Patent Application
20230347451
Embodiments of the present invention relate to a device and a method for separating a material by means of ultrashort laser pulses.
In recent years, the development of lasers with very short pulse lengths, e.g., with pulse lengths below one nanosecond, and with high mean powers, e.g., in the kilowatt range, has led to a novel type of material machining. The short pulse length and high pulse peak power, or the high pulse energy of a few microjoules to 100 μJ, may lead to nonlinear absorption of the pulse energy within the material, with the result that it is even possible to machine materials that actually are transparent or substantially transparent to the utilized laser light wavelength.
A particular field of application for such laser radiation lies in the separation and machining of workpieces. In the process, the laser beam is preferably introduced into the material with perpendicular incidence as this minimizes reflection losses at the surface of the material. For machining materials at a work angle, for example for facing a material edge or for producing chamfer and/or bevel structures with work angles of more than 30°, this still represents an unsolved problem, also because the large work angles at material edge lead to a significant aberration of the laser beam, with the result that there cannot be a targeted energy deposition in the material.
Embodiments of the present invention provide a method for separating a workpiece having a transparent material. The method includes providing ultrashort laser pulses using an ultrashort pulse laser, introducing material modifications into the transparent material of the workpiece along a separation line using the laser pulses, and separating the material of the workpiece along the separation line. The laser pulses form a laser beam that is incident onto the workpiece at a work angle. The material modifications are Type I and/or Type II modifications associated with a change in a refractive index of the material of the workpiece. The material modifications penetrate two sides of the workpiece that are located in intersecting planes. Separating the material of the workpiece produces a chamfer and/or a bevel. A length of a hypotenuse of the chamfer and/or bevel is between 50 μm and 500 μm.
Subject matter of the present disclosure will be described in even greater detail below based on the exemplary figures. All features described and/or illustrated herein can be used alone or combined in different combinations. The features and advantages of various embodiments will become apparent by reading the following detailed description with reference to the attached drawings, which illustrate the following:
Embodiments of the present invention provide an improved device for separating a workpiece, and also a corresponding method.
According to some embodiments, a method for separating a workpiece comprising a transparent material is proposed, wherein ultrashort laser pulses from an ultrashort pulse laser are used to introduce material modifications into the transparent material of the workpiece along a separation line, and the workpiece is then separated in a separation step along the material modification area that has arisen as a result. According to embodiments of the invention, the laser pulses are brought into the transparent material of the workpiece at a work angle and the material modifications are Type I and/or Type II modifications, which are associated with a change in the refractive index of the transparent material of the workpiece.
The ultrashort pulse laser in this case makes ultrashort laser pulses available. In this context, ultrashort may mean that the pulse length is for example between 500 picoseconds and 10 femtoseconds and in particular between 10 picoseconds and 100 femtoseconds. In the process, the ultrashort laser pulses move in the beam propagation direction along the laser beam formed thereby.
When an ultrashort laser pulse is focused into a material of the workpiece, the intensity in the focal volume may lead to nonlinear absorption, for example by multi-photon absorption and/or electron avalanche ionization processes. This nonlinear absorption leads to the generation of an electron-ion plasma, and permanent structural modifications may be induced in the material of the workpiece when the said plasma cools. Since energy can be transported into the volume of the material by way of nonlinear absorption, these structural modifications in the interior of the sample may be produced without the surface of the workpiece being influenced.
In this context, a transparent material is understood to be a material that is substantially transparent at the wavelength of the laser beam from the ultrashort pulse laser. The terms “material” and “transparent material” are used interchangeably herein—which is to say the material specified herein should always be understood to be a material that is transparent to the laser beam of the ultrashort pulse laser.
The material modifications introduced into transparent material by ultrashort laser pulses are subdivided into three different classes; see K. Itoh et al. “Ultrafast Processes for Bulk Modification of Transparent Materials” MRS Bulletin, vol. 31, p. 620 (2006): Type I is an isotropic refractive index change; Type II is a birefringent refractive index change; and Type III is what is known as a void or cavity. In this respect, the material modification created depends on laser parameters such as the pulse duration, the wavelength, the pulse energy and the repetition frequency of the laser, on the material properties such as, among other things, the electronic structure and the coefficient of thermal expansion, and also on the numerical aperture (NA) of the focusing.
The Type I type isotropic refractive index changes are traced back to locally restricted fusing by way of the laser pulses and fast resolidification of the transparent material. For example, quartz glass has a higher density and refractive index of the material if the quartz glass is cooled more quickly from a higher temperature. Thus, if the material in the focal volume melts and subsequently cools down quickly, then the quartz glass has a higher refractive index in the regions of the material modification than in the non-modified regions.
The Type II type birefringent refractive index changes may arise for example due to interference between the ultrashort laser pulse and the electric field of the plasma generated by the laser pulses. This interference leads to periodic modulations in the electron plasma density, which leads to a birefringent property, which is to say directionally dependent refractive indices, of the transparent material upon solidification. A Type II modification is for example also accompanied by the formation of what are known as nanogratings.
By way of example, the voids (cavities) of the Type III modifications can be produced with a high laser pulse energy. In this context, the formation of the voids is ascribed to an explosion-like expansion of highly excited, vaporized material from the focal volume into the surrounding material. This process is also referred to as a micro-explosion. Since this expansion occurs within the mass of the material, the micro-explosion results in a less dense or hollow core (the void) or a defect in the sub-micrometer range or in the atomic range, which void or defect is surrounded by a densified material envelope. Stresses which may lead to a spontaneous formation of cracks or which may promote a formation of cracks arise in the transparent material on account of the compaction at the shock front.
