Unstable laser resonator

Claim 2

An unstable laser resonator including two spherical mirrors spaced apart and disposed about a laser active medium so as to provide a collimated output beam with rotationally unsymmetrical magnification, distinguished by the fact that in the light paths between the spherical mirrors are at least two other optical elements with cylindrical surfaces, whose cylindrical axes are essentially perpendicular to each other.

Claim 3

An unstable laser resonator in accordance with claim 1, distinguished by the fact that said optical elements are mirrors.

Claim 4

An unstable laser resonator in accordance with claim 1, distinguished by the fact that said optical elements are lenses.

Claim 5

An unstable laser resonator in accordance with claim 3, distinguished by the fact that at least one of said lenses simultaneously functions as a window for a container containing said active medium.

Claim 6

An unstable laser resonator in accordance with claim 1, distinguished by the fact that one or more of said light paths are lengthened as a result of the fact that one or more folds are effected in said light paths by introducing one or more plane mirrors.

Claim 7

An unstable laser resonator in accordance with claim 1, distinguished by the fact that said spherical mirrors and optical elements are so arranged that the individual light paths between said spherical mirrors and optical elements are equal.

Claim 8

An unstable laser resonator in accordance with claim 1, distinguished by the fact that the light paths penetrate said active medium only in the region between one of said optical elements and one of said spherical mirrors.

Claim 9

An unstable laser resonator in accordance with claim 1, distinguished by the fact that said optical elements and spherical mirrors are arranged in such a manner that the entire light path lies in one plane.

Claim 10

An unstable laser resonator in accordance with claim 1, distinguished by the fact that one of said optical elements is a cylindrical mirror arranged in such a manner that said beam striking it forms an angle of approximately 45° with the normal to the surface of said cylindrical, and the axis of said cylindrical lies in the plane of incidence.

Claim 11

An unstable laser resonator in accordance with claim 1, distinguished by the fact that the curvatures of the mirrors and optical elements and their spacings are so chosen that a collimated output beam is produced, and the ratio of magnifications in different directions may be varied by appropriate selection of the spacings and/or the curvatures of the mirrors and optical elements.

Claim 12

An unstable laser resonator in accordance with claim 10, distinguished by the fact that when said spherical mirrors and optical elements are so arranged that the individual light paths between said spherical mirrors and optical elements are equal, the relations indicated in FIG. 4 are established among their curvatures: where R 1 indicates the radius of one spherical, concave mirror, R 2 is the radius of one cylindrical, convex optical element, R 3 is the radius of another cylindrical, convex optical element, R 4 is the radius of another spherical, convex mirror, and L is the overall length of the light path, and where the values 1, 10 and 100 assigned to each pair of solid and broken line graph plots in the graph are for respective particular ratios of -R 4 /L, the negative signs preceding the ratios R 2 /L, R 3 /L, and R 4 /L indicating that the respective optical element or mirror is convex.

Claim 13

An unstable laser resonator in accordance with claim 11, distinguished by the fact that the ratio of the magnifications (m x , m y ) in directions perpendicular to each other result from the relations indicated in FIG. 5 in function of the quantities R 1 and R 4 : where the values 1, 10, and 100 assigned to each solid line graph plot in the latter graph are for respective particular ratios of -R 4 /L, the negative sign preceding the ratio R 4 /L indicating that the respective mirror is convex.

Claim 14

An unstable laser resonator in accordance with claim 12 distinguished by the fact that the total geometric coupling K between said spherical mirrors results from the relations indicated in FIG. 7 in function of the quantities R 1 and R 4 : and where in the last of the three graphs the values 0.2, 0.4, 1, 2, 5, 10, 20, 40, and 100 assigned to each solid line graph plot are for respective particular ratios of -R 4 /L, the negative sign preceding the ratio R 4 /L indicating that the respective mirror is convex.

Claim 15

An unstable laser resonator in accordance with claim 11 distinguished by the fact that the total geometric coupling K between said spherical mirrors results from the relations indicated in FIG. 7 in function of the quantities R 1 and R 4 : where the values 0.2, 0.4, 1, 2, 5, 10, 20, 40, and 100 assigned to each solid line graph plot in the latter graph are for respective particular ratios of -R 4 /L, the negative sign preceding the ratio R 4 /L indicating that the respective mirror is convex.

Claim 16

An unstable laser resonator in accordance with claim 1, wherein the direction of flow of said medium is in the x-direction and distinguished by the fact that the ratio of the geometric coupling, K y in the y direction which is perpendicular to the x-direction to the total geometric coupling K between said spherical mirrors as a function of the radius R 1 of one of said spherical mirrors to the light path between the cylindrical mirrors at a given radius R 4 of the other spherical mirror, when the path lengths between said spherical mirrors and said cylindrical optical elements are equal is given by the relations indicated in FIG. 8: where L signifies the overall light path and where the values 1/8, 1/3, 1/2, and 1/1 assigned to each solid line graph plot in the graph are for respective particular ratios of -R 4 /L, the negative sign preceding the ratio R 4 /L indicating that the respective mirror is convex.