In order to improve a solid-state laser comprising a resonator, at least one solid-state rod arranged in the resonator and a pumping power source for exciting the solid-state rod such that the dissipation heat can be controlled better and excitation for high powers is possible in a simple way, it is proposed that the resonator be a coupled resonator, that the resonator have two elongated excitation sections lying in one plane with one of the solid-state rods being arranged in their respective beam, that the resonator have a coupling section which the beams of the excitation sections enter as outer beams extending parallel to one another but in spaced relation to one another and which couples the excitation sections with one another by displacement of the outer beams in the plane defined by these to a coupling axis lying parallel to and between the outer beams and beyond this coupling axis, and that irradiated by the pumping power source on another side surface.

The invention relates to a solid-state laser comprising a resonator, at 
least one laser amplification volume arranged in the resonator and a pump 
means for exciting the laser amplification volume. 
In all hitherto known solid-state lasers such as optically pumped 
solid-state rod lasers or semiconductor lasers, problems arise with the 
controlling of the dissipation heat. 
when unfiltered light from gas-discharge lamps is used as pumping power 
source, one has to assume that, for example, in the case of the Nd laser 
approximately three times the obtainable laser power will remain as heat 
in the solid-state rod. This heat causes temperature gradients which in 
individual cases result in breakage of the crystals, but at any rate in 
optical deformations. For these reasons, today's solid-state lasers are 
subject to a power limit which does not permit multi-kilowatt operation if 
the beam quality is still to be good and adaptable to changing operating 
conditions. 
A further problem of the known optically excited solid-state lasers resides 
in the design of the excitation light source. With a total laser 
efficiency of a few percent, the excitation lamps have to convert up to 
100 kW if the laser is to generate a few kW laser power. This power 
concentration can only take place in larger volumes and surfaces. On the 
other hand, the emitted light has to be directed at the active medium. The 
latter should absorb the excitation light as completely as possible, which 
requires a layer thickness of several mm. 
The same problems occur with the semiconductor laser where, in addition, a 
laser-active semiconductor layer region cannot be of optional, 
large-volume configuration if purposeful laser amplification is to be 
achieved. 
In view of these disadvantages of the prior art, the object underlying the 
invention is to so improve a solid-state laser of the generic kind that it 
is suitable for generating high power. 
This object is accomplished in accordance with the invention in a 
solid-state laser comprising a laser-active unit with a laser 
amplification volume extending in a first direction in a solid, a pump 
means associated with the laser amplification volume for exciting it and a 
resonator with an excitation section which is arranged between its 
resonator mirrors and in which a beam extends in a direction of 
propagation and thereby penetrates in the laser amplification volume in 
the first direction, by at least two excitation sections being provided, 
each having one laser amplification volume, by the beams of the excitation 
sections extending in spaced relation to one another, by the resonator 
having a coupling section containing a coherent joint beam of the 
resonator, the cross-section thereof being comprised of several partial 
beams, and by an optical element being arranged between the coupling 
section and each excitation section for imaging one of the partial beams 
of the joint beam into one of the beams extending in spaced relation to 
one another in the excitation sections. 
The advantage of the inventive solution is that with this solution it is 
made possible for the beams of the individual excitation sections to be 
imaged into partial beams which, for their part, add up in cross-section 
and thereby produce a joint beam in which there is coherent radiation over 
all of the partial beams. In this way, the amplification of at least two 
laser amplification volumes can be used to generate a joint beam which as 
such is coherent and has high laser power. 
With the invention solution, it is not absolutely necessary for all of the 
partial beams of the joint beam to be imaged into a beam of one of the 
excitation sections. It is also adequate for only individual ones of the 
partial beams of the joint beam to be imaged into a beam of one of the 
excitation sections while the other partial beams of the joint beam do not 
experience such imaging. In any case, it is, however, necessary for all of 
the partial beams to be coherent among one another in the joint beam. 
In accordance with the invention, it is particularly advantageous for the 
partial beams to form a joint beam which is coherent in the 
cross-sectional direction. 
The optical element can be designed in a variety of different ways and, in 
particular, the design of the optical element will depend on the shape of 
the partial beam and of the beam. It is particularly advantageous for the 
optical element to image the respective partial beam into the beam such 
that the latter is narrowed in a cross-sectional direction with respect to 
the partial beam. This enables the laser amplification volume to also be 
made narrower in conformance with the dimensions of the beam in this 
direction. 
In the above description of the inventive solution, the dimensions of the 
laser-active unit were not specified. However, particularly advantageous 
designs of the inventive solid-state layer are obtainable by the 
laser-active unit having in the cross-sectional direction a width which 
corresponds at the most to a width of the partial beam imaged by the 
optical element onto the beam in this direction. In this way it is made 
possible for a partial beam to be imaged into an excitation section 
without disturbing the course of the partial beam lying alongside it. 
This is, for example, made possible by a partial beam being imaged into the 
beam of an excitation section and the partial beam lying alongside it 
being allowed to run on alongside the excitation section. An embodiment of 
the inventive solution has proven particularly advantageous wherein the 
optical elements of excitation sections lying alongside one another adjoin 
one another and image partial beams immediately adjacent one another 
essentially continuously into the beams lying alongside one another and in 
spaced relation to one another. 
In such embodiments wherein the beam is narrowed in the one cross-sectional 
direction with respect to the partial beam, provision is preferably made 
for the laser-active unit to comprise in this cross-section direction 
supply elements arranged alongside the laser amplification volume for the 
latter. 
One embodiment of the inventive solution is designed such that the joint 
beam is imaged by the optical elements continuously into the beams of the 
excitation sections. 
So far no details of the design of the optical elements have been given. 
The optical elements are preferably designed so as to comprise a 
cylindrical optical means, particularly when the optical elements image 
the partial beam into a beam which is narrowed in a cross-sectional 
direction. 
The optical elements can be designed as reflectors or as lenses. The 
optical elements are preferably cylindrical lenses. 
Furthermore, it is advantageous for each optical element to image parallel 
rays of the joint beam into quasi-parallel rays of the beam so that, in 
particular, a joint beam with a substantially parallel path of rays is 
imaged into a beams with a likewise substantially parallel path of rays. 
Since the inventive concept is based on the excitation sections being 
arranged in spaced relation to one another, this preferably also 
incorporates the laser amplification volumes being spaced in relation to 
one another. 
In a particularly advantageous geometrical configuration, provision is made 
for the laser amplification volumes to be arranged at regular spacings 
from one another. 
The solution is preferably designed such that the beams penetrating 
different laser amplification volumes extend parallel to one another. In 
this way, in particular, a very compact design of the inventive 
solid-state laser is achieved. 
Since one must work with as high pumping powers as possible in the laser 
amplification volume in high-power lasers, cooling of the laser 
amplification volume is expedient, and this cooling is made as effective 
as possible. For this reason, it is advantageous for each laser 
amplification volume to be cooled on at least one side extending parallel 
to the beam. Herein it is even better for each laser amplification volume 
to be cooled on opposite sides. 
In this case, the supply elements mentioned at the beginning preferably 
carry out the cooling of the laser amplification volume. 
In particular, with laser amplification volumes arranged alongside one 
another, provision is advantageously made for that side on which cooling 
of the laser amplification volume takes place to be the side facing the 
adjacent laser amplification volume. This is advantageous particularly 
when this side of the laser amplification volume has a larger surface than 
the side facing away from the adjacent laser amplification volume as a 
more effective and, in particular, also more uniform cooling is possible 
with this solution. 
Furthermore, in the description of the embodiments so far no details were 
given as to the side from which excitation of the laser amplification 
volume is to take place. It is particularly advantageous for each laser 
amplification volume to be excitable from at least one excitation side 
extending parallel to the beam. 
Even more optimum excitation is obtained when each laser amplification 
volume is excitable from two opposite excitation sides. 
The excitation side can be selected so as to be that side facing away from 
the adjacent laser amplification volume but, in particular, in a 
semiconductor laser it is advantageous for the excitation side to be the 
side facing the adjacent laser amplification volume. 
In all of the embodiments described hereinafter, provision is made for at 
least one laser-active region penetrated by the respective beam to be 
provided in each laser amplification volume. 
Furthermore, the object mentioned hereinabove is accomplished in accordance 
with the invention is a solid-state laser of the kind described at the 
beginning by the resonator being a coupled resonator, by the resonator 
having two elongated excitation sections--in particular lying in one 
plane--with one of the laser amplification volumes being arranged in their 
respective beam, by the resonator having a coupling section which the beam 
of the excitation sections enter as outer beams extending in spaced 
relation to one another --in particular parallel to one another--and which 
couples the excitation sections with one another by displacing the outer 
beams in the plane defined by these to a coupling axis lying--in 
particular parallel to the outer beams--between these beyond this coupling 
axis, and by the laser amplification volumes being cooled on side surface 
extending along the beam and being excitable by the pump means from a side 
surface extending along the beam. 