In particular, the formation of voids may also be accompanied by Type I and Type II modifications. By way of example, Type I and Type II modifications may arise in the less stressed areas around the introduced laser pulses. Accordingly, if reference is made to the introduction of a Type III modification, then a less dense or hollow core or a defect is present in any case. By way of example, it is not a cavity but a region of lower density that is produced in sapphire by the micro-explosion of the Type III modification. On account of the material stresses that arise in the case of a Type III modification, such a modification moreover often is accompanied by, or at least promotes, a formation of cracks. The formation of Type I and Type II modifications cannot be completely suppressed or avoided when Type III modifications are introduced. Finding “pure” Type III modifications is therefore unlikely.
In the case of high laser repetition rates, the material is unable to cool down completely between the pulses, with the result that cumulative effects of the heat introduced from pulse to pulse may influence the material modification. By way of example, the laser repetition frequency may be higher than the reciprocal of the thermal diffusion time of the material, with the result that heat accumulation as a result of successive absorptions of laser energy may occur in the focal zone until the melting temperature of the material has been reached. Moreover, a region larger than the focal zone can be fused as a result of heat transport of the thermal energy into the areas surrounding the focal zone. The heated material cools quickly following the introduction of the ultrashort laser pulses, and so the density and other structural properties of the high-temperature state are, as it were, frozen in the material.
The material modifications are introduced into the material along a separation line. The separation line describes the line of incidence of the laser beam on the surface of the workpiece. For example, the laser beam and the workpiece are displaced relative to one another at a feed speed as a result of a feed, with the result that the laser pulses are incident on the surface of the workpiece at different locations as time passes. In this context, the feed speed and/or the repetition rate of the laser are chosen so that the material modifications in the material of the workpiece do not overlap but rather are present separate from one another in the material. In this case, displaceable relative to one another means both that the laser beam can be translationally displaced relative to a stationary workpiece and that the workpiece can be displaced relative to the laser beam. There may also be a movement of both the workpiece and the laser beam. The ultrashort pulse laser emits laser pulses into the material at its repetition frequency while the workpiece and laser beam are moved relative to one another.
The material modifications being pronounced in the beam propagation direction results in the creation of an area in the material of the workpiece in which all material modifications are present and which intersects the surface of the workpiece along the separation line. The area in which the material modifications are present is referred to as the material modification area. In particular, the material modification area may also be curved, with the result that material modifications which for example form the lateral surface of a cylinder or cone are also located within a material modification area.
The laser pulses are introduced into the material of the workpiece at what is known as a work angle. In this case, the work angle is given by the angle difference between the laser beam and the surface normal of the workpiece to be separated. When the work angle is not equal to zero, the material modification area is likewise inclined in relation to the surface normal of the workpiece. What needs to be taken into account in this context is that, in the case of a non-vanishing work angle, the laser beam is refracted depending on the respective refractive index of the surrounding medium, preferably air, and of the material of the workpiece, according to Snell's law. As a result, the beam propagation direction in the material of the workpiece may differ from the beam propagation direction prior to entry into the material of the workpiece. In particular, the material modification area may as a result also be tilted at a different angle with respect to the surface normal than the angle of incidence.
In the present case, Type I and II modifications are used to produce predetermined breaking points in the material, or weaken the material along the material modification area. The introduced Type I and Type II material weakening leads to the material being able to be separated along the material modification area.
The separation along the material modification area is implemented here within the scope of a separation step, with the result that the workpiece is divided into the bulk portion and what is known as the cutting of the workpiece.
In this case, the separation step may comprise a mechanical separation and/or a chemical separation step, preferably an etching procedure and/or an application of heat and/or a self-separation step.
By way of example, heat may be applied by way of a heating of the material or separation line or separation surface. By way of example, the separation line or separation surface may be heated locally by means of a continuous wave CO2 laser, with the result that the material in the material modification region expands differently in comparison with the untreated or unmodified material. However, an application of heat may also be realized by way of a hot air flow, or by baking on a hotplate or by heating the material in an oven. In particular, temperature gradients may also be applied within the scope of the separation step, in order thus to bring about a different thermal expansion within the material. The material modification and the material weakening accompanying this may ultimately lead to a promoted crack formation in the material modification area, with the result that a continuous and non-catching separation surface can form, by means of which the parts of the workpiece are separated from one another.
A mechanical separation may be generated by the application of a tensile or flexural stress, for example by the application of a mechanical load on the parts of the workpiece separated by the separation line or separation surface. By way of example, a tensile stress can be applied if opposing forces in the material plane act at a respective point of attack of the force on the parts of the workpiece separated by the separation line or separation surface, in a manner pointing away from the separation line or separation surface in each case. If the forces are not aligned parallel or antiparallel to one another, then this may contribute to the creation of a flexural stress. The workpiece is separated along the separation surface as soon as the tensile or flexural stresses are greater than the binding forces of the material along the separation line or separation surface. In particular, a mechanical change can also be obtained by a pulse-like action on the part to be separated. By way of example, a shock can generate a lattice vibration in the material. Tensile and compressive stresses which may trigger a crack formation in the material modification area can thus likewise be generated by the deflection of the lattice atoms. However, the material can preferably be separated by etching using a wet-chemical solution, with the etching process preferably placing the material against the material modification, which is to say the targeted material weakening. In other words, the selective etchability is increased by the introduction of the material modifications. The workpiece is separated along the separation surface as a result of the parts of the workpiece weakened by the material modification preferably being etched.
This is advantageous in that an ideal separation method can be chosen for the respective material of the workpiece, with the result that separation of the workpiece is accompanied by a high-quality separation edge.
Further, the material modifications may be introduced by accumulation of heat within the material of the workpiece.
