resonator formed by the mirror shown in Figure 4, with a plane coupler, is a
TO BE USED IN A LASER R~ONATOR THAT WILL SUIT
~Yh~l~lCATIONS OF A USER AND A CUSTOM PHASE-CONJUGATED
CIRCULAR MIRROR HADE AcrQRnING TO THE PROCESS
s FIELD OF THE INVENTION
The present invention relates to a process for making a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user, to a process for making a custom laser resonator that will suit specifications of the user, to a custom phase-conjugated circular mirror made according to the above-mentioned process, and to a custom laser resonator made according to the above-mentioned process.
RA~r7~ouND OF THE INVENTION
Known in the art, there is the U.S. patent no.
4,803,694 of Chun-Sheu LEE et al., granted on February 7, 1989, wherein there is described a laser resonator having a cavity for the propagation of a laser beam having a wavefront in which a laser medium is positioned, comprising an aspherical concave mirror means disposed in the cavity facing an optical means for reflecting the expanded wavefront toward the lasing medium and correcting wavefront aberrations induced when the laser beam passes through the laser medium. The geometry of the aspherical concave mirror is defined by a predetermined equation.
This patent does not provide the necessary means or the necessary method steps by which a user can determine specifications from which a custom phase-conjugated circular mirror or a laser resonator including such mirror can be made. ~
Also known in the art, there is the U.S. patents nos. 4,233,571; 4,529,273; 4,715,689; and 4,750,818, describing different conjugated mirrors, and lasers including such mirrors. But none of these patents describes the necessary means or the necessary method steps by which a user can determine specifications from which a conjugated mirror or a laser including such mirror can be made.
OBJECTS OF THE INVENTION
It is an object of the present invention to provide the necessary means or the necessary method steps by which a user can determine specifications from which a custom phase-conjugated circular mirror or a laser resonator including such mirror can be provided.
SUMHARY OF THE INVENTION
According to the present invention, there is provided a process for making a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user, said mirror reversing wavefront of one particular input beam ~O(X) determined by said user, said input beam ~O(x) having a given wavelength, said laser resonator including said mirror and an output coupler cooperating with said mirror and separated therefrom by a laser gain medium, said mirror being at a distance L
from said output coupler, said process comprising steps of:
(a) determining said input beam ~O(X) that will suit need of said user;
(b) calculating equation of ~L ( X ) which is a value of said input beam ~O(x) that is propagated through said laser gain medium at said distance L, where:
~ (x) = (~)/(lB)I ~(~)e(~i~/AB)(A~2 + Dx2)J[(2~x~ B]xd~
o where A, B and D are constants determined by optical elements in said laser gain medium, xO is an integration variable, x is radial distance in transverse direction of propagation, and JO is a Bessel function of zero order;
(c) calculating phase ~O(X) of said input beam, which is a phase of said input beam ~O(x) at said distance L, where:
~L(x) = ¦~L(X)¦ e (2~ O(X) said phase ~O(X) determining profile of said custom phase-conjugated mirror; and (d) fabricating said custom phase-conjugated mirror according to said profile determined in step (c), whereby a custom phase-conjugated mirror can be provided to suit said specifications of said user.
Also according to the present invention, there is provided a process for making a custom laser resonator that will suit specifications of a user, said laser including a phase conjugated circular mirror which reverses wavefront of one particular input beam ~O(x) determined by said user, said input beam ~O(X) having a given wavelength, said laser resonator including an output coupler cooperating with said mirror and separated therefrom by a laser gain medium, said mirror being at a distance L from said output coupler, said process comprising steps of:
(a) determining said input beam ~O(X) that will suit need of said user;
(b) calculating equation of ~L(X) which is a value of said input beam ~O(X) that is propagated through said laser gain medium at said distance L, where:
L( ) (i2~)/(AB)l ~0(xo)e(~ B)(Axo2 + DX2)J[(2 )/
where A, B and D are constants determined by optical elements in said laser gain medium, xO is an integration variable, x is radial distance in transverse direction of propagation, and JO is a Bessel function of zero order;
(c) calculating phase ~O(X) of said input beam, which is a phase of said input beam ~O(X) at said distance L, where:
~L(x) = I~L(X)I e (2~/A) ~O(X) said phase ~O(X) determining profile of said custom phase-conjugated mirror; and (d) fabricating said custom phase-conjugated mirror according to said profile determined in step (c), whereby a custom laser resonator can be provided to suit said specifications of said user.
