There is now a multitude of laser marking systems available at very affordable prices. Most commonly, such machines are lasers that react with the surface of the material for marking.
The suitability/reaction of the material to the laser is determined by the “laser wavelength”.
CO2 lasers, otherwise known as “gas lasers”, work best with materials such as wood, many types of plastic, card, leather and even glass. The typical operating wavelength of such a system is 10.6um (10,600nm) within the “Infrared Spectrum (IR)” and this type of laser is a surface marking system. If you own a laser system already then it is most likely to be a CO2 laser.
YAG lasers, otherwise known as “solid state lasers”, work best with materials such as metals, most types of opaque plastic and ceramics. The typical operating wavelength of a YAG laser is 1,064nm within the “Near Infrared Spectrum (NIR)” and this type of system is a surface marking machine. However, some materials are transparent to this laser wavelength, such as plate glass for example.
It is therefore possible to push the beam of a YAG laser at 1,064nm through a piece of plate glass and engrave stainless steel on the other side without affecting the glass at all.
IR and NIR lasers are invisible.
By using specific and additional components it’s possible to alter certain types of YAG laser by “frequency doubling” the wavelength from 1,064nm to 532nm.
Visible light ranges from 700nm to 400nm. Frequency doubled YAG at 532nm falls within the “Green Spectrum”, which is visible, and is therefore known as a “green laser”.
Green lasers can be used for high speed, fine detail surface marking and are a particular advantage when marking plastics but machines are now available that incorporate green laser technology to use for marking the inside of transparent materials, mostly crystal.
Such machines are capable of marking 3-dimensional designs with breathtaking speed and detail and so have proven very popular for marking images, logo’s, etc, to the inside of crystal giftware and promotional items as well as being used for part identification, anti-counterfeit and even architectural marking.
These types of machine are commonly known as “Sub Surface Laser Engraving” systems or “SSLE” for short.
With SSLE, images are represented as a series of co-ordinated points within the material. These points are actually micro fractures caused by rapid heating when the laser fires to a focused point. Within the laser industry such fractures are termed as “point clouds”.
As the laser beam passes through the crystal the material remains unaltered until the beam is honed to a “focal point”. The focal point is the smallest diameter that the lens is capable of focusing the beam to. The focal point will vary with each machine from approximately 20-80um depending on the design/build/technology levels of the machine.
A fracture is created when the laser beam is set to a sufficient energy enough to alter the structure of the material.
By altering the laser energy (power) the density/clarity of the point cloud can be adjusted. It’s important to note that using too much power and/or too many point clouds without sufficient spacing can cause the micro fractures to become a visible crack. At this point the image is flawed and so the part is rejected.
High resolution images tend to use point clouds of low laser power and low resolution images tend to use point clouds of high laser power.
Images are built-up by the laser marking many layers of point clouds. The laser always starts at the base of the image working upwards.
Design, control and layout software is used to determine the number and spacing of point clouds and layers within the image. Resolution is limited by the capability of the hardware.
SSLE, as with all YAG laser machines, use an intense and visible light as the source of the laser to “pump” the “laser medium” and generate the laser beam.
Older technology machines use a lamp as the light source.
Although lamp pumped lasers still have their uses in laser machines used for metal welding and cutting applications, as far as marking lasers are concerned, compared to more modern alternatives a lamp pumped marking laser is very inefficient and relatively unstable, deteriorating with use/time and often providing for inconsistent performance.
Lamps require frequent replacement, sometimes within just a few hundred hours of use, and are relatively high in power consumption. Therefore, frequency and cost of maintenance for a lamp pumped laser is relatively high. As a by-product of its very low efficiency a lamp pumped laser produces a high amount of heat that has to be taken away by a relatively large chiller unit. As a consequence, such a system often has a large footprint with high energy costs.
Risk of downtime when using a lamp pumped SSLE laser is higher than alternative technology and failure to maintain the system correctly can result in unnecessary and costly damage to the machine. Lamp pumped green lasers generate a relatively large focal point of between 40 to 80um. At this size significant space is required to be between the point clouds to prevent cracking. Therefore, such machines are incapable of engraving high detail, high resolution images.
Another weakness of the lamp pumped system is its pulse rate, measured in Hz: this is how fast the system can fire the laser pulse per second, which has a significant impact on how long it takes to produce the engraved design. Typically a lamp pumped system will work at maximum 200Hz (200 pulses per second).