Accumulation of heat may be achieved as a result of progressive absorption of the ultrashort laser pulses, provided that the pulse rate of the laser beam is greater than the rate of heat dissipation by material-specific heat transfer mechanisms. As a result of the increasing temperature in the material of the workpiece, it is thus ultimately possible to attain the melting temperature of the material of the joining partner, leading to local fusing of the material. As a result, a Type I and/or a Type II modification, in particular, can be generated in the material of the workpiece, as described above.
In order to fuse the material of the workpiece, it is possible to output a multiplicity of laser pulses at locations in the material, with these locations having to spatially overlap sufficiently such that an accumulation of heat can be attained despite the applied feed. In particular, the pulse overlap can be greater than 1, with the result that more than one pulse is output per location of incidence.
In this case, the spatial overlap needs to be greater than 1, with the overlap being given by df*R/V, where df is the beam diameter or the diameter of the transverse intensity distribution—see below—R is the repetition frequency of the laser, and V is the feed speed. The temporal pulse spacing needs moreover to be smaller than the diffusion time tD in the material, where the diffusion time is given by tD=(df/2){circumflex over ( )}2/2D, where D=kappa/(rho*cp) is the diffusivity, kappa is the thermal conductivity, cp is the specific heat capacity and rho is the density of the material. For example, the diffusion time in fused silica is 1 μs.
A high quality separation surface can be generated by the separation step by way of successively heating and fusing the material.
In particular, provision can be made for the material modifications to penetrate two sides of the workpiece which are located in intersecting planes, and for the separation step to produce a chamfer and/or a shaped edge, preferably a chamfer and/or a bevel.
Two sides are located in intersecting planes if the surface normals of the planes are not aligned parallel to one another. By way of example, in the case of a cuboid, two sides are located in intersecting planes if the sides can be connected by the edge of the cuboid. In the case of a disk-shaped material, the circumferential surface of the disk is, in a certain sense, located in an intersecting plane with the upper side and the lower side of the disk. At least when considered locally, a rectangular cross section arises in the plane of incidence of the laser beam even in the case of a disk.
The material modifications penetrate both adjacent sides. In this case, penetration means that the material modification starts on the one side and, in the beam propagation direction, finishes on the other side. However, this may also mean that the material modification only extends within the material of the workpiece in order to avoid chippings at the surface. However, a larger portion of the path of the laser between the two sides need to be modified by material modifications in this case. By way of example, as a result of positioning the material modifications in the material in strategically advantageous fashion, it may be sufficient to introduce material modifications along only a third of the path. However, it may also be possible for a material modification to be continuous over the entire path between the two sides.
As a result, a cutting of the workpiece arises in the plane of incidence of the laser beam in which the incident and the refracted beams are located. By way of example, this cutting may be triangular in the case of the cuboid. A triangular cutting of the workpiece has what is known as a hypotenuse, which is opposite the edge to be separated. In this case, the length of the hypotenuse is given by the length of the material modifications within the workpiece. Moreover, the distance of a side adjacent to the hypotenuse of the cutting is given by the distance of the separation line from the edge of the workpiece.
The predetermined breaking point is introduced over the entire hypotenuse length by virtue of the material modifications penetrating two sides of the material. As a result, the workpiece is separated along the material modification area in a subsequent separation step.
Following the separation, the material modification area becomes what is known as the shaped edge of the material. Shaped edges of the workpiece are subdivided into what are known as chamfers and bevels. In this case, a chamfer of the workpiece is understood to be a trim, in the case of which the original edge of the cuboid has been replaced by two edges. As a result, the original edge is diffused, or a transition region is created between a first cuboid side and a second cuboid side. By contrast, a bevel is produced if the hypotenuse of the cutting coincides with an edge of the workpiece or, in general, if a side of the triangular cutting corresponds to at least one side length of the workpiece running parallel thereto.
By way of example, the length of the hypotenuse of the chamfer and/or bevel is between 50 μm and 500 μm, preferably between 100 μm and 200 μm.
This is advantageous in that, as a result, the workpiece can be faced in a manner which is optically appealing and which has a high-quality effect. Moreover, it is consequently also possible to face relatively thick workpieces. Further, the provision of a shaped edge, a chamfer or a bevel allows a more stable edge to be obtained, the latter not chipping off as easily during the installation or in use at the final customer as an edge with a 90° angle.
The laser beam can be a non-diffractive laser beam.
In particular, non-diffractive beams and/or Bessel-type beams should be understood to refer to beams for which a transverse intensity distribution is propagation invariant. In particular, a transverse intensity distribution in a longitudinal direction and/or propagation direction of the beams is substantially constant in the case of non-diffractive beams and/or Bessel-type beams.
A transverse intensity distribution should be understood to mean an intensity distribution located in a plane oriented at right angles to the longitudinal direction and/or propagation direction of the beams. Moreover, the intensity distribution is always understood to mean the part of the intensity distribution of the laser beam which is greater than the modification threshold of the material. By way of example, this may mean that only some of the intensity maxima of the non-diffractive beam or only a few intensity maxima of the non-diffractive beam can introduce a material modification into the material of the workpiece. Accordingly, the phrase “focal zone” can also be used for the intensity distribution, in order to clarify that this part of the intensity distribution is provided in a targeted manner and an intensity boost in the form of an intensity distribution is obtained by focusing.
In respect of the definition and properties of non-refractive beams, reference is made to the following book: “Structured Light Fields: Applications in Optical Trapping, Manipulation and Organisation”, M. Wördemann, Springer Science & Business Media (2012), ISBN 978-3-642-29322-1. Express reference to the entire content thereof is made.