Also according to the present invention, there is provided a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user, said mirror reversing wavefront of one particular input beam YO(X) determined by said user, said input beam (X) having a given wavelength, said laser resonator including said mirror and an output coupler cooperating with said mirror and separated therefrom by a laser gain medium, said mirror being at a distance L from said output coupler, said mirror having a profile determined by ~O(X) where:
~L(x) = ¦~L(X)¦ e i(2~/~) ~O(X) where:
() (i2~)l(AB)l ~0(xo)e(-i~lAB)(~2 + Dxl)J[(2 20~734g2 where A, B and D are constants determined by optical elements in said laser gain medium, xO is an integration variable, x is radial distance in transverse direction of propagation, and JO is a Bessel function of zero order:
whereby a custom phase-conjugated mirror can be provided to suit said specifications of said user.
Also according to the present invention, there is provided a custom laser resonator that will suit specifications of a user, said laser including a phase conjugated circular mirror which reverses wavefront of one particular input beam ~O(X) determined by said user, said input beam ~O(X) having a given wavelength, said laser resonator including an output coupler cooperating with said mirror and separated therefrom by a laser gain medium, said mirror being at a distance L from said output coupler, said mirror having a profile determined by ~O(X) where:
~L( X) = ¦ ~L(X) ¦ e (2~/~) ~O(X) where:
00 . 2 2 ~L(X) (i2~)/(AB)l ~o(xo)e(-l~lAB)(Axo + Dx)J[(2 )/A
0 .
where A, B and D are constants determined by optical elements in said laser gain medium, xO is an integration variable, x is radial distance in transverse direction of propagation, and JO is a Bessel function of zero order;
whereby a custom laser resonator can be provided to suit said specifications of said user.
The objects, advantages and other features of the present invention will become more apparent upon reading of the following non restrictive description of preferred embodiment thereof, given for the purpose of exemplification only with reference to the accompanying drawings.
2073~92 BRIEF DESCRIPTION OF THE DRAWINGS
Figure 1 is a schematic diagram illustrating the relation between a specified input beam ~O(X) with respect to a custom phase-conjugated mirror;
Figure 2 is a schematic diagram illustrating a custom phase-conjugated mirror laser resonator;
Figure 3 is a schematic diagram illustrating a laser resonator made according to the present invention;
Figure 4 is a diagram illustrating ~O(X) with respect to x for a given mirror; and Figure 5 is a diagram illustrating ~O(X) with respect to x for another given mirror.
DETATT.~n DESCRIPTION OF TH~ DRAWINGS
Referring now to Figure 1, there is shown a schematic diagram illustrating the relation between a specified input beam ~O(x)~ a laser gain medium including an optical system 2, a custom phase-conjugated mirror 4 and the distance L. The process for making a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications o~ a user will be described by means of Figure 1. The mirror 4 reverses wavefront of one particular input beam ~O(X) determined by the user. The input beam ~O(X) has a given wavelength A. The laser resonator includes the mirror 4 and an output coupler (not shown in this Figure 1) cooperating with the mirror 4 and separate therefrom by a laser gain medium including optical elements 2. The mirror 4 is at a distance L from the output coupler (shown in Figure 2). The process comprises steps of (a) determining the input beam ~O(X) that will suit need of the user; (b) calculating equation of ~L(x) which is a value of the input beam ~O(X) that is propagated through the laser gain medium at the distance L, where:
2073~92 ~ (x) = (i2~)t(~B)¦ ~(x)e(~i~/AB)(A~2 + DX2)J[(2~xx)/~B]xdx where A, B and D are constants determined by the optical elements 2 in the laser gain medium, xO is an integration variable, x is radial distance in transverse direction of propagation, and JO is a Bessel function of zero order; (c) calculating phase ~O(X) of the input beam, which is a phase of the input beam ~O(x) at the distance L, where:
~L(x) = ¦~L(X)¦ e i(2~/A) ~O(X) the phase ~O(X) determining profile of the custom phase-conjugated mirror; and (d) fabricating the custom phase-conjugated mirror according to the profile determined in step (c), whereby a custom phase-conjugated mirror can be provided to suit the specifications of the user.
When the mirror has a slab geometry, ~(x) can be determined by the following equation:
~L(X) = (i/~B)l/2 1 ~O(xo)e[-i(~/~B) (Axo2 - 2xox + Dx2)] d _~
The phase-conjugated mirror (PCM) is an optical component that reverses the wavefront of an incoming beam.
A custom phase-conjugated mirror (CPCM) is an optical component that reverses wavefront of only one particular beam previously specified by the user.