Hence the inventive solution enables at least two laser amplification 
volumes to be advantageously coupled with one another, with the 
dissipation heat being controlled better in these two layer amplification 
volumes and the excitation for high powers being possible in a simple way. 
This is, for example, achieved by the laser amplification volumes being 
cooled on at least one side and being irradiated by the high-power source 
on a side which is not cooled. On those sides which are cooled, this 
cooling can thus be made as effective as possible, which enables better 
removal of the dissipation heat than in the solutions heretofore. 
Furthermore, this also allows the laser amplification volume to be excited 
with higher pumping powers. Finally, use of at least two laser 
amplifications volumes makes it possible to use a compact design, in 
particular, a compact structural length, and yet to couple-in the pumping 
power over a large surface and remove the dissipation heat. 
No details were given in the description of the embodiments hereinabove as 
to the design of the coupling section. Particularly good coupling is 
achieved in the coupling section by the coupling section comprising the 
beam path of an unstable resonator. 
Furthermore, a particularly advantageous, compact geometrical arrangement 
with best possible imaging characteristics is achieved with the outer 
beams lying symmetrically in relation to the coupling axis. 
Regarding the design of the mirrors of the coupling section, it is 
particularly expedient for the coupling section to comprise one mirror 
which reflects towards the coupling axis and one mirror which reflects 
away from the coupling axis, with these complementing each other in such a 
way that the outer beams are displaced parallel in the direction towards 
the coupling axis and imaged towards the latter by the two mirrors. 
In the simplest case, provision is made for the mirror reflecting towards 
the coupling axis to protrude with its active region in the radial 
direction away from the coupling axis beyond the active region of the 
mirror reflecting away from the coupling axis and to be acted upon by the 
outer beams in this protruding region. 
In geometrically advantageous solutions, provision is made for the coupling 
section to comprise one convex and one concave resonator mirror. 
With a view to achieving geometrical relations which are as simple as 
possible, it is preferable for the resonator mirrors to be designed and 
arranged confocally in the coupling section. 
In the explanation of the embodiments hereinabove, no details were given 
about the mirrors with which the excitation sections are equipped. In a 
preferred embodiment, provision is made for the excitation sections to be 
closed off by end mirrors on each side facing away from the coupling 
section. 
These end mirrors preferably reflect the beams in the excitation sections 
into the coupling section and if a mirror which reflects towards the 
coupling axis is used in the coupling section, these beams strike this 
mirror, while the mirror reflecting away from the coupling axis extends 
between the beams coming from the excitation sections and preferably as 
far as these. 
In the description of the embodiments so far, no details were given as to 
how the laser radiation is to be coupled out of the resonator. One 
advantageous possibility is for one of the end mirrors to be 
semitransmissive. As an alternative to this, it is, however, also 
conceivable for both end mirrors to be semitransmissive. 
In principle, the end mirrors can be of flat mirror design. However, since 
the beams of the excitation sections extend over a considerable length and 
even diffraction effects cause a beam with a parallel beam path to later 
expand in the coupling section, provision is preferably made for the end 
mirrors to have a curvature which compensates expansion of the beam in the 
excitation section and reflects the radiation coming from the coupling 
section back into it. Hence expansion of the beams in the excitation 
sections can also be compensated with the end mirror and the resonator 
thereby made more efficient. 
In the event there are two excitation sections, the structurally simplest 
solution is to use separate end mirrors. If, however, the end mirrors are 
to be held in a stable manner, it is advantageous particularly if a 
plurality of excitation sections is used, for the end mirrors which close 
off the excitation sections to be united to a mirror ring. 
If, as described hereinabove, the end mirror should expediently also have a 
curvature in order to compensate expansion of the beams in the excitation 
sections, provision is preferably made for the mirror to be of toroidal 
shape. 
Particularly advantageous guidance of the beams in the coupling sections 
which is geometrically desirable as far as the imaging characteristics are 
concerned is achieved by the coupling axis being the axis of symmetry of 
the resonator mirrors of the coupling section. 
In the even that only two excitation sections are used, provision is 
expediently made, for reasons of simplicity, and, in particular, in view 
of the advantageous beam shape of the emerging laser beam, for the 
resonator mirrors of the coupling section to have cylindrical mirror 
surfaces, and, in particular, in this case, the resonator is a cylinder 
resonator with confocally arranged mirrors. 
Within the scope of the inventive solution, it is advantageous, in 
particular, to increase the power yet remove the dissipation heat 
expediently, to provide several outer beams which are arranged in 
different planes extending through the coupling axis and continuous in 
corresponding excitation sections. 
The planes are preferably arranged at constant angular spacings from one 
another so the outer beams are at constant spacings from one another 
running in the azimuthal direction around the coupling axis. 
In this case, the resonator mirrors of the coupling section are preferably 
of such shape that they have spherical mirror surfaces and extend 
symmetrically with respect to rotation around the coupling axis. 
In arrangement which is advantageous particularly from a geometrical point 
of view, the outer beams form annular segments relative to the coupling 
axis. 
Insofar as the outer beams which continue in the beams of the excitation 
sections are spaced from one another in the azimuthal direction around the 
coupling axis, it is particularly advantageous, in order to achieve 
optimum coupling of all outer beams with one another in the coupling 
section, for the coupling section to be closed off in the annular segments 
which receive no outer beams coming from the excitation sections by 
mirrors which reflect back. The mirrors which reflect back serve to close 
off the coupling section completely in the azimuthal direction so that 
formation of a beam path radially symmetrically in relation to the 
coupling axis in all directions is possible and all directions are thereby 
coupled with one another via the coupling axis. 
In the simplest case, provision is made for the mirrors which reflect back 
to be essentially flat mirrors and to thus reflect back the incident rays 
in the same way as the end mirrors of the excitation sections. 
The mirrors which reflect back are preferably positioned such that in the 
direction of propagation of the radiation on the coupling section side 
they are arranged before the solid-state rods to thereby enable the spaces 
between the solid-state rods to be used for cooling these. 
A solution wherein the mirrors which reflect back are arranged directly at 
the level of one of the mirrors of the coupling section, preferably the 
mirror that reflects away from the coupling axis, is particularly 
advantageous. 
In a particularly preferred embodiment, in particular to improve the 
coupling of the outer beams and to achieve an optimum, compact structural 
design, provision is made for the sum of all of the outer beams to form 
essentially a closed annulus in the coupling section so the mirrors which 
reflect back can be dispensed with. 
Particularly when more than two excitation sections are provided, it has 
proven expedient for the excitation sections to be arranged axially 
symmetrically around an axis. 
Furthermore, in order to simplify the structural design, in particular, a 
compact structural design, the excitation sections are aligned so as to 
extend parallel to one another. 
To establish correct imaging relations between the coupling section and the 
excitation sections, there is preferably provided between the coupling 
section and the excitation sections an optical element for imaging the 
outer beams onto the beams in the excitation sections. 
The optical element expediently comprises a cylindrical optical mean which, 
in particular, is of such design that a cylindrical axis of the 
cylindrical optical means extends in the radial direction. 
Such a cylindrical optical means enables optimum exploitation of the 
coupling section in the azimuthal direction and, on the other hand, 
azimuthal spacings which are as large as possible between the laser 
amplification volumes, namely when the cylindrical optical means comprises 
a cylindrical, optical, annular segment which respectively images the 
outer beam forming an annular segment in the coupling section onto a beam 
which is narrower in the azimuthal direction in relation to the coupling 
axis in the excitation section. 
The width of the beam in the azimuthal direction in the excitation section 
preferably corresponds at the most to the width of the laser amplification 
volume in this direction. 
A particularly preferred solution within the meaning of the invention is 
obtained when the cylindrical, optical, annular segments unite to form an 
annulus and when this annulus comprised of cylindrical, optical, annular 
segments is capable of imaging an annulus closed by the outer beams in the 
coupling section onto a plurality of beams spaced from one another in the 
azimuthal direction in the excitation section so that, on the one hand, 
there is a cylindrical-symmetrical beam path in relation to the coupling 
axis in the coupling section and, on the other hand, the spacings of the 
beams in the azimuthal direction in the excitation sections enable the 
laser amplification volumes to be cooled in the region of these spaces. 
In the description of an embodiment of the inventive solution hereinabove, 
no details were given as to how the laser amplification volumes are to be 
arranged and designed. 
In a preferred embodiment, provision is made for he laser amplification 
volumes to be aligned parallel to one another. 