Accordingly, non-diffractive laser beams are advantageous in that they may have an intensity distribution which is elongated in the beam propagation direction, to a greater extent than the transverse dimensions of the intensity distribution. In particular, this renders possible the production of material modifications which are elongated in the beam propagation direction, with the result that these can penetrate the two sides of the workpiece easily.
The laser beam may have a non-radially symmetric transverse intensity distribution, with the transverse intensity distribution appearing elongate in the direction of a first axis in comparison with a second axis and with the second axis being perpendicular to the first axis.
In this case, non-radially symmetric means that the transverse intensity distribution depends not only on the distance to the optical axis but also at least on the polar angle about the beam propagation direction. By way of example, a non-radially symmetric transverse intensity distribution may mean that the transverse intensity distribution is, for example, cruciform or is triangular or is polygonal, for example is pentagonal. A non-radially symmetric transverse intensity distribution may also comprise further rotationally symmetric and minor-symmetric beam cross sections. In particular, a non-radially symmetric transverse intensity distribution may also have an elliptical form, with the ellipse having a major axis A and a minor axis B perpendicular thereto. Accordingly, an elliptical transverse intensity distribution is present if the ratio A/B is greater than 1, in particular if A/B=1.5. The elliptical transverse intensity distribution of the laser beam may correspond to an ideal mathematical ellipse. However, the non-radially symmetric transverse intensity distribution of the non-diffractive laser beam may also merely have the aforementioned ratios of long principal axis and short principal axis, and may have a different contour—for example an approximated mathematical ellipse, a dumbbell-type shape or any other symmetric or asymmetric contour enveloped by a mathematically ideal ellipse.
In particular, elliptical non-diffractive beams can be generated by way of non-diffractive beams. Here, elliptical non-diffractive beams exhibit special properties, which emerge from the analysis of the beam intensity. By way of example, elliptical quasi non-diffractive beams have a principal maximum which coincides with the center of the beam. The center of the beam is in this case given by the location at which the principal axes intersect. In particular, elliptical quasi non-diffractive beams may emerge from the superposition of a plurality of intensity maxima, wherein, in this case, only the envelope of the intensity maxima involved is elliptical. In particular, the individual intensity maxima do not have to have an elliptical intensity profile.
As a result of the non-radially symmetric transverse intensity distribution, the material modification in the cross section perpendicular to the beam propagation direction in the material will also likewise be non-radially symmetric. Rather, the shape of the material modification corresponds to the intensity distribution of the non-diffractive beam in the material of the workpiece.
In the case of non-diffractive beams, there are in particular regions of high intensity, which interact with the material and introduce material modifications, and regions below the modification threshold. The non-radially symmetric transverse intensity distribution in this case relates to the intensity maxima above the modification threshold.
For example, if the feed direction is parallel to the long axis of the transverse intensity distribution, it is possible to generate a large pulse overlap easily, as a result of which the feed speed can be increased. As a result, the separation process becomes faster and more cost effective.
In the projection of the non-radially symmetric transverse intensity distribution onto the surface of the workpiece, the first axis and the second axis may appear to have the same size as a result of the work angle.
The mathematical projection of the non-radially symmetric transverse intensity distribution onto the surface of the workpiece at the work angle may lead to distortions of the intensity distribution. Thus, for example, a round intensity distribution may be created on the workpiece by an originally elliptical intensity distribution. However, what may in particular also be achieved thereby is that an elliptical projection is realized on the surface of the workpiece by way of an originally round intensity distribution. As a result, material modifications with an intensity distribution which arise from the projection onto the surface of the workpiece at the work angle are introduced into the material.
However, the projection may also result in the distortion of a previously chosen preferred direction of the non-radially symmetric transverse intensity distribution, with the result that the preferred direction deviates from the actually effective intensity distribution.
In an embodiment, it is therefore preferable for the non-radially symmetric transverse intensity distribution to appear round as a result of the work angle. In particular, in the case of an originally elliptical transverse intensity distribution, this means that the major axis A and the minor axis B of the ellipse appear to have the same size as a result of the projection. As a result, it effectively is a round intensity distribution that acts in relation to the production of the material modifications.
The projection of the non-radially symmetric intensity distribution onto the surface of the workpiece can be elongated in the feed direction.
As a result, the distortion by the projection of the intensity distribution onto the surface of the workpiece can be controlled so that the long axis of the transverse intensity distribution points in the feed direction. By virtue of the preferred direction pointing in the direction of the feed direction and consequently running parallel to the separation line, it is possible to separate the workpiece easily and with a high quality along the material modification area arising as a result.
The material modification area can be inclined at an angle of up to 35° in terms of magnitude, in relation to the surface of the workpiece.
According to Snell's law, the product of refractive index of the surrounding medium and sine of the work angle corresponds to the product of refractive index of the material and sign of the angle of refraction. Accordingly, depending on the refractive indices, the work angle can be chosen so that the material modification area is inclined at no more than 35° with respect to the surface of the workpiece. In particular, the angle specification relates to the material modification area in which the material modifications are located, with the result that this angle directly corresponds to the angle of refraction.
The pulse energy of the laser pulses can be between 10 μJ and 50 mJ and/or the mean laser power can be between 1 W and 1 kW and/or the laser pulses can be individual laser pulses or part of a laser burst and/or the wavelength of the laser can be between 300 nm and 1500 nm, in particular 1030 nm.
This is advantageous in that optimal laser parameters can be provided for various materials.
By way of example, the ultrashort pulse laser may provide individual laser pulses with a pulse energy of 100 μJ, with the mean laser power being 5 W and the wavelength of the laser being 1030 nm.
A laser burst may comprise 2 to 20 laser pulses, with the laser pulses of the laser burst having a temporal spacing of 10 ns to 40 ns, preferably 20 ns.