The design of a CPCM proceeds as follows:
- first, the specified beam ~O(X) is propagated through the optical system 2 till a distance L using, for example, the Huygen-Fresnel integral operator:
~ (x) = (~)/(AB)I ~(X)e(~~ B)(A~2 + DX2)J~(2~xx)/AB]xdx where A is the wavelength of the beam. The above-mentioned equation has been written here for only one transverse dimension x. However, the generalization of two transverse dimensions is immediate;
- second, the phase ~O(X) of this propagated complex beam is extracted according to:
~L(x) = ¦~L(X)¦ e i(2~/A) ~O(X) - third, a mirror is fabricated according to this profile ~O(x) using the appropriate technique for a given wavelength A.
As a consequence of this design procedure, in general, any other beam than the specified one ~O(X), that passes through the same optical system 2 will, after reflection by the CPCM, diverge. Only the specified beam (X) will, after reflection and passage through the same optical system 2, be completely phase-conjugated (reversed), resulting in a nearly exact replica of the specified beam (X) at the same plane z = 0.
This feature can be used to optimize many optical systems. An example is an optical laser resonator.
Referring now to Figure 2, there is shown a schematic diagram illustrating such laser resonator. The laser resonator is an open resonator formed by a reflecting mirror 4 and an output coupler 6 enclosing a laser gain medium including optical components 2. The laser resonator is made here with a CPCM 4 and an output coupler 6 enclosing an optical system 2. According to the theory of CPCM, the specified beam ~O(x) used to design the CPCM Will necessarily be a low loss eigenmode of the resonator when the CPCM 4 has a large enough transverse dimension. This eigenmode will be of the stable type and the resonator can be described by a generalized G parameter related to the beam size (RMS)Wo of the specified beam ~O(X), namely by the following first equation:
WO2 = MZ[ (AL)/~] [G/(1-G)]1/2 where M2 is the beam quality factor.
Appropriate specification of the beam ~O(X) will lead to a large low loss fundamental eigenmode that improves the efficiency of the laser system. The discrimination feature of the laser resonator can be assessed by solving the usual eigen Huygen-Fresnel integral equation on a computer. For the practical situation of short length (L) of the resonator, an approximate differential equation of the eigenmodes ~n(x) can be derived from the following second and third equations:
[ (d21!n)/(dx2) ] + (En--V(x) )~I!n =
where the potential V(x) is proportional to the phase profile of the mirror and is related to the specified beam ~O(X) by:
V(x) = [l/~o(x)][(d2~o)/(dx2)]
These last two equations form a useful tool in order to specify a beam ~O(X) that results in a potential V(x) having a low number of confined eigenmode solutions of the second equation. For example, for ~O(X) = sech x, all the other modes ~n are unconfined resulting in high loss and highly perturbed by diffraction. This resonator has therefore only one transverse confined mode of the stable type and all the other higher modes are of the unstable type (unconfined). Although this differential equation is only approximated, it gives good information that can be confirmed by numerical calculation of the integral equation on the computer.
The fundamental eigenmode of the resonator being of the stable type characterized by a geometrical parameter G, all the optimized parameter relations for thermal lensing compensation do apply by simply changing the geometrical parameter G of the stable resonator by G of the above-mentioned first equation.
The beam ~O(x) used to generate the CPCM was specified onto the output coupler in the previous description of the resonator. However, the beam ~O(X) can be specified at any place inside or outside the resonator and the CPCM be designed by taking into account the extra propagation.
Two super-Gaussian output resonators have been demonstrated for a pulsed TEA-C02 laser and CW-C02 laser using the present design procedure. As shown on Figure 3, the resonator is formed by a CPCM 4 and the output coupler 6 separated by a distance of 2 meters. The value of h is 17 mm. No additional optical elements were located inside the resonator, which means that the constants A and D equal 1, and B = L. The two CPCM profiles were generated according to the procedure described above for a specified output on the coupler ~O(x). Accordingly, for a first design procedure:
~ ( 1 -(x/3)~
where x is in millimeters, the distance L and B are substantially two meters, the constants A and D are 1, and ~ is substantially 10.6 micrometers. The profile of this mirror is shown more specifically on Figure 4.
For a second design procedure, it has been determined that:
~ ( ) _(X/3-5)6 where x is in millimeters, the distance L and B are substantially two meters, the constants A and D are 1, and A is substantially 10.6 micrometers. The profile of this mirror is shown more specifically on Figure 5.
It should be noted that these two resonators have a geometrical parameter G = 0.5. The resonator formed by the mirror shown in Figure 4, with a plane coupler, is a
2~73~92 classical stable semi-confocal resonator.
These mirrors can be fabricated by using the diamond-turning technique on a cooper substrate. The CPCM
aperture is limited here to a Fresnel number of 3.5 by the gain medium transverse dimension.
For the TEA-C02 laser, the output energy in monomode operation is 690 mJ and 750 mJ for the mirrors shown respectively on Figures 4 and 5. This corresponds to an increase of laser efficiency of 40% and 50% for the mirrors shown respectively on Figures 4 and 5 as compared to a classical resonator.