In particular, for geometrical-optical reasons, provision is expediently 
made for the laser amplification volumes to be identical in shape. In 
principle, the geometry of the laser amplification volumes can be selected 
optionally. A round or oval cross-section is, for example, conceivable. It 
is, however, particular advantageous for the laser amplification volumes 
to be designed as elongate laminae. 
To achieve amplification which is as uniform as possible, it is, 
furthermore, advantageous for the laser amplification volumes to be made 
of identical material. 
A geometry of the laser amplification volumes has, however, proven 
particularly advantageous wherein the laser amplification volumes have two 
broad sides facing each other, with the spacing of the broad sides 
preferably being selected such that optimum heat removal of the 
dissipation heat from the laser amplification volumes can take place in 
the direction of the broad sides. 
It is furthermore, advantageous for the laser amplification volumes to have 
two narrow sides facing each other, with the spacing of the narrow sides 
being selected such that it is essentially of the order of magnitude of a 
penetration depth of the pumping power so coupling-in of the pumping power 
preferably takes place via the narrow sides. 
The type of the laser amplification volume was not specified in any of the 
inventive solutions described hereinabove. In an advantageous embodiment 
the layer amplification volume is formed by a solid-state rod. 
This solid-state rod is preferably optically excitable and, in particular, 
the pumping means irradiates the solid-state rod from one side. 
An embodiment wherein the pumping power impinges upon a narrow side is 
particularly simple. 
In this case, it is then likewise advantageous for at least one broad side 
to be cooled. 
The broad sides are preferably flat surfaces. It is similarly expedient for 
the narrow sides, in particular the narrow side on which the pumping power 
impinges, to also be designed as flat surfaces. 
In the simples case, it is advantageous for the solid-state rods to have an 
essentially four-cornered cross-section, with the two broad sides 
extending essentially perpendicular to the two narrow sides. 
Particularly advantageous cooling of the solid-state rod is possible when 
the solid-state rod is cooled on both broad sides. Optimum cooling of the 
solid-state rod is possible when the solid-state rod is additionally 
cooled on a narrow side and coupling-in of the pumping power, therefore, 
takes place on one narrow side only. 
The description of the embodiments hereinabove contains no details of the 
type of cooling. It has proven particularly advantageous for the 
solid-state rods to be cooled by contact with a flow-free material, i.e., 
for cooling to take place by direct thermal contact with an elastic or 
plastic substance or a rigid body, it also being possible, in the even a 
rigid body is used as cooling element, for an elastic or plastic substance 
to serve as heat-transmitting medium between the cooling element and the 
solid-state rod. 
In general, if such contact cooling is used, it is advantageous for the 
solid-state rods to be cooled on their sides facing one another so the 
solid-state rods can, for example, be acted upon the pumping power on 
their sides facing away from one another. 
In particular if the excitation sections are arranged axially symmetrically 
in relation to an axis, provision is expendiently made from the 
solid-state rods to be cooled on a side extending approximately in the 
direction towards a radius direction of the axis. 
In accordance with the invention, the most advantageous cooling is enabled 
by the solid-state rods being cooled by contact with a cooling element, 
with the cooling element preferably resting on two sides of the 
solid-state rod facing each other. 
In this case, to avoid a heat-transmitting medium in the form of an elastic 
or plastic material, provision is preferably made for the cooling element 
to rest with a press fit on the solid-state rod, with the press fit 
preferably being established by the contact with the two sides of the 
solid-state rod facing each other. 
In principle, it is possible to allocate to each solid-state rod a cooling 
element of its own. It is, however, particularly advantageous for the 
cooling element to lie between the solid-state rods of the excitation 
sections which belong to one another. 
Furthermore, the cooling element also makes it possible for it to be 
designed so as to carry the solid-state rods so that fixing of the 
solid-state rods by additional holding means is not necessary but at the 
same time cooling of the solid-state rod also takes place via these 
holding means. 
In a particularly preferred solution, provision is made for the solid-state 
rod to sit with both broad sides and one narrow side in a groove of the 
cooling element. 
Details have also not been given about the material from which the cooling 
element should be made. It is advantageous for the cooling element to be 
made of a material with good heat conductivity, and it is preferable for 
the cooling element to be a metal element. 
To keep the cooling element at a constant temperature, it is expedient for 
a cooling medium to flow through the cooling element. 
In the description of the embodiments hereinabove, it was not explained in 
detail how the solid-state rods are acted upon by the pumping power. In a 
particularly preferred solution, provision is made for the solid-state 
rods to be acted upon with pumping power on their sides facing away from 
one another. Such a solution provides the optimum geometrical 
possibilities for introducing as much pumping power as possible into the 
solid-state rods. In all of the embodiments in which the excitation 
sections are arranged axially symmetrically around an axis, this is 
achieved by the solid-state rods being irradiated by the pumping power 
source on a side surface extending essentially transversely to a radius 
direction of the axis. This makes it possible for the solid-state rods to 
be acted upon with pumping power in the radial direction in relation to 
the axis away from this axis or in the radial direction in relation to the 
axis towards this axis. It has proven particularly advantageous for the 
solid-state rods to be acted upon with the pumping power in the radial 
direction of the axis toward the latter. 
Moreover, in all the embodiments in which the solid-state rods are cooled 
by the cooling element, the solid-state rods can be advantageously acted 
upon with the pumping power by each solid-state rod being acted upon by 
the pumping power on its side surface which is not encompassed by the 
cooling element. 
In combination with the arrangement of the cooling element, the most 
advantageous geometrical arrangement of cooling element and pumping power 
source is for the cooling element to be surrounded by the pumping power 
source. In this case, the pumping power source is expendiently designed so 
as to radiate in an essentially radial direction onto the cooling element. 
To enable the pumping power to be coupled into the solid-state rods as 
effectively as possible, it is expedient for elements which concentrate on 
the solid-state rods to be provided for the pumping power. 
These concentrating elements are preferably designed to deflect onto the 
solid-state rods electromagnetic radiation emitted by the pumping power 
source into a solid angle. 
One possibility of providing such concentrating elements is to provide an 
optical refraction means, for example, in the form of a cylindrical lens 
between the pumping power sources and the solid-state rods. 
It is, however, even more advantageous for the concentrating elements to be 
reflectors which can be arranged on a side of the pumping power source 
facing the respective solid-state rod or between the pumping power source 
and the respective solid-state rod. 
In a particular good combination of the concentrating elements with the 
cooling element, provision is made for the intermediate webs of the 
cooling elements to pass on the pumping power impinging thereon to the 
solid-state rods, it being possible for this passing-on to be implemented 
in a variety of different ways. 
Here, it has, however, proven particularly advantageous for the 
intermediate webs to comprise surfaces which reflect the pumping power to 
the solid-state rods. 
In the simplest case, the intermediate webs are designed so as to rise in 
tapering configuration above the solid-state rods, the simplest solution 
from a manufacturing viewpoint being that of the intermediate webs 
tapering in wedge-shaped configuration. 
Within the scope of the present invention, a very wide variety of solutions 
is likewise conceivable for the type of design of the pumping power 
source. 
In a particularly preferred embodiment, provision is made for the pumping 
power source to surround the solid-state rods in annular configuration. 
In this case, the pumping power source is preferably a gas-discharge lamp. 
Such a gas-discharge lamp can be operated in many different ways. In a 
preferred embodiment, provision is made for a gas discharge to be 
generated in the gas-discharge lamp by a field extending essentially 
radially in relation to its axis. 
It is however, also conceivable for a gas discharge to be generated in the 
gas-discharge lamp by a field extending azimuthally in relation to its 
axis, the gas-discharge lamp being divided by electrodes into annular 
segments for this purpose. 
It is particularly advantageous for the gas discharge to be generated by 
high frequency in the gas-discharge lamp, with the high frequency then 
being applied by electrodes spaced in the radial or azimuthal direction. 
As an alternative to this, it is, however, also conceivable, instead of 
using electrodes, for the high frequency to be coupled into the 
gas-discharge lamp in the form of microwaves. 
A further alternative to the coupling of the high frequency into the 
gas-discharge lamp is inductive coupling of the high frequency into the 
gas-discharge lamp. 
As an alternative to provision of a single pumping power source, it is, 
however, likewise conceivable to arrange a plurality of single pumping 
power sources around the cooling element, the single pumping power sources 
being arranged, in particular, alongside one another. In the simplest 
case, the single pumping power sources are likewise gas-discharge lamps 
with the gas discharge preferably being generated by high frequency with 
one of the types of coupling-in mentioned hereinabove. 
As an alternative to this it is, however, also conceivable for the single 
pumping power sources to be designed as rows of laser diodes which have 
the advantage of an emission characteristic concentrated on a small solid 
angle. 