By way of example, a laser burst may comprise 10 laser pulses and the temporal spacing of the laser pulses may be 20 ns. In this case, the repetition frequency of the laser pulses is 50 MHz. In this case, the laser bursts can be emitted at the repetition frequency of the individual laser pulses which is of the order of 100 kHz.
By using laser burst, it is possible to respond to the material-specific heat properties, with the result that it is possible to produce a shaped edge with a high surface quality.
Material modifications running parallel to the surface normal of the workpiece can be introduced into the material of the workpiece in a first method step and material modifications running at an angle to the surface normal of the workpiece can be introduced into the material of the workpiece in a second method step, with the material modification area of the second method step intersecting the material modification area of the first method step and with the separation step being carried out following the second method step.
In this context, material modifications which are able to determine the external dimensions of the workpiece following the separation step are introduced into the material of the workpiece by the first method step. The material modifications which lead to the creation of the chamfer or bevel with the separation step are introduced into the material of the workpiece by the second method step.
In this case, the separation step can be carried out after the first method step and after the second method step, with the result that two modification steps and two separation steps are needed in each case. However, the material modifications for cutting to length and for facing can also be introduced into the material of the workpiece in a first step, and can be separated in a joint separation step. As a result, at least one separation step can be economized, as a result of which the method can be carried out in time-efficient fashion.
The incident laser beam may be polarized parallel to the plane of incidence.
The refraction of the laser beam during the transition from the surrounding medium to the material of the workpiece does not only depend on the work angle and the refractive indices. In this case, the polarization of the laser beam also plays an important role. Using the so-called Fresnel equations, it is possible to show that, for an angle of incidence of greater than 10°, the transmission through a material of a laser beam polarized parallel to the plane of incidence is always greater than the transmission of a laser beam polarized perpendicular to the plane of incidence.
In particular, it is thus possible to minimize reflection losses of the laser beam with P-polarization, in order to realize an optimal energy yield for the separation process within the material. Moreover, advantageous energy input coupling into the material can be obtained in the case of an incidence of the laser beam at the Brewster angle.
The object stated above is also achieved by means of a device for separating a workpiece having the features of claim 11. Advantageous developments are evident from the dependent claims, the description and the figures.
Accordingly, a device for separating a workpiece comprising a transparent material is proposed, comprising an ultrashort pulse laser configured to provide ultrashort laser pulses, a processing optical unit configured to introduce the laser pulses into the transparent material of the workpiece, and a feed device configured to move the laser beam made of laser pulses and the workpiece relative to one another with a feed along a separation line and to orient the optical axis of the processing optical unit at a work angle relative to the surface of the workpiece. According to embodiments of the invention, the laser pulses are introduced into the transparent material of the workpiece at a work angle, wherein the material modifications are Type I and/or Type II modifications, which are associated with a change in the refractive index of the material of the workpiece.
By way of example, a processing optical unit can optically imaging system. By way of example, a processing optical unit may consist of one or more component parts. By way of example, a component part can be lens or an optically imaging free-form surface or a Fresnel zone plate. By way of the processing optical unit, it is possible to determine, in particular, the depth at which the intensity distribution is introduced into the material of the workpiece. In a sense, this can set the placement of the focal zone in the beam propagation direction. For example, a focal zone can be placed onto the surface of the workpiece, or preferably be placed into the material of the workpiece, by adjusting the processing optical unit. By way of example, this allows a focal zone to be set so that the laser beam penetrates through two adjacent sides and consequently leads to the creation of a material modification which, by means of a separation step, allows a whole-area separation of the workpiece.
By way of example, in this case the feed device can be an XY stage or an XYZ stage, in order to vary the point of incidence of the laser pulses on the workpiece. In this case, the feed device can move the workpiece and/or the laser beam so that the material modifications can be introduced into the material of the workpiece, next to one another along the separation line.
A feed device can likewise have an angle adjuster such that the workpiece and the laser beam can be rotated relative to one another about all Euler angles. This can ensure that the work angle can be maintained along the entire separation line.
In particular, the work angle is also understood to be the angle between the optical axis of the processing optical unit and the surface normal of the workpiece material. In this case, the work angle between the optical axis of the processing optical unit and the surface normal can be between 0 and 60°, for example.
A beam shaping optical unit can shape a non-diffractive laser beam from the laser beam, with the transverse intensity distribution of the non-diffractive laser beam being able to be non-radially symmetric, with the non-radially symmetric transverse intensity distribution being able to be elongate in a first axis in comparison with the second axis, and with the second axis being perpendicular to the first axis.
By way of example, the beam shaping optical unit can be in the form of a diffractive optical element (DOE), a free-form surface in a reflective or refractive embodiment or an axicon or a micro-axicon, or may contain a combination of a plurality of these component parts or functionalities. If the beam shaping optical unit shapes a non-diffractive laser beam from the laser beam upstream of the processing optical unit, then it is possible by way of the focusing of the processing optical unit to determine the depth at which the intensity distribution is introduced into the material. However, the beam shaping optical unit may also be configured in such a way that the non-diffractive laser beam is only generated by way of imaging with the processing optical unit.
A diffractive optical element is configured to influence one or more properties of the incident laser beam in two dimensions. A diffractive optical element is a fixed component which can be used to produce exactly one intensity distribution of a non-diffractive laser beam from the incident laser beam. Typically, a diffractive optical element is a specifically formed diffraction grating, with the incident laser beam being brought into the desired beam shape by the diffraction.
An axicon is a conically ground optical element which shapes a non-diffractive laser beam from an incident Gaussian laser beam as the latter passes through. In particular, the axicon has a cone angle α which is calculated from the beam entrance surface to the lateral surface of the cone. As a result, the marginal rays of the Gaussian laser beam are refracted to a different focal spot than near axis rays. In particular, this yields an intensity distribution which is elongate in the beam propagation direction.