For the CW-C02, the power output in monomode operation is 5.9 watts and 6.4 watts for the mirrors shown respectively on Figures 4 and 5, which corresponds to an increase of laser efficiency of 18% and 28% as compared to a standard resonator.
The super-Gaussian output of the resonator including the mirrors shown respectively on Figures 4 and 5 has much lower diffraction rings in the near field than a standard Gaussian output resonator.
Accordingly, there is provided a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user. The mirror reverses wavefront of one particular input beam ~O(X) determined by said user, the input beam ~O(x) having a given wavelength, the laser resonator including the mirror and an output coupler cooperating with the mirror and separated therefrom by a laser gain medium, the mirror being at a distance L
from the output coupler, the mirror having a profile determined by ~O(X) where:
~L(X) = ¦~L(X)¦ e ( /A) ~O(X) where:
( ~)/(~B)I ~0(xo)e(~ B)(Axo2 + Dx2)J[(2 2~734g2 where A, B and D are constants determined by optical elements in said laser gain medium, xO is an integration variable, x is radial distance in transverse direction of propagation, and JO is a Bessel function of zero order;
whereby a custom phase-conjugated mirror can be provided to suit said specifications of said user.
Also, there is provided a custom laser resonator that will suit specifications of a user, the laser including the phase conjugated circular mirror mentioned above.
Although the present invention has been explained hereinabove by way of a preferred embodiment thereof, it should be pointed out that any modifications to this preferred embodiment within the scope of the appended claims is not deemed to alter or change the nature and scope of the present invention.
These mirrors can be fabricated by using the diamond-turning technique on a cooper substrate. The CPCM
aperture is limited here to a Fresnel number of 3.5 by the gain medium transverse dimension.
For the TEA-C02 laser, the output energy in monomode operation is 690 mJ and 750 mJ for the mirrors shown respectively on Figures 4 and 5. This corresponds to an increase of laser efficiency of 40% and 50% for the mirrors shown respectively on Figures 4 and 5 as compared to a classical resonator.
For the CW-C02, the power output in monomode operation is 5.9 watts and 6.4 watts for the mirrors shown respectively on Figures 4 and 5, which corresponds to an increase of laser efficiency of 18% and 28% as compared to a standard resonator.
The super-Gaussian output of the resonator including the mirrors shown respectively on Figures 4 and 5 has much lower diffraction rings in the near field than a standard Gaussian output resonator.
Accordingly, there is provided a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user. The mirror reverses wavefront of one particular input beam ~O(X) determined by said user, the input beam ~O(x) having a given wavelength, the laser resonator including the mirror and an output coupler cooperating with the mirror and separated therefrom by a laser gain medium, the mirror being at a distance L
from the output coupler, the mirror having a profile determined by ~O(X) where:
~L(X) = ¦~L(X)¦ e ( /A) ~O(X) where:
( ~)/(~B)I ~0(xo)e(~ B)(Axo2 + Dx2)J[(2 2~734g2 where A, B and D are constants determined by optical elements in said laser gain medium, xO is an integration variable, x is radial distance in transverse direction of propagation, and JO is a Bessel function of zero order;
whereby a custom phase-conjugated mirror can be provided to suit said specifications of said user.
Also, there is provided a custom laser resonator that will suit specifications of a user, the laser including the phase conjugated circular mirror mentioned above.
Although the present invention has been explained hereinabove by way of a preferred embodiment thereof, it should be pointed out that any modifications to this preferred embodiment within the scope of the appended claims is not deemed to alter or change the nature and scope of the present invention.
Claims (16)
1. A process for making a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user, said mirror reversing wavefront of one particular input beam ?o(x) determined by said user, said input beam ?o(x) having a given wavelength, said laser resonator including said mirror and an output coupler cooperating with said mirror and separated therefrom by a laser gain medium, said mirror being at a distance L
from said output coupler, said process comprising steps of:
(a) determining said input beam ?o(x) that will suit need of said user;
(b) calculating equation of ?L(x) which is a value of said input beam ?o(x) that is propagated through said laser gain medium at said distance L, where:
?L(x)= (i2.pi.)/(.lambda.B) ?o(xo)e(-i.pi./.lambda.B)(Axo2 + Dx2)Jo[(2.pi.xxo)/.lambda.B]xodxo where A, B and D are constants determined by optical elements in said laser gain medium, xo is an integration variable, x is radial distance in transverse direction of propagation, and Jo is a Bessel function of zero order;
(c) calculating phase .PHI.o(x) of said input beam, which is a phase of said input beam ?o(x) at said distance L, where:
?L(X) = ¦ ?L(X) ¦ e-i(2.pi./.lambda.) .PHI.o(x) said phase .PHI.o(x) determining profile of said custom phase-conjugated mirror; and (d) fabricating said custom phase-conjugated mirror according to said profile determined in step (c), whereby a custom phase-conjugated mirror can be provided to suit said specifications of said user.