As an alternative to the variant of the solid-state laser described 
hereinabove with an optically pumped solid-state rod, provision is 
likewise preferably made in the inventive solution for the laser 
amplification volume to be that of a semiconductor layer and, in this 
case, the laser-active unit is formed by a semiconductor laser means of 
commonly known design. In such a semiconductor laser, provision is made 
for several laser-active regions to be provided in each layer 
amplification volume. Herein the laser-active regions are the 
laser-amplifying semiconductor layer regions of a semiconductor laser. 
In the inventive use of a semiconductor laser as laser-active units, 
provision is preferably made for the laser-active regions to be seated 
between semiconductor layers of the pumping means forming a pn-junction. 
These laser-active regions are preferably of strip-shaped design and, in 
particular, arranged in spaced relation to one another to make is possible 
for these laser-active regions to be supplied with sufficient cooling 
power. 
In an expedient arrangement, provision is made for the laser-active regions 
to extend parallel to one another. 
In this case, laser-inactive regions are preferably arranged in spaces 
between the layer-active regions so that laser-active and laser-inactive 
regions alternate with one another in a layer. 
In one variant which allows the beam to run in a disturbance-free manner in 
such a laser excitation volume, provision is preferably made for the 
laser-inactive regions to be of transparent design for the beam, in 
particular, to be made of transparent material. 
Herein the laser-inactive regions are preferably in the form of 
semiconductor layer regions but with an increased ban gap with respect to 
the laser-active regions so that there is no absorption of the laser 
radiation in the laser-inactive regions. 
Since in such an embodiment of the inventive solution the beam penetrates 
partly laser-active and partly laser-inactive regions, problems arise when 
the laser-inactive regions and the laser-active regions do not have the 
same index of refraction. In this case, the arrangement of the 
laser-active and laser-inactive regions represents a phase grid for the 
beam. Hence in the event the laser-active and laser-inactive regions do 
not have the same index of refraction, it is advantageous for the optical 
length of the laser-active and laser-inactive regions to be of such 
dimensions that the parts of the beam penetrating these have the same 
phase position so that the maximum intensity lies in the zeroth order of 
the phase grid. 
As an alternative to the solution in which the laser-inactive regions are 
made of transparent material, provision is made in a further inventive 
solution for the laser-inactive regions to be material-free channels so 
that no problems can arise with the absorption in these laser-inactive 
regions. 
However, in this case the indexes of refraction differ between the 
laser-active and laser-inactive regions so that the optical length of the 
laser-active and laser-inactive regions is advantageously of such 
dimensions that the parts of the beam penetrating these differ in phase by 
an integral multiple of 2.pi.. 
In a particularly preferred embodiment of the inventive solution, it is 
additionally advantageous for the same partial beam, imaged as beams, to 
penetrate two laser amplification volumes of two laser-active units which 
are arranged one after the other in the direction of propagation of the 
beams so that a further power increase is thereby possible. 
Herein the laser-active units are advantageously arranged either 
immediately one behind the other or in the form of two excitation sections 
which are arranged one behind the other and between which imaging into a 
partial beam again takes place. 
In the cases where the laser-active units are arranged immediately one 
behind the other, it is possible for the laser-active and laser-inactive 
regions to be in alignment with one another. It is, however, also possible 
for the laser-active regions to be arranged in offset relation to one 
another so that, for example, a laser-inactive region of a laser-active 
unit is in alignment with the laser-active region of the other 
laser-active unit or the laser-active regions are offset in relation to 
one another in the transverse direction. 
In particular, such arrangements are also advantageous with excitation 
sections which are arranged in succession. Herein a further advantageous 
variant is made possible by the laser-active units being turned with 
respect to one another, preferably through an angle of 90.degree., about 
an axis parallel to the direction of propagation. 
Furthermore, an advantageous embodiment makes provision for several 
laser-active units to be arranged alongside one another in sandwich-like 
configuration. It is particularly advantageous for several laser-active 
units to form a laser-active block. 
The pumping means is preferably connected to a cooling element so that the 
laser-active regions are preferably pumped and cooled from sides facing 
one another. 
The cooling element is expediently designed so as to comprise at least one 
heat-conducting layer. 
The pumping means and the cooling element are preferably integrated into 
the laser-active unit and arranged as such in an excitation section.

A first embodiment of an inventive solid-state laser, illustrated in FIG. 
1, comprises a resonator designated in its entirety 12 and comprising a 
first excitation section 14 and a second excitation section 16 which are 
both arranged parallel to one another and symmetrically in relation to an 
axis 18 and each comprise a path of rays with a parallel beam 20 and 22, 
respectively, and so the beams 20 and 22 also extend parallel to one 
another and symmetrically in relation to the axis 18. 
These beams 20 and 22, respectively, enter as outer beams 24 and 26, 
respectively, a coupling section designated in its entirety 28 of the 
resonator 12 symmetrically in relation to a coupling axis 30 and are 
reflected in the coupling section by reflection in the direction of the 
coupling axis 30, preferably imaged towards the coupling axis 30, so the 
coupling between the two outer beams 24 and 26 beyond the coupling axis 30 
results in the joint beam 31. 
The two outer beams 24 and 26 thereby form a coupling plane extending 
through the coupling axis 30 and are reflected by the coupling section 28 
of the resonator 12 in this coupling plane towards the coupling axis 30 in 
order to couple with one another beyond the coupling axis 30 to form the 
joint beam 31. 
Owing to this design of the resonator 12, the first excitation section 14 
and the second excitation section 16 are completely coupled with one 
another and so coherent laser radiation forms in these two excitation 
sections 14 and 16 beyond the coupling section 28. 
The first excitation section is preferably closed off on a side opposite 
the coupling section 28 by an end mirror 32 and the second excitation 
section 16 by an end mirror 34, these preferably being flat mirrors both 
lying in a plane 36 perpendicular to the axis 18. 
The coupling section 28, in turn, is preferably formed on its side opposite 
the excitation sections 14 and 16 by a concave mirror 38 and on its side 
facing the excitation sections 14 and 16 by a convex mirror 40. The convex 
mirror 40 extends between the two outer beams 24 and 26 which propagate as 
straight-line continuation of the beams 20 and 22 into the coupling 
section 28 past the sides of the convex mirror 40 and impinge upon the 
concave mirror 38 which reflects onto the convex mirror 40 which then 
reflects back again to the concave mirror 38, more particularly, parallel 
to the outer beams 24 and 26. This results in reflection back and forth of 
the beams 24 and 26 until these reach the coupling axis 30 and pass over 
the 34 latter into the respective other beam 26 and 24, respectively. 
The concave mirror 38 and the convex mirror 40 are preferably designed as 
the two mirrors of a cylinder resonator, in particular, a confocal 
cylinder resonator, the resonator axis of which is the coupling axis 30. 
It is preferably for both the concave mirror 38 and the convex mirror 40 to 
have cylindrical mirror surfaces 42 and 44 which are curved in the 
direction of the coupling plane, but are preferably not curved 
perpendicular to the coupling plane. 
In the case of a cylinder resonator formed by mirrors 38 and 40, the 
resonator axis is that axis which stands perpendicular on both mirror 
surfaces 42 and 44. 
The excitation sections 14 and 16 each contain a solid-state rod 46 and 48, 
respectively, which with a longitudinal axis parallel to a first direction 
50 and 52, respectively, each extend parallel to the axis 18, with each 
solid-state rod 46 and 48, respectively, being completely permeated by the 
respective beam 20 and 22, respectively. 
For coupling the laser radiation out of the resonator 12, the end mirror 
32, for example, is designed as semi-transmissive mirror which thus 
reflects the beam 20 only partly and from which there emerges a 
coupled-out beam 54 which is expanded to a beam with a square 
cross-section by a cylindrical optical means 56. 
It is, however, also conceivable for both the end mirror 32 and the end 
mirror 34 to be of semitransmissive design and for two coupled-out beams 
to be allowed to emerge from the resonator 12. As illustrated in FIG. 2, 
the solid-state rods 46 and 48 are designed as rods with a rectangular 
cross-section, each solid-state rod having two broad sides 60 and 62 
facing each other and two narrow sides 64 and 66 facing each other which, 
in accordance with the invention, are formed by flat surfaces, with the 
broad sides 60 and 62 extending perpendicular to the narrow sides 64 and 
66. 
Each solid-state rod 46 and 48 is, for its part, held in a cooling element 
designated in its entirety 68 which engages over each solid-state rod 46 
and 48, respectively, on both broad sides 60 and 62 and preferably also on 
the narrow side 66 facing the axis 18 and rests in a thermally contacting 
manner on the two broad sides 60 and 62 and preferably also on the narrow 
side 66. 
