Convincing: Examples for expertise and custom specific development
Overview
> Lenses for laser process observation
> Observing lenses
> Optical coherence tomography
> F-theta lenses for polygon scanners
> Lenses for mask imaging
> Different housing material for UV lenses
> Dynamic z shifting optics
> Alignment turning
> Measurement of the centering error
> Beam manipulation
> Special shapes
ZnSe lenses for CO2 lasers
Sill Optics is able to design and manufacture scan lenses, beam expanders and other customized special lenses from zinc selenide for applications with CO2 lasers.
CO2 lasers emit in the infrared spectral range at wavelengths between 9 and 11 µm. The spectrum is far above the wavelengths used for conventional laser material processing.
Due to their high cutting quality, CO2 lasers are often used to process transparent materials such as acrylic or Plexiglas. In addition, CO2 lasers are also used in machines for laser material processing of wood, textiles and plastics as well as for oxide-free cutting of sheet metal or for drilling circuit boards. The application of infrared lasers is diverse and common in various sectors such as the automotive, electrical or textile industries.
Nevertheless, the long-wave CO2 lasers challenge optical designers who design and manufacture the focusing scan lens and the upstream beam expander, as only a few glasses are transparent in this spectral range. The transmission curves show that zinc selenide and germanium are among the few materials that absorb less than 30 - 60 % at infrared wavelengths, while conventional optical glasses or fused silica are completely opaque in this range.
Fig.1: transmission curves of common optical glasses and ZnSe (all materials without coating; material thickness between 5 and 10 mm)
Zinc selenide is usually preferred to germanium due to its higher temperature resistance. The processing of zinc selenide is particularly difficult due to the soft material properties and toxic particles that are released during manufacturing. However, the finished lens is not toxic, as the material is only toxic if swallowed or inhaled according to the safety data sheet.
Zinc sulphide (ZnS) is a good alternative to zinc selenide (ZnSe) if the visible and short-wave infrared range (SWIR) is also to be imaged. It is also cheaper and non-toxic during processing. However, if lasers with a wavelength of 10.6 µm are used with medium or high power, ZnSe must still be used because ZnS absorbs significantly more radiation at this wavelength. This results in greater heating and lower transmission.
A special coating is then applied to the finished lens in order to reduce reflection at the transitions from glass to air or vice versa. As the transmission of the uncoated material barely exceeds 70%, the effect of the coating is strong. At wavelengths between 2 and 13 µm, an increase of over 20 percentage points is possible (see Fig. 2). This means that less energy remains in the lens, resulting in less heating and higher efficiency. Nevertheless, special coatings must be applied for this extremely long-wave spectral range, whereas standard coatings are designed for the range of a few hundred nm.
Fig. 2: transmission curves of non-coated and AR coated ZnSe (material thickness: 5 mm)
The engineers at Sill Optics have risen to these challenges and have already developed some lenses for the use of CO2 lasers. Since these types of lenses are no standard products, they are not included in the Sill catalog. Nevertheless, we Sill Optics has the expertise to design CO2 lenses, have coated lenses manufactured and install them in specially designed and manufactured mounts and housings. If you require optics such as scan lenses or beam expanders for your CO2 system, Sill Optics would be delighted if you would contact them with your specifications. The engineering team will then develop a lens in close consultation with you, according to your wishes and ideas.
Lenses for laser process obervation
Conventional observation lenses
Conventional observation lenses do not suffice for three dimensional scan field measuring. Optical coherence tomography is a contactless method and the solution for this kind of process observation.
The basic idea is the superposition of the wavelength of two beam paths. The generated interferogram helps to calculate a distance difference between reference and measuring beam path. If reference distance and distance difference are known the distance of the measuring beam path can be calculated. Other measurements, which are displaced in x- and y-direction create a three-dimensional map of the scan field. Accuracies in the range of some micrometers can be reached.
Optical coherence tomography
Conventional observation lenses do not suffice for three dimensional scan field measuring. Optical coherence tomography is a contactless method and the solution for this kind of process observation.
The basic idea is the superposition of the wavelength of two beam paths. The generated interferogram helps to calculate a distance difference between reference and measuring beam path. If reference distance and distance difference are known the distance of the measuring beam path can be calculated. Other measurements, which are displaced in x- and y-direction create a three-dimensional map of the scan field. Accuracies in the range of some micrometers can be reached.