from said output coupler, said process comprising steps of:
(a) determining said input beam ?o(x) that will suit need of said user;
(b) calculating equation of ?L(x) which is a value of said input beam ?o(x) that is propagated through said laser gain medium at said distance L, where:
?L(x)= (i2.pi.)/(.lambda.B) ?o(xo)e(-i.pi./.lambda.B)(Axo2 + Dx2)Jo[(2.pi.xxo)/.lambda.B]xodxo where A, B and D are constants determined by optical elements in said laser gain medium, xo is an integration variable, x is radial distance in transverse direction of propagation, and Jo is a Bessel function of zero order;
(c) calculating phase .PHI.o(x) of said input beam, which is a phase of said input beam ?o(x) at said distance L, where:
?L(X) = ¦ ?L(X) ¦ e-i(2.pi./.lambda.) .PHI.o(x) said phase .PHI.o(x) determining profile of said custom phase-conjugated mirror; and (d) fabricating said custom phase-conjugated mirror according to said profile determined in step (c), whereby a custom phase-conjugated mirror can be provided to suit said specifications of said user.
2. A process according to claim 1, wherein said mirror has a slab geometry; wherein:
?L(x)= (i/.lambda.B) ?o(xo)e [-i(.pi./.lambda.B) (Axo2 - 2xox + Dx2)] dxo.
?L(x)= (i/.lambda.B) ?o(xo)e [-i(.pi./.lambda.B) (Axo2 - 2xox + Dx2)] dxo.
3. A process according to claim 1, wherein:
?o(x)=e-(x/3)4 wherein x is in millimeters; and wherein said distance L and B are substantially two meters, said constants A and D are 1, and .lambda. is substantially 10.6 micrometers.
?o(x)=e-(x/3)4 wherein x is in millimeters; and wherein said distance L and B are substantially two meters, said constants A and D are 1, and .lambda. is substantially 10.6 micrometers.
4. A process according to claim 1, wherein:
?o(x)=e-(X/3-5)6 wherein x is in millimeters; and wherein said distance L and B are substantially two meters, said constants A and D are 1, and .lambda. is substantially 10.6 micrometers.
?o(x)=e-(X/3-5)6 wherein x is in millimeters; and wherein said distance L and B are substantially two meters, said constants A and D are 1, and .lambda. is substantially 10.6 micrometers.
5. A process for making a custom laser resonator that will suit specifications of a user, said laser including a phase conjugated circular mirror which reverses wavefront of one particular input beam ?o(x) determined by said user, said input beam ?o(x) having a given wavelength, said laser resonator including an output coupler cooperating with said mirror and separated therefrom by a laser gain medium, said mirror being at a distance L from said output coupler, said process comprising steps of:
(a) determining said input beam ?o(x) that will suit need of said user;
(b) calculating equation of ?L(X) which is a value of said input beam ?o(x) that is propagated through said laser gain medium at said distance L, where:
?L(x) = (i2.pi.)/(.lambda.B) ?o(xo)e(-i.pi./.lambda.B)(Axo2 + Dx2)Jo[(2.pi.xxo)/.lambda.B]xodxo where A, B and D are constants determined by optical elements in said laser gain medium, xo is an integration variable, x is radial distance in transverse direction of propagation, and Jo is a Bessel function of zero order;
(c) calculating phase .PHI.o(x) of said input beam, which is a phase of said input beam ?o(x) at said distance L, where:
?L(x) = ¦?L(X)¦ e-i(2.pi./.lambda.) .PHI.o(x) said phase .PHI.o(x) determining profile of said custom phase-conjugated mirror; and (d) fabricating said custom phase-conjugated mirror according to said profile determined in step (c), whereby a custom laser resonator can be provided to suit said specifications of said user.
(a) determining said input beam ?o(x) that will suit need of said user;
(b) calculating equation of ?L(X) which is a value of said input beam ?o(x) that is propagated through said laser gain medium at said distance L, where:
?L(x) = (i2.pi.)/(.lambda.B) ?o(xo)e(-i.pi./.lambda.B)(Axo2 + Dx2)Jo[(2.pi.xxo)/.lambda.B]xodxo where A, B and D are constants determined by optical elements in said laser gain medium, xo is an integration variable, x is radial distance in transverse direction of propagation, and Jo is a Bessel function of zero order;
(c) calculating phase .PHI.o(x) of said input beam, which is a phase of said input beam ?o(x) at said distance L, where:
?L(x) = ¦?L(X)¦ e-i(2.pi./.lambda.) .PHI.o(x) said phase .PHI.o(x) determining profile of said custom phase-conjugated mirror; and (d) fabricating said custom phase-conjugated mirror according to said profile determined in step (c), whereby a custom laser resonator can be provided to suit said specifications of said user.