Instead of a lamp, more modern systems use diodes to pump the laser medium. Such machines are known as “Diode Pumped Solid State” lasers or “DPSS” for short. DPSS lasers are much more efficient than lamp pumped machines and therefore consume far less power. As a consequence, they are much easier and cheaper to cool.
The performance of a DPSS laser is consistently good, as is its reliability. The diodes do not last forever and will require replacement at some point but typically a good quality diode will last for many thousands of hours, which can equate to years of use.
The rate of pulse for a good DPSS system will be 2 kHz (2,000 pulses per second), which equates to 10 times the speed of a typical lamp pumped machine. Some specialist systems, such as those used for architectural work, are capable of pulse rates as high as 5kHz but most machines cannot benefit from rates above 2kHz as there are factors other than the pulse rate that effect the systems top marking speed.
These machines generate small focal points of between 20 to 60um, which is about half the size of a lamp pumped alternative. Some DPSS machines can produce up to 4 x higher resolution than when compared to some lamp pumped systems.
In short, using a diode pumped system offers minimal system footprint, minimal downtime and minimal “total cost of ownership” (TCO) with maximum performance, output quality and reliability. For these reasons most people consider that a lamp pumped SSLE system is a false economy and so DPSS machines are now the most popular type of SSLE sold Worldwide.
After choosing DPSS as the basis for a good machine there is now the type of diode to consider as not all diode lasers are the same.
Differences in type of DPSS effect laser quality and reliability. As well as differences in quality/design for the core components the way in which the diodes are presented to the laser medium can differ too.
Lower cost diode lasers will normally pump the laser medium from the side. The best, highest quality output and performance comes from machines that incorporate diodes pumping the end of the laser medium. Such systems are known as “end pumped” diode lasers.
End pumped diode lasers typically use higher grade components and are more difficult to assemble/configure. Therefore, as a consequence they are higher in cost when compared to other types of DPSS system.
There are two ways to deliver the beam:
Over the last 10 years or so SSLE machines have evolved at a considerable pace and there is now a massive difference between the price, performance and output quality of SSLE machines of different make-up and technology.
For example, prices can range from as little as £15k to as much as £350k.
Like with most things in life and business “you get what you pay for”.
Low cost SSLE machines (£15k to £25k) are typically lamp pumped and consist of 3 axis (XY for the worktable and Z to focus the head). They offer no advantages other than low initial cost. In summary low cost SSLE machines are:
Although many transparent materials will mark to some extent with SSLE, those with minimal impurities, deformations and high thermal conductivity are best.
In general, low quality/cost products will mark better with lamp pumped laser technology and higher quality/cost products will mark better with DPSS laser technology.
Lead crystal is not suitable for SSLE apploication as the lead content of the glass will block the path of the SSLE beam.
You may often hear the term “K9” to describe a type of glass most suitable for SSLE.
Technically, K9 is a “borosilicate crown glass”. Borosilicate is commonly used to manufacture items such as test tubes and some household items like bowls for holding high temperature liquids. Pyrex, for example, is a form of borosilicate glass.
Crown glass (optical) is a term given to a type of borosilicate used in the manufacture of components used for optical purposes, such as lenses, etc. Crown glass can be worked to precise dimensions and is known to be more stable than other forms of glass.
Borosilicate crown glass has a very low “thermal expansion coefficient”. This means that it is resistant to thermal shock (when heat is applied), about one third that of normal glass. It also has “low dispersion” and a “low refractive index”. These terms are used to describe how much the glass absorbs light that enters in to it and how much the light is refracted (deflected at an angle) when it enters/exits the glass.
In short, K9 glass provides minimal beam absorption, minimal beam deflection and minimal heat reaction. It has fewer impurities and internal stresses than when compared to other types of glass.
Impurities and internal stresses prevent SSLE from producing clear, high quality results so wherever possible, for SSLE applications use K9 in preference to all other types of glass.
As with all of the laser technology that we supply, the right system is a machine capable of performing the application, within your budget, without too many restrictions and/or additional on-costs.
Purchasing the wrong SSLE system can be a very costly mistake.
As SSLE technology is a refined subject it is best you contact one of our qualified technical staff at email@example.com who would be pleased to advise you after a short consultation without obligation to buy.