With the narrow side 64 facing away from the axis 18, each of the 
solid-state rods 46 and 48 faces a light source 70 and 72, respectively, 
acting as pumping power source, In the simplest case, the light sources 70 
and 72 are gas-discharge lamps. Each of the solid-state rods 46, 48 forms 
with the respective light source 70 and 72, respectively, a laser-active 
unit 73. 
These light sources 70 and 72 are preferably designed so as to emit their 
light in the form of pumping radiation 74 and 76, respectively, 
essentially in the direction of the narrow side 64 so the pumping 
radiation can penetrate the respective solid-state rod 46 and 48, 
respectively, via the respective narrow side 64, the spacing of the narrow 
side 64 from the narrow side 66 preferably being selected in the order of 
magnitude of the penetration depth of the pumping radiation 74 and 76, 
respectively, in order that the pumping radiation 74 and 76, respectively, 
will penetrate the solid-state rod 76 and 48, respectively, over its 
entire expanse in the direction of the broad sides 60 and 62 and hence 
excite these to an essentially full extent. 
In order to also use diverging pumping radiation 74 and 76, respectively, 
coming from the light sources 70 and 72 as fully as possible for 
excitation of the respective solid-state rod 46 and 48, respectively, the 
cooling element 68 is additionally provided with reflector surfaces 78 and 
80, respectively, which, in accordance with the invention, extend from 
each solid-state rod, starting at the level of the respective narrow side 
64 on the respective broad sides 60 and 62, respectively, away from the 
axis 18 with increasing spacing from one another and preferably at an 
acute angle and symmetrically in relation to a center plane 82 which, for 
its part, extends through the axis 18 and through the light source 70 as 
well as through the center of the respective solid-state rod 46 and 48, 
respectively. By means of these expanding reflector surfaces 78 and 80, 
respectively, pumping radiation 74 propagating at an acute angle to the 
center plane 82 is also reflected towards the respective solid-state rod 
46 and 48, respectively, and hence used to excite the latter. 
The spacing of the broad sides 60 and 62 is chosen in accordance with the 
heat conductivity of the solid-state rods 46 and 48, respectively, more 
particularly, such that the heat to be removed from these solid-state rods 
46 and 48, respectively, can be conducted away quickly enough for it not 
to cause excessive heating-up of the solid-state rods 46 and 48, 
respectively, and hence the known problems caused by the thermal expansion 
of the solid state rods 46 and 48 no longer occur. 
To achieve optimum heat transfer from the broad sides 60 and 62 to the 
cooing element 68, the solid state rods 46 and 48, respectively, are 
preferably clamped into the cooling element between two side webs 84 and 
86, respectively, which thus rests with pressure on the broad sides 60 and 
62. The heat conductivity between the solid-state rods 46 and 48 can be 
additionally improved by a heat conducting agent, for example, a heat 
conducting paste being applied between the side webs 84 and 86 and the 
broad sides 60 and 62. 
Optimum thermal contact can be established between the narrow side 66 and 
the cooling element 68 in the same way. For this purpose, a groove 
designated in its entirety 88 is preferably provided between the side webs 
84 and 86, with the narrow side 66 resting on the groove bottom 90 
thereof. 
To improve the illumination of the solid-state rods 46 and 48, 
respectively, a contact surface 92 and 94 of the side webs 84 and 86 is 
preferably a reflecting design and hence serves as continuation of the 
respectively reflector surface 78 and 80, respectively, so that all of the 
pumping radiation 74 and 76, respectively, reflected by the reflector 
surfaces 78 and 80, respectively, into the groove 88 is also reflected 
back and forth by these contact surfaces 92 and 94, respectively, and 
hence optimum illumination of the solid-state rods 46 and 48, 
respectively, takes place over their entire cross-section. 
For optimum removal of the heat into the cooling element, the latter 
preferably contains cooling channels 96 preferably extending in the 
longitudinal direction of the cooling element 68, i.e., parallel to the 
axis 18, and near the contact surfaces 92 and 94 as well as the groove 
bottom 90. 
A good heat conducting material, i.e., for example, copper is used as 
preferred material for the cooling element 68. 
Ruby or neodymium and, for example, also titanium sapphire are preferably 
used for the solid-state rods 46 and 48, respectively, of this inventive 
solid-state laser. 
A second embodiment of an inventive solid-state layer, illustrated in FIGS. 
3 to 5, is, in principle, of exactly the same design as the first 
embodiment. In particular, a resonator 112 thereof is likewise provided 
with a first excitation section 14 and a second excitation section 16 both 
lying with their beams 20 and 22 in a plane which in the coupling section 
28 is a coupling plane over which the outer beam 24 couples with the outer 
beam 26. In contrast with the first embodiment, however, not only two 
excitation sections 14 and 16 are provided, but instead a plurality of 
planes 114, 116, 118 and 120 which all extend through the axis 18 and 
through the coupling axis 30 coaxial with the latter and form a family of 
planes in relation to the axis 18. 
Arranged in each of these planes 114, 116, 118 and 120 are a first 
excitation section 14 and a second excitation section 16 with their beams 
20 and 22. 
The coupling section 28 likewise comprises the concave mirror 38 and the 
convex mirror 40, with the concave mirror 38 having a spherical concave 
mirror surface 122 and the convex mirror 40 and a convex spherical mirror 
surface 124, and the mirror surfaces 122 and 124 likewise lying confocally 
in relation to each other. Hence the coupling section 28 forms a spherical 
unstable resonator which couples the outer beams 24 and 26 of the 
respective planes 114, 116, 118 and 120 with one another, but also in the 
region of the coupling axis 30 the beams of the individual planes 114, 116 
and 120 with one another so that, in all, a joint beams 121 with coherent 
radiation is formed in the resonator 112 with a plurality of first and 
second excitation sections 14, 16 and with a coupling section 28. 
The end mirrors 32 and 34 of the first and second excitation sections 14 
and 16 are preferably all of semitransmissive design so that a plurality 
of coupled-out beams 126, all arranged axially symmetrically in relation 
to the axis 18 around the latter, emerges from the resonator 112. 
To improve the coupling of the radiation propagating in the respective 
planes in the resonator 112 between the planes 114, 116, 118 and 120, 
there is arranged between the coupling section 28 and the excitation 
sections 14 and 16 a mirror element 128 which, as illustrated in FIG. 5, 
by means of non-reflective sectors 130, 132, 134 and 136 allows the beams 
24 and 26 in the respective planes 114, 116, 118 and 120 to pass, but 
between these sectors 130, 132, 134 and 136 comprises mirrored sectors 
138, 140, 142, and 144 which close off the coupling section 28 in the 
sector regions between the beams 24 and 26 in order to also permit 
radiation propagation in these regions in the coupling section 28 and 
hence optimally couple all outer beams 24 and 26 with one another. The 
mirrored sectors 138, 140, 142 and 144 are preferably likewise flat 
mirrors which reflect back in the same way as the end mirrors 32 and 34 
which are likewise preferably designed as flat mirrors, in order to also 
ensure between the outer beams 24 and 26 in the coupling section 28 a 
parallel path of rays which can thus circulate in the azimuthal direction 
and pass over into the parallel path of rays of the outer beams 24 and 26. 
In the second embodiment, the planes 114, 116, 118 and 120 are preferably 
arranged at constant angular spacings relative to one another so that the 
axis 18 and the coupling axis 30 form multiple axes of symmetry for the 
path of rays in the resonator 112. 
As illustrated in FIG. 4, the cooling element 146 is arranged as cylinder 
coaxially with the axis 18 and comprises grooves 88, with the planes 114, 
116, 118 and 120 forming center planes corresponding to the center plane 
82 for the arrangement of the solid-state rods 46 and 48 and the 
arrangement of the light sources 70 and 72. Furthermore, reflector 
surfaces 78 and 80 are provided in the same way as i the first embodiment, 
and the reflector surfaces 88 and 78 form successive points 148. In this 
embodiment, the solid-state rods 46 and 48 are preferably of trapezoidal 
design, with the broad sides 60 and 62 lying in radial planes extending 
through the axis 18, while the narrow sides 64 and 66 extend parallel to 
one another. 
For a description of parts of the second embodiment which have the same 
reference numerals as those of the first embodiment and hence are 
identical with these with respect to function, reference is to be had to 
the description and explanation of the function of the first embodiment. 
In a third embodiment, illustrated in FIGS. 6 to 9, those parts identical 
with those of the first and second embodiments have the same reference 
numerals and so insofar reference is to be had to the description of the 
first and second embodiments. 
In contrast with the second embodiment, as illustrated in FIGS. 7 and 9, a 
large number of planes 150 corresponding to the planes 114 to 120 is 
provided. These all form a family of planes extending through the axis 18 
and the coupling axis 30 and are at identical angular spacing from one 
another, and a first and a second excitation section 14 and 16 with 
solid-state rods 46 and 48, respectively, and beams 20 and 22, 
respectively, lie in each plane 150. 
