The above and other objects, features, and advantages will become more readily apparent from the following description, reference being made to the accompanying drawing in which:
As seen in
A focusing lens 7 in the beam path focuses the laser beam 2 at a focal plane 20 on which the laser beam has its focal point and thus its minimum extension in the x and y directions, so that the laser power at the surface is at a maximum. It is necessary for marking that the surface to be marked be placed on this plane, since the most effective marking having the sharpest contour is obtained at this location due to the minimum focal point and the resulting maximum power density.
Displacement of the surface to be marked along the z axis away from the focal plane 20 causes enlargement of the focal point, and thus a quadratic-reduction in the power density, so that satisfactory marking results are obtained only within a focal depth range between upper boundary plane 20a and a lower boundary plane 20b. Outside this region the achievable marking results are unsatisfactory, or marking is not possible at all.
If as shown in
When, for example, two deflection mirrors 31a and 31b are used in the mirror system 31 define a given angle, for example 90°, and form a prism-shaped reflector, for example, a laser beam 2 incident on the mirrored surface 31a or 31b is deflected either in direction 32a or 32b, depending on the previous deflection, so that in this example two marking cones 5a and 5b result that form different second fields.
By means of the respective third reflector assembly, composed of deflection mirrors 33a and 33b, provided downstream, these marking cones 5a and 5b are deflected in such a way that the surface of the object 10 to be inscribed, composed of different third fields, is marked in the partial areas 34a and 34b such that the partial areas combine to form a common marking surface 34.
The distance of the respective partial areas 34a and 34b from the focusing lens 7 corresponds to the focal distance of the lens 7 used, so that each partial area 34a and 34b essentially lies in the focal plane. For this purpose, the deflection mirrors 33a and 33b may be displaceably and/or rotatably attached in a mount (not illustrated) in order to conform the respective distances of the partial areas to be inscribed to the marking lens 7.
When objects that essentially are always the same are inscribed, this adjustment is made once. In addition, for a suitable choice of the directions of impingement for the marking cones 5a and 5b on the surface of the object 10 to be marked, the respective partial areas 34a and 34b lie within the allowable focal depth, so that the entire marking in the marking surface 34 as a whole lies within the allowable focal depth, and a high-quality marking is thus possible. Of course, the marking cone may also be split into more than the two partial cones stated as an example, for example into three, four, or more partial cones, in order to inscribe spherical or conical surfaces.
In an alternative embodiment according to the invention, it is also possible to mark elongated concave surfaces as shown in
It may also be practical to omit a marking lens 7. In this case the deflection mirrors 31a and 31b and/or 33a and 33b are designed as curved mirrors so that the laser beam 2 is similarly focused in a focal plane lying essentially on the surface of the object to be inscribed. The curved mirrors may have spherical, parabolic, hyperbolic, or similar designs, or may also be off-axis mirrors, depending on requirements.
For the inscription, any laser is suitable that has a wavelength, power, and operating system that allows adequate marking in each particular case, for example gas lasers such as CO2 lasers, argon lasers, metal vapor lasers, ion lasers, excimer lasers, etc., or semiconductor lasers or solid-state lasers such as Nd:solid-state lasers, ruby lasers, alexandrite lasers, sapphire lasers, or also free-electron lasers.
Number | Date | Country | Kind |
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102006037921.7 | Aug 2006 | DE | national |