The processing optical unit may comprise telescope system configured to introduce the laser beam with a reduced and/or increased size into the material of the workpiece.
An increase or in a reduction in the size of the laser beam or in its transverse intensity distribution allows the laser beam intensity to be distributed over a large or small focal zone. As a result of distributing the laser energy over a large or small area, the intensity is adapted such that, in particular, it is also possible to make a choice between modification types I, II and III by way of the increase and/or decrease.
In particular, by increasing or reducing the non-radially symmetric transverse intensity distribution, it is also possible to introduce larger or smaller material modifications into the material of the workpiece. For example, introducing a smaller elliptical transverse intensity distribution into the material is accompanied by a reduction in the radius of curvature of the material modification introduced thereby. In other words, a given curvature becomes more pointed as a result of a reduction in size. This can promote a crack formation in the material of the workpiece. Moreover, the optical system can be adapted to match the given machining conditions by way of an increase or a reduction in size, with the result that the device can be used more flexibly.
The feed device may comprise an axis device and a workpiece holder which are configured to move the processing optical unit and the workpiece relative to one another along three spatial axes in translational fashion and about at least two spatial axes in rotational fashion.
By way of example, an axis device can be a 5-axis device. By way of example, the axis device can also be a robotic arm which guides the laser beam over the workpiece or which moves the workpiece vis-à-vis the laser beam.
As a result of the laser beam and the workpiece being moved relative to one another for the purpose of being able to introduce the material modifications along the separation line, it is necessary for the laser beam or the workpiece to be locally co-rotated in order to maintain the work angle relative to the separation line. As a result, the material modification area may always have the same angle with respect to the surface of the workpiece in the case of curved separation lines.
In particular, such an axis device at the same time also allows a non-radially symmetric transverse intensity distribution to be oriented relative to the separation line, so that material modifications whose preferred directions run parallel to the separation line and which promote a crack formation along the latter are produced.
Moreover, an axis device may also comprise fewer than the 5 movable axes for as long as the workpiece holder is movable about the corresponding number of axes. By way of example, if the axis device is only displaceable in the XYZ-directions, then the workpiece holder may for example have two rotational shafts in order to rotate the workpiece relative to the laser beam.
The beam components of the laser beam can be incident on the workpiece at an angle of incidence of no more than 80° with respect to the surface normal of the workpiece.
As a result of the processing optical unit, the laser pulses converge to the optical axis, which is oriented at the work angle with respect to the surface normal of the workpiece. In this case, the component laser rays of the ray bundle include an angle with respect to the optical axis of the processing optical unit. In particular, these angles may include very large or very small angles as a result of the numerical aperture.
By virtue of these enveloping component laser rays of the laser ray bundle being incident on the surface of the workpiece at an angle of no more than 80°, it is possible to avoid large reflection losses. According to the Fresnel formulas, the reflection and transmission of the laser beam at the surface of the workpiece depends on the angle of incidence and the refractive indices. In the case of grazing incidence of the laser beam only little laser light can input couple into the material, and so effective material machining ceases. Moreover, the shape of the non-diffractive beam can be negatively influenced as a result.
A polarization optical unit, preferably comprising a polarizer and a waveplate, can be configured to adjust the polarization of the laser beam relative to the plane of incidence of the laser beam, preferably to set the said polarization parallel to the plane of incidence.
A waveplate, such as what is known as half-wave plate, can rotate the polarization direction of linearly polarized light through a selectable angle. As a result, it is possible to impress a desired polarization on the laser beam.
By way of example, a polarizer can be a thin-film polarizer. The thin-film polarizer only transmits laser radiation with a specific polarization.
Therefore, the polarization state of the laser radiation can always be controlled with a combination of waveplate and polarizer.
A polarization of the laser beam parallel to the plane of incidence is advantageous according to the Fresnel formulas in that, for an angle of incidence of more than 10°, the transmission is always greater than if the laser beam were polarized perpendicular to the plane of incidence. In particular, the transmission in the case of a parallel-polarized laser beam is more constant and uniform over a greater range of angles of incidence than in the case of perpendicular-polarized light. As a result, it is also possible to use a processing optical unit with a large numerical aperture. In the process, there would be an asymmetric beam reflection at the surface of the workpiece in the case of a perpendicular-polarized laser beam, with the result that optical aberrations reduce the quality of the material modifications and hence the quality of the separation surface.
A beam guiding device can be configured to guide the laser beam to the workpiece, the beam guidance being implemented by way of a minor system and/or an optical fiber, preferably a hollow core fiber.
What is known as a free-beam guidance uses a minor system in order to guide the laser beam in various spatial dimensions from a stationary ultrashort pulse laser to the beam shaping optical unit. A free-beam guidance is advantageous in that the entire optical path is accessible, and so for example further elements such as a polarizer and a waveplate can be installed without problems.
A hollow core fiber is a photonic fiber which is able to flexibly transmit the laser beam from the ultrashort pulse laser to the beam shaping optical unit. The adjustment of a minor optical unit can be dispensed with as a result of the hollow core fiber.
Control electronics can be configured to trigger a laser pulse emission of the ultrashort pulse laser on account of the relative positions of laser beam and workpiece.
A local reduction in the feed speed may be advantageous in the case of curved or polygonal feed trajectories. However, in the case of a constant repetition frequency of the laser, this may lead to the material modification area not being formed homogeneously, with the result that a uniform surface quality cannot be obtained during the separation step. For this reason, control electronics are able to control the pulse emission on the basis of the relative position of laser beam and workpiece.