The resonator 152 comprises in the same way as the resonator 112 a 
plurality of beams 20 and 22 which are coupled with one another by the 
joint beam 121 in the coupling section 28 provided with spherical mirror 
surfaces 122 and 124 via a coupling axis 30 and so in this connection 
reference is to be had in full to the explanations of the first and second 
embodiments. 
In contrast with the second embodiment, however, the mirror element 128 is 
replaced by an imaging element 154 illustrated in FIGS. 6, 7 and 8 which, 
as illustrated in FIGS. 7 and 8, comprises a plurality of cylindrical 
optical segments 156 seated alongside one another and designed in the form 
of adjoining annular segments in relation to the axis 18. 
Each of these cylindrical optical segments 156 is designed symmetrically in 
relation to the respective plane 150 and has a convex cylindrical surface 
158 facing the coupling section 28 and a concave cylindrical surface 160 
facing the respective excitation section 14 and 16, respectively, the two 
cylindrical surfaces 158 and 160 having such a curvature that a parallel, 
outer beam 24 and 26, respectively, forming a partial beam of the joint 
beam 121 and having the shape of an annular segment is narrowed in the 
azimuthal direction 162 and hence forms the corresponding beam 20 and 22, 
respectively, which thus extends in the azimuthal direction 162 to a 
likewise parallel beam over a smaller angular area, and, conversely, a 
beam 20 extending over a smaller angular area in the azimuthal direction 
162 is expanded by the cylindrical surfaces 160 and 158 to an outer beam 
24 extending over a larger angular area in the azimuthal direction 162. 
Since all of the cylindrical optical segments 156 are preferably designed 
such that the convex cylindrical surfaces 158 adjoin one another, the path 
of rays in the resonator 152 can be selected such that all outer beams 24 
and 26, respectively, of successive planes 150 touch one another and hence 
the coupling section 28 comprises beams 24 and 26, respectively, which 
follow one another directly and adjoin one another as they circulate in 
the azimuthal direction 162. On the other hand, a shorter extent of the 
beams 20 and 22, respectively, in the azimuthal direction 162 is achieved 
with the cylindrical optical segments 156 and so spaces 164 remain between 
the successive beams 20 and 22, respectively. As a result of this, there 
also remain between the solid-state rods 46 and 48 located in the 
respective planes 150 spaces in which the side webs 84 and 86 of the 
cooling element 166 enclosing the solid-state rods 46 and 48 between them 
are arranged, the cooling element 166 being of similar design to the 
cooling element 146, but having grooves 88 which lie closer together so as 
to permit a larger number of planes 150. 
In a modification of the first and second embodiments, as illustrated in 
FIG. 6, the end mirrors 32 and 34 of the excitation sections 14 and 16 
are, furthermore, united to form an annular end mirror 168 comprising 
mirror surfaces 172 curved in the radial direction 170 in relation to the 
axis 18, the curvature of the mirror surfaces 172 being toroidal. The 
curvature of the mirror surfaces 172 is selected such that it compensates 
a slight expansion of the beams 20 and 22 in the radial direction 170 
caused by diffraction effects in the coupling section 28 by reflecting 
each incident ray of the beams 20 and 22, respectively, back into itself 
and hence keeping the outer beams 24 and 26 parallel in the coupling 
section 28. 
In contrast with the first and second embodiments, there is preferably 
provided in the third embodiment, as illustrated in FIG. 9, a single, for 
example, cylindrical light source 174 which, in particular, can be a 
cylindrical discharge lamp arranged coaxially with the axis 18. This is 
preferably also cooled by a cylindrical cooling jacket 176 which is 
arranged on the side of the light source 174 facing the cooling element 
166 and, in the simplest case, comprises a coolant 182 conducted between 
an outer cylinder wall 178 and an inner cylinder wall 180, the coolant 182 
being constantly exchanged and externally cooled. 
In the simplest case, the light source 174 is a gas discharge lamp with the 
gas discharge which takes place being initiated by an electric field 
strength extending in the radial direction 170. 
For the purpose, the light source 174 is provided with an outer electrode 
184 and, on the other had, the cooling element 166 can represent the inner 
electrode. 
The light source 174 forms with each of the solid-state rods a laser-active 
unit 73. 
In contrast with the gas discharge by means of a radial, electric field, it 
is, however, also conceivable for the light source 174, as illustrated in 
FIG. 10, to be divided up into flat electrodes 186 and 188 which are 
arranged in the radial direction 170 and between which an electric field 
strength oriented in the azimuthal direction 162 can be generated in order 
to initiate therein a gas discharge in a gas-discharge space 190 of the 
light source 174', this gas discharge preferably being a high-frequency 
gas discharge. 
As an alternative to this, it is also possible for the electrodes 186 and 
188 to be omitted and for a gas discharge to then be initiated to couple 
microwaves to the gas-discharge space 190. 
In a further variant of the inventive solution, illustrated in FIG. 11, the 
reflection surfaces 78 and 80 are drawn from the cooling element 166 up to 
a row of semiconductor diodes 192, with the row of semiconductor diodes 
192 extending parallel to the axis 18, preferably essentially over the 
length of the solid-state rods 46 and 48, respectively, in this direction. 
The reflection surfaces 78 and 80 serve to radially conduct the light 
emitted from the respective row of semiconductors 192 in the direction 
towards the respectively associated solid-state rod 46 and 48, 
respectively, so that essentially the total light emitted from the 
semiconductor diode 192 is guided to the respective solid-state rod 46 and 
48, respectively, and serves to excite the latter. 
Semiconductor diode rows 192 are preferably arranged in the azimuthal 
direction 162 around the entire cooling element 166, with their light 
being guided from the respective reflection surfaces 78 and 80, 
respectively, to the respective solid-state rod 46 and 48, respectively. 
The resonator concepts described on the basis of resonators 12, 122 and 152 
could also be modified within the scope of the present invention, for 
example, the scope of the present invention also allows use of resonator 
concepts as described in the article "Unstable resonators for annular gain 
volume lasers" in APPLIED OPTICS, Volume 17, No. 6, Mar. 15, 1978, to 
which references is expressly made in this connection. 
In a fourth embodiment of an inventive solid-state rod, illustrated in 
FIGS. 12 and 13, the resonator 212 is identical in design to the resonator 
112 of the first embodiment and, in addition, the excitation sections 14 
and 16 as well as the beams 20 and 22 are arranged in the same way, with 
two excitation sections 14 and 16 likewise lying in each of the planes 
114, 116, 118 and 120. 
Moreover, the coupling section 28 is also of identical design and comprises 
the beams 24 and 26 as well as the coupling axis 30. Therefore, in this 
connection reference is to be had in full to the statements on the second 
embodiment. 
Furthermore, the concave mirror 38 is also provided in the same way as in 
the second embodiment with a spherical concave mirror surface 122 and the 
convex mirror 40 with a convex spherical mirror surface 124. As likewise 
described in detail in connection with the second embodiment, these 
cooperate with one another to couple the beams 24 and 26 of the respective 
planes 114, 116, 118 and 120 with one another to form the joint beam 121. 
In addition, the end mirrors 32 and 34 are also designed in the same way as 
in the second embodiment so that a plurality of coupled-out beams 126 
likewise form in axially symmetrical relation to the axis 18 and emerge 
from the resonator 212. 
Finally, the mirror element 128 also acting in the same way as in the 
second embodiment is provided for coupling the radiation which builds up 
the resonator 212 and so reference is also to be had in this connection go 
the statements on the second embodiment. 
The fourth embodiment differs from the second embodiment in that instead of 
the solid-state rods 46 and 48, laser-active units 214 in the form of 
semiconductor lasers are now seated in the grooves 88 of the cooling 
element 146. 
As illustrated in FIGS. 13 and 14, each of the laser-active units 214 
comprises a laser amplification volume 216 with a pumping means designated 
in its entirety 218 adjoining it on either side thereof. This pumping 
means 218 comprises in sandwich-like configuration semiconductor layers 
220 and 222 of a pn-junction which enclose the laser amplification volume 
216 between them and on which there is positioned as contact and cooling 
area a metal layer 224 and 226, respectively, facing the laser 
amplification volume 216. The power supply leads to the metal layers 224 
and 226. 
The laser-active unit 214 is preferably a semiconductor laser in the form 
of a gallium arsenide laser so that the semiconductor layer 222 is, for 
example, the p-gallium arsenide layer, the semiconductor layer 220 the 
n-gallium arsenide layer and the metal layer 226 is supplied with the 
positive supply voltage and the metal layer 224 with the negative supply 
voltage. 
