The present invention relates to a device for absorbing a laser beam as claimed in the preamble of claim 1, as well as a device for attenuating a laser beam as claimed in the preamble of claim 9.
Disadvantages of known absorption devices for laser beams and so-called radiation traps, respectively, are the restriction to rotationally symmetric beam cross-sections and comparatively low beam intensities. However, in particular, laser diode bars have linear cross-sections and, at high beam intensities, present conventional radiation traps with major problems.
The problem on which the present invention is based is the creation of devices of the type mentioned initially which are suitable for laser beams with high beam intensities.
According to the invention, this is achieved by devices of the type mentioned initially with the characterizing features of claims 1 and 9. The dependent claims relate to advantageous developments of the invention.
Claim 1 provides for the device still to comprise optical means to expand the laser beam prior to its incidence on the absorption surface. Through expansion of the laser beam, the absorption surface can be used in a more effective manner for the absorption of the laser beam, so that laser beams of higher intensities can be absorbed.
The device may comprise a housing in which the absorption surface is arranged. In this case, it is possible for an elongated hole, through which the laser beam can enter the housing and be incident on the absorption surface, to be arranged in the housing. This elongated hole allows a laser beam with a linear cross-section to enter the absorption device in an effective manner; when the laser beam enters the housing, the line of the linear cross-section can extend in the longitudinal direction of the elongated hole.
Further features and advantages of the present invention will become clear from the following description of preferred exemplary embodiments and with reference to the attached figures, in which
The embodiment of a device according to invention for attenuating a laser beam as shown in
In the illustrated exemplary embodiment, the beam splitter means 3, 4 are in the form of plane-parallel plates, which are provided with a dielectric coating. For example, the coating is in this case chosen in such a way that, in the case of an angle of 45° (see example in
If the angle is not equal to 45°, a partial beam 6 passes through the first beam splitter means 3 and is incident on the second beam splitter means 4. Said beam splitter means 4 will preferentially be at an angle corresponding to that of the first splitter means 3 to the laser beam 5 that is to be attenuated, so that the beam offset caused by the plane-parallel plates is compensated for. In particular, the second beam splitter means 4 can be twisted synchronously with the first beam splitter means 3, so that in general the same percentage is reflected and transmitted. The partial beam 9 reflected by the second beam splitter means 4 enters the second of the devices 2 according to the invention for absorbing a laser beam and is likewise absorbed there. The beam 8 which has passed through the second beam splitter means 4 leaves the device according to the invention for attenuating a laser beam as the attenuated beam 8.
The housing 10 is elongated and is closed on its top face (as in
The elongated hole 17 is longer than it is wide. In particular, the elongated hole can be more than twice as long as it is wide. It is possible for the length of the elongated hole 17 to be three to five times or more than five times as large as the width of the elongated hole 17. For example, the elongated hole 17 can be five to ten times as long as it is wide and, in particular, it may be approximately seven or eight times as long as it is wide. It is also possible for the length of the elongated hole 17 to be more than ten times as large as the width of the elongated hole 17.
The cooling channels 13 run under the absorption surface 14, so that the heat produced by the absorbed laser radiation can be transported away from the absorption surface 14 in this manner.
Optical means 18 can be arranged in the region of the elongated hole 17. In the illustrated exemplary embodiment, the optical means are in the form of a plano-concave cylindrical lens, whose cylinder axis extends in the longitudinal direction of the housing 10 and in the longitudinal direction of the elongated hole 17. With the help of such a cylindrical lens, a laser beam incident on it is expanded in the transverse direction of the housing 10, so that it is distributed over a larger area of the absorption surface 14. In this manner, laser beams with relatively high intensities can be absorbed by the device 2 according to the invention.
In the illustrated exemplary embodiment, the cylindrical lens is arranged only in the front region according to
The top face of the housing 10, according to
Number | Date | Country | Kind |
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DE102005018986.5 | Apr 2005 | DE | national |
Number | Date | Country | |
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Parent | PCT/EP2006/003644 | Apr 2006 | US |
Child | 11876255 | US |