By way of example, the feed device may comprise a spatially resolving encoder which measures the position of the feed device and laser beam. An appropriate trigger system of the control electronics may trigger the pulse emission of a laser pulse at the ultrashort pulse laser on the basis of the spatial information.
In particular, computer systems may also be used to trigger the pulses. By way of example, the locations of the laser pulse emission may be defined for the respective separation line prior to the machining of the material, with the result that an optimal distribution of the material modifications along the separation line is ensured.
What this achieves is that the spacing of the material modifications is always the same, even if the feed speed varies. In particular, what this also achieves is that it is possible to produce a uniform separation surface, and the chamfer or bevel has a high surface quality.
The workpiece holder may have a surface that does not reflect and/or does not scatter the laser beam.
In particular, this can prevent the laser beam from being guided back into the material, and causing another material modification there, after it has passed through the material. In particular, a non-reflective and/or non-scattering surface may also increase safety at work.
Preferred exemplary embodiments are described below with reference to the figures. In this case, elements that are the same, similar or have the same effect are provided with identical reference designations in the different figures, and a repeated description of these elements is omitted in some instances, in order to avoid redundancies.
During the transition into the workpiece 1, the laser beam 20 is refracted at the surface 10 of the workpiece 1 according to Snell's law, and so the laser beam 20 continues to propagate in the material of the workpiece 1 at the angle β with respect to the surface normal N. The material of the workpiece 1 is heated in the focal zone 220 of the laser beam 20, preferably by accumulation of heat, as a result of the introduction of the laser pulses into the workpiece 1 by way of the laser beam 20. In this case, the material of the workpiece 1 in the focal zone of the laser beam is fused, with the material of the workpiece 1 having a different refractive index vis-à-vis the original state during the renewed cooling down. The modification of the material of the workpiece 1 in the focal zone 220 is referred to as material modification 5, with the material modifications 5 being Type I or Type II material modifications in particular. As a consequence of the material modifications 5, the material of the workpiece 1 is weakened in targeted fashion, with the result that a targeted separation of the material 1 by way of a separation step is enabled.
In this case, the pulse energy of the laser pulses can be between 100 and 50 mJ and/or the mean laser power can be between 1 W and 1 kW and/or the laser pulses can be individual laser pulses or part of a laser burst and/or the wavelength of the laser can be between 300 nm and 1500 nm. Moreover, it may be the case that a laser burst comprises 2 to 20 laser pulses, with the laser pulses of the laser burst having a temporal spacing of 10 ns to 40 ns, preferably 20 ns.
As shown in
In the case of an elongate material modification 5 in the beam propagation direction, what is known as a material modification area 50, within which the material modifications 5 are located, is produced within the material of the workpiece 1 by the simultaneous feed V of the laser beam 20. In this case, the material modification area 50 is preferably introduced homogeneously into the material of the workpiece 1, which can be obtained by way of a sufficient pulse overlap of the laser pulses in the material 1. The workpiece 1 is separated into what is known as the bulk workpiece 1′ and into what is known as the cutting 12 by way of the material modification area 50. By way of example, the material modification area 50 can be inclined at an angle β of up to 35° in terms of magnitude, in relation to the surface 10 of the workpiece 1.
The material of the workpiece 1 is weakened in a targeted manner by the material modifications 5 in the material modification area 50, with the result that the workpiece 1 and the cutting 12 can be separated from one another easily along this material modification area 50.
The actual separation can be realized by specific separation steps. By way of example, the cutting 12 can be separated from the bulk workpiece 1′ over an area by chemical action on the cutting 12. By way of example, the cutting 12 can be separated from the bulk workpiece 1′ in a chemical bath, as shown in
What is known as a chamfer and/or a bevel, as shown in
To produce a shaped edge 14, it is advantageous for the material modifications 5 to penetrate those sides of the workpiece 1 which form the edge that should be faced. By way of example, the sides 10 and 11 in
In
In
In each case shown, what is known as the hypotenuse H of the cutting 12 is given by the length of the material modifications in the material.
Even if the description to this point has been reduced to the separation of cuboids, round materials 1 or rounded-off materials can also be separated by way of the method. By way of example,
A further example is shown in
A further example is shown in
What are known as non-diffractive laser beams 20 are suitable for producing simple material modifications 5, which penetrate the workpiece 1 at least in sections. Non-diffractive beams 20 preferably have an elongate focal zone 220 of length L in the beam propagation direction. The workpiece 1 can be faced easily and effectively by virtue of the length L of the focal zone 220 being greater than the length of the desired hypotenuse H of the cutting 12.
Aberrations arise in the material in the case of an oblique incidence of the laser beam 20, which is to say in the case of a non-vanishing work angle α, since the upper beam is incident on the workpiece 1 at an angle α+α′ and the lower beam path is incident at the angle α−α′. As a result, the focal zone 220 may shorten or become distorted, as shown in
In a manner analogous to
If a laser beam 20 with such a focal zone 220 is introduced into the workpiece 1, then the material modification 5 arising as a result has the same form, as shown in
If a laser beam 20 with a round or a non-radially symmetric transverse intensity distribution is projected onto a surface 10 of the workpiece 1 at a work angle α, then this results in a distortion of the intensity distribution in the plane of incidence. This is shown in
In particular, the laser beam 20 can be polarized, preferably be polarized parallel to the plane of incidence, in order to minimize reflection losses. In this respect,
By way of example, in the case of a work angle α=50° and a convergence angle of α′=20°, the component laser rays 200 are incident on the surface 10 of the workpiece 1 in an angular range from α−α′=30° to α+α′=70°. As a result, the transmission in the case of parallel incidence ranges between 96% and 94% while it varies between 95% and 70% in the case of perpendicular incidence. Accordingly, the variation for laser beams 20 polarized perpendicular to the plane of incidence is significantly more pronounced than that for light polarized parallel to the plane of incidence. Therefore, for the purpose of reducing reflection losses, it is advantageous for the component laser rays 200 to be incident on the workpiece 1 at an angle of less than 80° with respect to the surface normal N.