In the simplest case, the laser amplification volume 216 could be a 
continuous laser-active layer lying between the semiconductor layers 220 
and 222 with its band gap being lowered with respect to the adjacent 
layers by additional aluminum doping and hence having the lowest band gap. 
However, in such a case there are problems with the heat dissipation and 
so the layer amplification volume 216 preferably comprises strip-shaped 
laser-active regions 228 extending in a first direction 230 parallel to 
the longitudinal direction 21 and 23 of the beams 20 and 22, respectively. 
Arranged between the laser-active regions 228 are laser-inactive regions 
232 which in one variant likewise represent a semiconductor layer whose 
band gap is preferably selected such that this semiconductor layer does 
not absorb the laser radiation propagating in the respective beam 20 and 
22, respectively, i.e., that the band gap of the semiconductor layer is 
greater than the band gap in the laser=active region. The laser-inactive 
regions 232 preferably extend between the laser-active regions 228 
likewise in strip-shaped configuration in the first direction 230. 
Hence the laser amplification volume in the embodiment of the laser-active 
unit 214 illustrated in FIG. 14 is formed by the sum of the laser-active 
regions 228 and the laser-inactive regions 232 which both extend in the 
first direction 230. 
In the embodiment of the laser-active unit 214 illustrated in FIG. 14, the 
laser-active regions 228 and the laser-inactive regions 232 are the same 
length and so the laser-active unit comprises a front side 234 
representing one plane and in the same way a rear side, not illustrated in 
the drawing, extending parallel to the front side 234. The front side 234 
preferably extends perpendicular to the first direction 230. 
The strip-shaped laser-active regions 228 are of such dimensions that their 
narrow side 236 extending between the semiconductor layers 220 and 222 has 
approximately and expanse of 1 .mu.m and their broad side 238 extending 
perpendicular, i.e., parallel to the semiconductor layers 220 and 222, an 
expanse of approximately 2 .mu.m. Furthermore, the strip-shaped 
laser-active regions 228 extending the first direction 230 over a distance 
of the order of 1 mm. 
The narrow side 240 of the laser-inactive regions 232 also has the exactly 
the same width as the narrow side 236 of the laser-active regions 228, and 
a broad side 242 of the laser-inactive regions is of such dimensions that 
it has an expanse of the order of 5 .mu.m. 
The total expanse of the laser amplification volume 216 parallel o the 
broad sides 238 and 242 in the direction of a height 244 of the laser 
amplification volume 216 is of the order of 10 mm and so a correspondingly 
large number of laser-active regions 228 and laser-inactive regions 232 
alternate with one another. 
The laser-active units 214 are seated in the grooves 88 such that the 
respective layer amplification volume 216 is penetrated by the beams 20 
and 22, respectively, with the beams 20 and 22, respectively, extending 
with their directions of propagation 21 and 23, respectively, parallel to 
the first direction 230 of the respective laser-active unit 214. 
Furthermore, the beams 20 and 22, respectively, have such an expanse in a 
transverse direction 25 to its direction of propagation 21, 23 that they 
extend within the laser amplification volume 216 and hence between the 
semiconductor layers 220 and 222, the width of the narrow sides 236 and 
240, respectively, of the laser-active regions 228 and the laser-inactive 
regions 232, respectively. 
The fourth embodiment operates by the beam 20 and 22, respectively, 
penetrating the laser amplification volume 216, with laser amplification 
being imparted to the segments of the beams 20 and 22, respectively, 
passing through a laser-active region 228, whereas no laser amplification 
is imparted to the other segments passing through the laser-inactive 
regions 232. Averaged over the respective beam 20 and 22, respectively, 
the laser amplification is, however, so great that the emerging laser beam 
has the power of a high-power laser. 
Owing to the small dimensions of the successive laser-active regions 228 
and laser-inactive regions 223, these act like a phase grid extending in 
the direction of the height 244 for the beam 20 and 22, respectively, 
passing through the laser amplification volume 216. For this reason, the 
laser-active regions 228 and the laser-inactive regions 232 are preferably 
made of a semiconductor material which has a similar index of refraction. 
Furthermore, the extent of the laser-active regions 228 and the 
laser-inactive regions 232 in the direction of the first direction is 
preferably such that the segments of the respective beams 20 and 22, 
respectively, passing through these move through the same optical path 
length so that these have the same phase position after passing through 
the laser-active regions 228 and the laser-inactive regions 232. 
This is either achievable with a planar front side 234 and a planar rear 
side by the extent of the laser-active regions 228 and the laser-inactive 
regions 232 in the direction of the first direction 230 being selected 
accordingly. 
Or, alternatively, with the laser=active unit 214' of the variant of the 
fourth embodiment, illustrated partially and on an enlarged scale in FIG. 
15, the constant phase position of the segments of the beam 20 and 22, 
respectively, penetrating the laser-active regions 228' and of the 
segments of the beams 20 and 22, respectively, penetrating the 
laser-inactive regions 232' is achievable by these segments having a 
different length in the first direction 230. This is achievable by, for 
example, the front side 234 no longer being one plane but, for example, 
having grooves 248 lying between the laser-active regions 228' so that end 
faces 250 of the laser-active regions 228 lie in one plane and end faces 
252 of the laser-inactive regions 232' in another plane, with the latter 
plane being offset in the first direction 230 in relation to the one first 
mentioned. 
Owing to the spacing of the two planes, the above-mentioned same phase 
position of the segments of the beams 20 and 22, respectively, passing 
through the laser-active regions 228 and the laser-inactive regions 232' 
can be achieved in the variant 214' of the laser-active unit. 
In a further variant 214" of the laser-active unit, illustrated partially 
in FIG. 16, the laser-inactive regions 232" are produced as material-free 
channels 254 which extend parallel to the laser-active regions 228" so 
that segment of the respective beam 20 and 22, respectively, run either 
through one of the laser inactive regions 228" with a pumped semiconductor 
layer or through one of the channels 254 produced material by etching. 
With this variant of the laser-active unit 214", too, the aim is preferably 
for the phase position of the segments passing through the laser-active 
regions 228" to be identical with that of the segments of the beams 20 and 
22, respectively, passing through the laser-inactive regions 232", i.e., 
through the channels 254 so that the expanse of the laser-active regions 
228" in the first direction 230 and the expanse of the channels 254 in the 
first direction 230 are likewise coordinated. 
In all of the variants of the inventive laser-active unit, pumping of the 
laser-active regions 228, 228' and 228" is carried out in the usual way 
for semiconductor lasers with the pumping means 218 and is described, for 
example, in Principles of Lasers, 3rd. Ed., by O. Svelto, Plenum Press, 
New York 1989 and/or in Handbook of Solid State Lasers, by P.K. Cheo, 
Marcel Dekker Inc., New York 1989. 
For the rest, the fourth embodiment of the inventive solution operates in 
the same way as the second embodiment and so reference is to be had in 
full in this connection to the statements on the second embodiment. 
In the same way as described by way of example in connection with the 
fourth embodiment in comparison with the second embodiment, replacement of 
the solid-state rods 46 and 48 by laser-active units 214, 214' and 214" is 
also possible in the first and third embodiments. 
In a fifth embodiment of the inventive solid-state laser, illustrated in 
FIG. 17, the optical resonator designated in its entirety 262 is 
represented as half of a confocal unstable resonator. Herein a convex 
mirror 264 and a concave mirror 266 are arranged facing one another and 
extend from an optical axis 268 of this resonator 262 in a transverse 
direction 270, the expanse of the convex mirror 264 in this transverse 
direction 270 being shorter than that of the concave mirror 266 so that a 
laser beam 272 starting from the concave mirror 266 emerges from the 
resonator 262 at the side of the convex mirror 264. 
The confocal mirror surface 274 and 276, respectively, of the convex mirror 
264 and the concave mirror 266 are preferably designed as cylindrical 
mirror surfaces and hence extend in a height direction 278 perpendicular 
to the transverse direction 270 and perpendicular to the optical axis 268 
parallel to one another, as illustrated in FIG. 18. 
Such as confocal resonator with cylindrical mirrors is described in detail, 
for example, in German patent 37 29 053 or in A.E. Siegman, Unstable 
Optical Resonators, Appl. Optics, 13, pages 353-367 (1974). 
A plurality of excitation sections 280 is arranged between the mirrors 264 
and 266 in the beam path of the resonator 262. These excitation sections 
280 lie between two coupling sections 282 and 284 immediately adjoining 
the mirrors 264 and 266, respectively. A joint beam of the resonator 262 
is present in these coupling sections 282 and 284. This joint beam 286 is 
coherent and has a beam path like that known in confocal unstable 
resonators. The joint beam 286, for its part, is made up of partial beams 
292 lying directly alongside one another in the transverse direction 270. 