6. A process according to claim 5, wherein said mirror has a slab geometry; wherein:
?L(x)= (i /.lambda.B) ?o(xo)e[-i(.pi./.lambda.B) (Axo2 - 2xox + Dx2)] dxo.
?L(x)= (i /.lambda.B) ?o(xo)e[-i(.pi./.lambda.B) (Axo2 - 2xox + Dx2)] dxo.
7. A process according to claim 5, wherein:
?o(x)=e-(x/3)4 wherein x is in millimeters; and wherein said distance L and B are substantially two meters, said constants A and D are 1, and .lambda. is substantially 10.6 micrometers.
?o(x)=e-(x/3)4 wherein x is in millimeters; and wherein said distance L and B are substantially two meters, said constants A and D are 1, and .lambda. is substantially 10.6 micrometers.
8. A process according to claim 5, wherein:
?o(x)=e-(x/3.5)6 wherein x is in millimeters; and wherein said distance L and B are substantially two meters, said constants A and D are 1, and .lambda. is substantially 10.6 micrometers.
?o(x)=e-(x/3.5)6 wherein x is in millimeters; and wherein said distance L and B are substantially two meters, said constants A and D are 1, and .lambda. is substantially 10.6 micrometers.
9. A custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user, said mirror reversing wavefront of one particular input beam ?o(x) determined by said user, said input beam ?o(x) having a given wavelength, said laser resonator including said mirror and an output coupler cooperating with said mirror and separated therefrom by a laser gain medium, said mirror being at a distance L from said output coupler, said mirror having a profile determined by .PHI.o(x) where:
?L(x) = ¦?L(x)¦ e-i(2.pi./.lambda.) .PHI.o(x) where:
?L(x)= (i2.pi.)/(.lambda.B) ?o(xo)e(-i.pi./.lambda.B)(Axo2 + Dx2)Jo[(2.pi.xxo)/.lambda.B]xodxo where A, B and D are constants determined by optical elements in said laser gain medium, xo is an integration variable, x is radial distance in transverse direction of propagation, and Jo is a Bessel function of zero order;
whereby a custom phase-conjugated mirror can be provided to suit said specifications of said user.
?L(x) = ¦?L(x)¦ e-i(2.pi./.lambda.) .PHI.o(x) where:
?L(x)= (i2.pi.)/(.lambda.B) ?o(xo)e(-i.pi./.lambda.B)(Axo2 + Dx2)Jo[(2.pi.xxo)/.lambda.B]xodxo where A, B and D are constants determined by optical elements in said laser gain medium, xo is an integration variable, x is radial distance in transverse direction of propagation, and Jo is a Bessel function of zero order;
whereby a custom phase-conjugated mirror can be provided to suit said specifications of said user.
10. A mirror according to claim 9, wherein said mirror has a slab geometry; wherein:
?L(x) = (i /.lambda.B) ?o(xo)e[-i(.pi./.lambda.B) (Axo2 - 2xox + Dx2)] dxo.
?L(x) = (i /.lambda.B) ?o(xo)e[-i(.pi./.lambda.B) (Axo2 - 2xox + Dx2)] dxo.
11. A mirror according to claim 9, wherein:
?o(x)=e-(x/3)4 wherein x is in millimeters; and wherein said distance L and B are substantially two meters, said constants A and D are 1, and .lambda. is substantially 10.6 micrometers.
?o(x)=e-(x/3)4 wherein x is in millimeters; and wherein said distance L and B are substantially two meters, said constants A and D are 1, and .lambda. is substantially 10.6 micrometers.
12. A mirror according to claim 9, wherein:
?o(X)=e-(X/3.5)6 wherein x is in millimeters; and wherein said distance L and B are substantially two meters, said constants A and D are 1, and .lambda. is substantially 10.6 micrometers.
?o(X)=e-(X/3.5)6 wherein x is in millimeters; and wherein said distance L and B are substantially two meters, said constants A and D are 1, and .lambda. is substantially 10.6 micrometers.