F-Theta lenses for polygon scanners
Standard galvanometer scanners are often not fast enough for lasers with extremely high repetition rates. Ultrafast polygon scanners are a highly suited alternative in this case. They are line scanning systems and much faster than galvanometer scanners, which highly decreases the laser processing time. Many existing f-theta lenses are suitable without significant impact on the performance. However, Sill Optics offers custom lenses to exploit the full advantage of the possibilities of polygon scanners.
Lenses for mask alignment
There are two methods usually used for micro-structuring with lasers, maskless or direct write and mask projection.
Flexibility, ease of use and cost effectiveness are the features of the direct laser process with DPSS laser for feature sizes on a micrometer scale.
Mask projection systems usually use excimer lasers where a mask pattern is de magnified by a certain factor to reach feature sizes on a sub-micrometer scale. Additional benefits are good depth uniformity and distortion free features.
A combination of both techniques is the so-called “Scanned Mask Imaging (SMI)”. An expanded, homogenized and shaped beam scans a mask using a 2D scanner and a telecentric f-theta lens. The illuminated area of the mask is de-magnified with a double side telecentric low distortion lens onto the substrate area. Sill Optics designs telecentric lenses for scanning and distortion free imaging on customers’ requirements.
Different housing material for UV lenses
Long term exposure of black anodized aluminium housing parts to ultraviolett light can lead to bleaching. Eventually released particles might contaminate the lens surfaces and result in a decreased lifetime on the optical components. Therefore it is possible to buy f-thtea lenses and beam expanders for the ultraviolet wavelength band with a resistant colorless anodized housing (no extra costs). For scan lenses a special order of such a housing is necessary, but there is an extra catalog series for UV beam expanders ("S6EXN").
Dynamic z shifting optics
Besides the well-known f-theta lenses for galvanometer scanners where the scanner is prior to the scan lens, lens systems with adjustable focal length could be used for processing flat fields. These lens systems incorporate a moving lens and a focusing system. The position of the moving lens in respect to the focusing lens has to be synchronized with the scanner movement to avoid a spherical scan field. So it is possible to create an even scan field, but the beam spot diameter depends on its position and changes more over the field in respect to f-theta lenses. Nevertheless there are some applications which utilize the big advantage of working in three dimensions with z shifting optics.
Alignment turning
Alignment turning is a high precise production technique which enables a minimum tilt between lens axis and optical axis. Production accuracy is about one micrometer with this tool. Before starting the process it is necessary to fi x the lens into its housing by curling, sticking or using knurled rings. After that the lens becomes positioned inside the machine so that optical and mechanical axis are exactly in line with each other. With the help of ceramic tools, the outer surfaces as well as the front and rear bearing surfaces are centered. Outside diameter tolerances of just a few microns are producible. If there are high specifications on lens centering, Sill Optics uses this technique for producing modern high precision optics.
Measurement of the centering error
It is useful to check the position and geometry of individual lenses after assembly for projects with a high centering sensitivity. The centering error of each surface within an optical system can be measured with a sub-micron resolution. If required the design can be adjusted after assembly which decreases the centering error extremely.
The measuring device can also be used for cementing pairs of lenses. Specifically it can be checked whether the center thickness, air gaps and radii are within the tolerance for systems with up to 20 surfaces.
Beam manipulation
Due to the constantly growing requirements for throughput and precision, in many industrial applications beam splitters and beam shapers are in use.
Beam splitters are optical components that split a beam into two or more beams with a certain angular spacing. To realize this, so-called DOEs, diffractive optical elements are often used. DOEs can generate 1D or 2D patterns. The angles between neighboring orders depend on the order numbers and are not linear. This nonlinearity results in non-equidistant spacing of focal points if standard lenses are used. To compensate this scan lenses can be designed in a special way.
Beam shaper transform a single mode Gaussian beam into a beam with uniform energy distribution. Diffractive or aspherical optical elements are used to achieve this. It should be noted that in subsequent optical systems such as beam expanders or f-Theta objectives, more than twice the beam diameter is often required as a free aperture. In addition, the imaging power must be diffraction limited to obtain the beam shape.
Special shapes
Sill Optics offers various customized rotationally symmetric optics. The product portfolio ranges from spherical lenses to aspheres and segmented lenses. Upon request, Sill Optics is happy to develop custom lenses designed specifically for your application.