For each excitation section 280, one of the partial beams 292 of the joint 
beam 286 is imaged by means of an optical element 288 and 290, 
respectively, in the form of a cylindrical optical means on either side of 
the excitation section 280 into a beam 294 in this excitation section 
which extends with its longitudinal direction 296 between the two 
cylindrical optical means 288 and 290. The cylindrical optical means 288 
and 290 image the partial beam 292 into the beam 294 such that its extent 
in the transverse direction 25 parallel to the transverse direction 270 is 
less than the extent of the partial beam 292 in the transverse direction 
270. 
As illustrated in FIGS. 17 and 19, there is arranged in each excitation 
section 280 a laser-active unit 214 whose laser amplification volume 216 
is penetrated by the beam 294 with an essentially parallel beam path, the 
first direction 230 of the laser amplification volume 216 extending 
parallel to the direction of propagation 296 of the beam 294. Furthermore, 
the height 244 of the laser amplification volume 216 extends parallel to 
the height direction 278. Hence the extent of the beam 294 in the 
transverse direction 25 is less than or equal to the expanse of the narrow 
side 236 of the laser-active regions 228. Furthermore, the width of the 
laser-active unit 214 in the transverse direction 270 corresponding at the 
most to the width of the respective partial beam 292 in this direction. 
In the fifth embodiment, a plurality of laser-active units 214 are placed 
close together and form a laser-active block 298, the laser amplification 
volume 216 of the individual laser-active units 214 being arranged in 
succession at constant, equal spacings in the transverse direction 270. 
The cylindrical optical means 288 and 290 are each designed such that, as 
mentioned previously, they image a partial beam 292 with an essentially 
parallel beam path and a certain extent in the transverse direction 270 
into the beam 294 of the respective excitation section 280 with an 
essentially parallel beam path, the extent of each partial beam 292 in the 
transverse direction 270 being such that the following partial beam 292 
immediately adjoining it is detected by the following cylindrical optical 
means 288 and 290, respectively, and hence, in all, the joint beam 286 is 
imaged in the region of the laser-active block 298 continuously into the 
beams 294 so that the block 298 appears transparent for the joint beam 286 
although there are non-transparent regions between the individual beams 
294 of the individual excitation sections 280 but owing to the imaging by 
the cylindrical optical means 288 and 290, these do not have a shading 
influence on the joint beam 286. 
Furthermore, in the design of the cylindrical optical means described 
hereinabove, the beam divergence upon emergence of the beam 294 from the 
laser amplification volume 216 owing to the small width of the beam 294 in 
the transverse direction 25 has to be taken into consideration and so the 
scattering effect of the cylindrical optical means 298 and 290 has to be 
of correspondingly smaller dimensions. 
The extent of the joint beam 286 in the height direction 278 is selected 
such that it is at the most equal to or less than the extent of the laser 
amplification volume 216 in the direction of the height 244. Moreover, the 
cylindrical optical means 288 and 290 are of such dimensions that, for 
their part, they extend at least over the extent of the joint beam 286 in 
the height direction 278 and do, therefore, also not contribute to any 
switching-off of the joint beam in this direction. 
The laser-active units 214 which form the laser block 298 can be designed 
in the same way as in the fourth embodiment or its variants so that the 
block 298 can be made up of the laser-active units 214, 214'or 214". 
Therefore, regarding the design of the laser-active units 214, reference is 
to be had in full to the statements on the fourth embodiment in this 
context. 
In a variant of the fifth embodiment, illustrated in FIG. 20, several 
laser-active units 214a and 214b are arranged one behind the other in each 
excitation section 280 in order to increase the amplification in the 
individual excitation sections 280 by enlarging the extent of the 
laser-active regions in the first direction 230. In this variant, in the 
simplest case, the laser-active regions 228 are arranged in alignment with 
one another and the laser-inactive regions 232 in alignment with one 
another so that the optical lengths of the laser-active regions 228 add 
up. This does, of course, require the dimensions of the laser-active 
regions with respect to their narrow sides 236 and their broad sides 238 
as well as the dimensions of the laser-inactive regions 232 with respect 
to their narrow sides 240 and their broad sides 242 to be identical. 
In a further variant, illustrated in FIG. 21, two laser-active units 214c 
and 214d are likewise provided in each excitation section 280, the 
laser-active unit 214d adjoining the layer-active unit 214c being arranged 
such that its laser-active regions 228 are not in alignment with the 
laser-active regions 228 of the laser-active unit 214c but instead with 
the laser-inactive regions 232 of the laser-active unit 214d and, 
conversely, the laser-active regions 232 with the laser-active regions 228 
of the laser-active unit 214c. 
In this case, it is particularly advantageous for the cross-sections of the 
regions in respective alignment with one another to be identical so that, 
in all, each segment of each beam 294 passes one time through a 
laser-inactive regions 232 and another time through a laser-active region 
228, and the laser-active regions 228 and the laser-inactive regions 232 
is both laser-active units 214d and 214c preferably have equally long 
dimensions in the first direction 230 so that after passing through the 
two laser-active units 214c and 214d all of the segments of the beam 214 
have the same phase position. 
Common to both variants of the fifth embodiment is, however, always that 
the two laser amplification volumes 216 of the two laser-active units 214a 
and b as well as 214c and d are in respective alignment with one another, 
have the same cross-section and the two layer amplification volumes 216 in 
alignment with one another are penetrated by a single beam 294. 
In a sixth embodiment, illustrated in FIGS. 22 and 23, the resonator 300 is 
designed as confocal, unstable resonator comprising spherical mirrors 304 
and 306 arranged symmetrically in relation to a resonator axis 302. The 
mirror 304 is a convex mirror and the mirror 306 a concave mirror, and the 
concave mirror 306 extends beyond the convex mirror 304 so that a 
ring-shaped laser beam 308 with rays running parallel to the resonator 
axis 302 emerges from the resonator 300 past the convex mirror 304. Hence 
the joint beam 286 extends symmetrically from the resonator axis 302 as 
far as the emerging laser beam 308. Such resonators are described in 
detail in A.E. Siegman, Unstable Optical Resonators, Appl. Optics, 13, 
pages 353-367 (1974). 
The extent of the joint beam in the transverse direction 270 is, therefore, 
identical with that in the height direction 278. 
Two block 298e and 298f are provided in the sixth embodiment, illustrated 
in FIG. 22 and FIG. 23, and their laser amplification volumes 216a and 
216b are respectively arranged in an excitation section 280e and 280f and 
are penetrated by a beam 294e and 294f of the respective excitation 
section 280e and 280f. Each of the excitation sections 280e and 280f is 
provided on either side thereof with a cylindrical optical means 288e, 
290e and 288f, 290f, respectively, which image the beam 294e and 294f, 
respectively, in the respective excitation section 280e and 280f, 
respectively, into the joint beam 286 so that the joint beam 286 is, in 
turn, also present between the two excitation sections 280e and 280f. 
Moreover, in the sixth embodiment, the laser excitation volumes 216e and 
215f are arranged such that the laser excitation volume 216e stands 
parallel to the height direction 278 but the laser excitation volume 216f 
parallel to the transverse direction 270. In the same way, the cylindrical 
optical means 288e, 290e and 288f, 290f are arranged in tilted relation to 
one another through 90.degree. respectively. Furthermore, the extent of 
both laser-active blocks 298e and 298f in the transverse direction 270 is 
preferably selected such that this identical. 
Hence a homogenization of the laser amplification in the joint beam 286 is 
achieved with the arrangement according to the sixth embodiment where one 
time the width of the partial beam 292 parallel to the transverse 
direction 270 is reduced by imaging by the cylindrical optical means 288e, 
290e and another time the extent of parts of the partial beam 292 in the 
height direction height 278 is compressed by the cylindrical optical means 
288f, 290f owing to the optical imaging by the cylindrical optical means 
288f, 290f. 
In a seventh embodiment, illustrated in FIG. 24, the laser amplification 
volumes 216 of the block 298g and h are aligned parallel to one another 
but are offset in relation to one another in the transverse direction 270 
such that each laser amplification volume 216h is seated between two laser 
amplification volumes 216g. In the same way, the optical elements 288g, 
290g and 288h, 290h are also offset in relation to one another in the 
transverse direction 270 so that, for example, part of the rays of 
adjacent beams 294g is imaged into the beam 294h by each optical element 
288h. 
In the fifth, sixth and seventh embodiments, it is likewise possible for 
the laser-active units 214, 214' and 214" to be replaced by the 
solid-state rods 46 and 48, with optical pumping occurring in the 
direction of the height direction 278, for example, in the fifth and 
seventh embodiments.