13. A custom laser resonator that will suit specifications of a user, said laser including a phase conjugated circular mirror which reverses wavefront of one particular input beam ?o(x) determined by said user, said input beam ?o(x) having a given wavelength, said laser resonator including an output coupler cooperating with said mirror and separated therefrom by a laser gain medium, said mirror being at a distance L from said output coupler, said mirror having a profile determined by .PHI.o(x) where:
?L(x) = ¦?L(x) e-i(2.pi./.lambda.) .PHI.o(x) where:
?L(x) = (i2µ)/(.lambda.B) ?o(xo)e(-i.pi./.lambda.B)(Axo2 + Dx2)Jo[(2.pi.xxo)/.lambda.B]xodxo where A, B and D are constants determined by optical elements in said laser gain medium, xo is an integration variable, x is radial distance in transverse direction of propagation, and Jo is a Bessel function of zero order;
whereby a custom laser resonator can be provided to suit said specifications of said user.
?L(x) = ¦?L(x) e-i(2.pi./.lambda.) .PHI.o(x) where:
?L(x) = (i2µ)/(.lambda.B) ?o(xo)e(-i.pi./.lambda.B)(Axo2 + Dx2)Jo[(2.pi.xxo)/.lambda.B]xodxo where A, B and D are constants determined by optical elements in said laser gain medium, xo is an integration variable, x is radial distance in transverse direction of propagation, and Jo is a Bessel function of zero order;
whereby a custom laser resonator can be provided to suit said specifications of said user.
14. A laser resonator according to claim 13, wherein said mirror has a slab geometry; wherein:
?L(x) = (i/.lambda.B) ?o(xo)e[-i(.pi./.lambda.B) (Axo2 - 2xox + Dx2)] dxo.
?L(x) = (i/.lambda.B) ?o(xo)e[-i(.pi./.lambda.B) (Axo2 - 2xox + Dx2)] dxo.
lS. A laser resonator according to claim 13, wherein:
?o(X)=e-(x/3)4 wherein x is in millimeters; and wherein said distance L and B are substantially two meters, said constants A and D are 1, and .lambda. is substantially 10.6 micrometers.
?o(X)=e-(x/3)4 wherein x is in millimeters; and wherein said distance L and B are substantially two meters, said constants A and D are 1, and .lambda. is substantially 10.6 micrometers.
16. A laser resonator according to claim 13, wherein:
?o(x)=e-(x/3.5)6 wherein x is in millimeters; and wherein said distance L and B are substantially two meters, said constants A and D are 1, and .lambda. is substantially 10.6 micrometers.
?o(x)=e-(x/3.5)6 wherein x is in millimeters; and wherein said distance L and B are substantially two meters, said constants A and D are 1, and .lambda. is substantially 10.6 micrometers.
Priority Applications (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US07/906,358 US5255283A (en) | 1992-06-30 | 1992-06-30 | Process for making a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user and a custom phase-conjugated circular mirror made according to the process |
| CA002073492A CA2073492C (en) | 1992-06-30 | 1992-07-08 | Process for making a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user and a custom phase-conjugated circular mirror made according to the process |
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US07/906,358 US5255283A (en) | 1992-06-30 | 1992-06-30 | Process for making a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user and a custom phase-conjugated circular mirror made according to the process |
| CA002073492A CA2073492C (en) | 1992-06-30 | 1992-07-08 | Process for making a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user and a custom phase-conjugated circular mirror made according to the process |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CA2073492A1 CA2073492A1 (en) | 1994-01-09 |
| CA2073492C true CA2073492C (en) | 1996-12-17 |
Family
ID=25675313
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA002073492A Expired - Fee Related CA2073492C (en) | 1992-06-30 | 1992-07-08 | Process for making a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user and a custom phase-conjugated circular mirror made according to the process |
Country Status (2)
| Country | Link |
|---|---|
| US (1) | US5255283A (en) |
| CA (1) | CA2073492C (en) |
Families Citing this family (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5454004A (en) * | 1994-05-06 | 1995-09-26 | Regents Of The University Of Minnesota | Phase grating and mode-selecting mirror for a laser |
| WO1995031024A2 (en) * | 1994-05-06 | 1995-11-16 | Regents Of The University Of Minnesota | Optical element for a laser |
| US5627847A (en) * | 1995-05-04 | 1997-05-06 | Regents Of The University Of Minnesota | Distortion-compensated phase grating and mode-selecting mirror for a laser |
| US5880873A (en) * | 1997-05-16 | 1999-03-09 | The Regents Of The University Of California | All solid-state SBS phase conjugate mirror |