In this case, the polarization optical unit 32 may comprise a polarizer which polarizes the laser beam 20 emitted by the ultrashort pulse laser 2 such that the said laser beam only has a well-defined polarization. Then, a subsequent half-wave plate can ultimately rotate the polarization of the laser beam 20 such that the laser beam 20 can be introduced into the workpiece 1 with a polarization preferably parallel to the plane of incidence.
In the example shown, the beam shaping optical unit 34 is an axicon for shaping the incident laser beam 20 into a non-diffractive laser beam. However, the axicon may also be replaced by other elements for the purpose of generating a non-diffractive beam. The axicon generates a conically tapering laser beam 20 from the preferably collimated input beam. In this context, the beam shaping optical unit 34 may also impress a non-radially symmetric intensity distribution on the incident laser beam 20. Finally, the laser beam 20 can be imaged into the workpiece 1 via a telescope optical unit 36, which consists of two lenses 360, 362 here, with the imaging being able to be a magnifying or a reducing imaging. A part of the telescope optical unit 36, in particular the lens 360, may also be integrated in the beam shaping optical unit 34. By way of example, a refractive free-form surface or an axicon with a spherically polished back side may incorporate both the lens function of the lens 360 and the beam shaping function of the beam shaping optical unit 34.
In particular, the laser beam 20 can be input coupled into the processing optical unit 3 by way of a beam guiding device 38. In this case, the beam guiding device may be a free-space path with a lens and mirror system, as shown in
In the present example of
In this case, the feed device 6 can move the workpiece 1 under the laser beam 20 with a feed V such that the laser beam 20 introduces material modifications 5 along the desired separation line 4. In particular, in the shown
For this purpose, the feed device 6 may also be connected to control electronics 64, the control electronics 64 converting the user commands of a user of the device into control commands for the feed device 6. In particular, predefined cutting patterns may be stored in a memory of the control electronics 64 and the processes may be automatically controlled by the control electronics 64.
The control electronics 64 may in particular also be connected to the ultrashort pulse laser 2. In this context, the control electronics 64 may demand or trigger the emission of a laser pulse or a laser pulse train. The control electronics 64 may also be connected to other specified components and may thus coordinate the material machining.
In particular, a position-controlled pulse trigger can be realized in this way, with for example an axis encoder 600 of the feed device 6 being read out and the axis encoder signal being interpreted as a location specification by the control electronics 64. Consequently, it is possible that the control electronics 64 automatically trigger the emission of a laser pulse or laser pulse train, for example if an internal adder unit, which adds the traversed path length, reaches a value and resets to 0 after this value has been reached. Thus, for example, a laser pulse or laser pulse train can be automatically emitted into the workpiece 1 at regular intervals.
By virtue of it being possible to also process the feed speed V and the feed direction, and hence the separation line 4, in the control electronics 64, there can be an automated emission of the laser pulses or laser pulse trains.
The control electronics 64 are also able to calculate, on account of the measured speed and the fundamental frequency provided by the laser 2, the distance or a location at which a laser pulse train or laser pulse should be emitted. What can be achieved as a result in particular is that the material modifications 5 form a material modification area 50 that is as homogeneous as possible.
By virtue of the emission of the laser pulses or the pulse trains being implemented under position control, complicated programming of the separation process can be dispensed with. Moreover, freely selectable process speeds can be implemented easily.
Insofar as applicable, all individual features presented in the exemplary embodiments can be combined with one another and/or interchanged, without departing from the scope of the invention.
While subject matter of the present disclosure has been illustrated and described in detail in the drawings and foregoing description, such illustration and description are to be considered illustrative or exemplary and not restrictive. Any statement made herein characterizing the invention is also to be considered illustrative or exemplary and not restrictive as the invention is defined by the claims. It will be understood that changes and modifications may be made, by those of ordinary skill in the art, within the scope of the following claims, which may include any combination of features from different embodiments described above.
The terms used in the claims should be construed to have the broadest reasonable interpretation consistent with the foregoing description. For example, the use of the article “a” or “the” in introducing an element should not be interpreted as being exclusive of a plurality of elements. Likewise, the recitation of “or” should be interpreted as being inclusive, such that the recitation of “A or B” is not exclusive of “A and B,” unless it is clear from the context or the foregoing description that only one of A and B is intended. Further, the recitation of “at least one of A, B and C” should be interpreted as one or more of a group of elements consisting of A, B and C, and should not be interpreted as requiring at least one of each of the listed elements A, B and C, regardless of whether A, B and C are related as categories or otherwise. Moreover, the recitation of “A, B and/or C” or “at least one of A, B or C” should be interpreted as including any singular entity from the listed elements, e.g., A, any subset from the listed elements, e.g., A and B, or the entire list of elements A, B and C.
| Number | Date | Country | Kind |
|---|---|---|---|
| 10 2020 134 197.0 | Dec 2020 | DE | national |
This application is a continuation of International Application No. PCT/EP2021/080510 (WO 2022/128242 A1), filed on Nov. 3, 2021, and claims benefit to German Patent Application No. DE 10 2020 134 197.0, filed on Dec. 18, 2020. The aforementioned applications are hereby incorporated by reference herein.
| Number | Date | Country | |
|---|---|---|---|
| Parent | PCT/EP2021/080510 | Nov 2021 | US |
| Child | 18336045 | US |