| US6614585B1 (en) * | 1999-05-06 | 2003-09-02 | Trumpf Photonics Inc. | Phase conjugating structure for mode matching in super luminescent diode cavities |
| US6195379B1 (en) * | 1999-12-27 | 2001-02-27 | Synrad, Inc. | Laser assembly system and method |
| US20010033588A1 (en) * | 1999-12-27 | 2001-10-25 | Broderick Jeffery A. | Laser system and method for beam enhancement |
| US6198759B1 (en) * | 1999-12-27 | 2001-03-06 | Synrad, Inc. | Laser system and method for beam enhancement |
| US6198758B1 (en) * | 1999-12-27 | 2001-03-06 | Synrad, Inc. | Laser with heat transfer system and method |
| US6879616B2 (en) * | 2003-01-24 | 2005-04-12 | Trumpf, Inc. | Diffusion-cooled laser system |
Family Cites Families (10)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4233571A (en) * | 1978-09-27 | 1980-11-11 | Hughes Aircraft Company | Laser having a nonlinear phase conjugating reflector |
| US4500855A (en) * | 1982-06-10 | 1985-02-19 | University Of Southern California | Phase conjugation using internal reflection |
| US4529273A (en) * | 1982-12-21 | 1985-07-16 | California Institute Of Technology | Passive phase conjugate mirror |
| US4709368A (en) * | 1985-09-24 | 1987-11-24 | The United States Of America As Represented By The Secretary Of The Army | Side-arm phase-conjugated laser |
| US4750818A (en) * | 1985-12-16 | 1988-06-14 | Cochran Gregory M | Phase conjugation method |
| US4794605A (en) * | 1986-03-13 | 1988-12-27 | Trw Inc. | Method and apparatus for control of phase conjugation cells |
| US4720176A (en) * | 1986-05-20 | 1988-01-19 | Hughes Aircraft Company | Erase beam apparatus and method for spatial intensity threshold detection |
| US4715689A (en) * | 1986-05-20 | 1987-12-29 | Hughes Aircraft Company | Apparatus and method for spatial intensity threshold detection |
| US4803694A (en) * | 1987-07-08 | 1989-02-07 | Amada Company, Limited | Laser resonator |
| US4875219A (en) * | 1988-11-28 | 1989-10-17 | The United States Of America As Represented By The Secretary Of The Army | Phase-conjugate resonator |
-
1992
- 1992-06-30 US US07/906,358 patent/US5255283A/en not_active Expired - Fee Related
- 1992-07-08 CA CA002073492A patent/CA2073492C/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| US5255283A (en) | 1993-10-19 |
| CA2073492A1 (en) | 1994-01-09 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| Magni et al. | ABCD matrix analysis of propagation of Gaussian beams through Kerr media | |
| US5553093A (en) | Dispersion-compensated laser using prismatic end elements | |
| US5025446A (en) | Intra-cavity beam relay for optical harmonic generation | |
| US5079772A (en) | Mode-locked laser using non-linear self-focusing element | |
| US4803694A (en) | Laser resonator | |
| CA2073492C (en) | Process for making a custom phase-conjugated circular mirror to be used in a laser resonator that will suit specifications of a user and a custom phase-conjugated circular mirror made according to the process | |
| US20060114947A1 (en) | Solid-state laser generator | |
| US5097471A (en) | Mode-locked laser using non-linear self-focusing element | |
| Oron et al. | Laser mode discrimination with intra-cavity spiral phase elements | |
| ATE369641T1 (en) | TUNABLE HIGH POWER LASER | |
| Paré et al. | Custom laser resonators using graded-phase mirrors: circular geometry | |
| EP0886897B1 (en) | Optical resonator with spiral optical elements | |
| GB1083534A (en) | Improvements in or relating to optical masers | |
| Gerber et al. | Generation of super-Gaussian modes in Nd: YAG lasers with a graded-phase mirror | |
| Arabgari et al. | Thin-disk laser resonator design: The dioptric power variation of thin-disk and the beam quality factor | |
| EP0979546A1 (en) | Optical resonators with discontinuous phase elements | |
| US6285705B1 (en) | Solid-state laser oscillator and machining apparatus using the same | |
| Kitano et al. | Stable multipulse generation from a self-mode-locked Ti: sapphire laser | |
| US6289029B1 (en) | Solid state laser | |
| Huang et al. | Analytical design for Kerr-lens mode locking of compact solid-state lasers | |
| Kim et al. | Stable range enhancement in a symmetric confocal two-rod resonator with 90 optical rotator | |
| Yu et al. | Optical resonator with hyperbolic-cosine-Gaussian modes | |
| RU2069430C1 (en) | Laser stable resonator | |
| Barnes et al. | Ti: Al2O3 Laser Pumped by a Frequency Doubled Nd: YAG Laser | |
| Marczak | Designs of the resonators increasing the efficiency of laser oscillators |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| EEER | Examination request | ||
| MKLA | Lapsed |