tutorial modifying laser beams -...

Ophir Photonics Group

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Tutorial: Modifying Laser Beams – No Way

Around It, So Here’s How

By John McCauley, Product Specialist, Ophir Photonics

There are many applications for lasers in the world today with even more on

the horizon. In order to apply a laser to an industrial process, medical

therapy or communications technology it is usually necessary to modify the

laser beam to achieve the desired results. Laser beam measurement tools

make this possible. In this article we will discuss how to match an

appropriate laser beam profiling technique to a laser application. The topics

will include building an aligned optical system, collimation and focusing, high

power laser quality measurements and proper attenuation techniques for

making accurate laser measurements.

Building an Aligned Optical System

Many laser applications are based on a system that includes a laser with

associated optics to deliver a laser beam of known size and position to do

something. Examples of these are as diverse as laser printers and marking

machines, laser range finder, LIDAR or military targeting systems, and laser

projection systems for movie theatres. What all of these have in common is

the need to put a beam of a certain size at a certain place in space. Using a

beam profiler allows this to be done quickly and efficiently — simply place

the profiler where the beam is to be aimed and measure the size and position.

These parameters can be adjusted with direct feedback from the profiler.

Beam profilers to do this can be either based on CCD or CMOS array or

scanning slit technology. Each has its advantages. Arrays will provide a true

two dimensional image of the beam and show any irregularities in power

distribution; scanning slits will provide an XY profile, but can measure much

smaller beams, as small as 10µm, and will require little or no attenuation or

adjustment to the profiler itself. In addition, the scan plane of the slit

profiler is very well known, allowing the z-location of a beam waist to be

located very accurately. Both camera and slit profilers can determine the x-y

position of the beam in space to less than a µm.


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Fig 1. Scanning slit and array profilers.

For applications where pointing accuracy is very important it is necessary to

isolate linear and angular pointing error and also to eliminate external

influences on the measurement. Pointing accuracy is dependent on the

profiler, the fixturing of the laser system and external influences. Localized

heating, air currents, vibration all contribute to uncertainty in pointing

measurements. One way to isolate external influences is to shrink the

measurement to as short a distance as possible. Rather than measuring

pointing over a distance of 10s of meters, using a very accurate profiler on the

bench top can deliver better results. By using scan averaging with a

NanoScan slit scanning profiler it is possible to measure pointing accuracy to

submicron precision, allowing a range finder to be aligned in a very small test

fixture.

Isolating linear from angular pointing error can be done with a two profiler

method. By splitting the beam and looking at the near-field and far-field

through an f-theta lens these motions can be separated. Angular motion will

show up as a shift in the near-field measurement, but will not be seen in the

far-field due to the f-theta correction. Linear motion, on the other hand will

be seen in the far-field as a shift in position on the far-field profiler.


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Fig 2. Angular vs linear pointing measurement set up.

This may be more than most applications need, and simply placing the

profiler where the beam is to be delivered is usually enough.

Collimation and Focusing

Other applications often require that a laser either be focused to a particular

beam waist or collimated to a minimally diverging or converging beam.

Focusing can be a fairly simple process for low power beams, such as those

used in fiber optic telecommunication or point-of-sale scanners. It is much

more complicated for higher power applications like ophthalmic surgery,

medical therapeutics or precision welding. For a low power application, one

can simply place the profiler at the focus point and adjust the optics until the

desired beam size if obtained. This is routinely done with passive optical

components for free space coupling of fiber.

Fig 3. Focusing fiber optic components.

Measuring a higher power focused beam can be much more difficult because

the power density of the laser increases geometrically as beam size shrinks.

Although the slit scanner can often handle direct measurement of fairly high


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power beams, often the power density can exceed the damage threshold for

the slit material. Camera measurement of focused beams is always a bit

more complicated, because arrays always need attenuation to measure lasers

without saturating the signal. With a focused beam it is usually impossible to

get the focused beam to the array through attenuators without distortion.

Fig 4. Focused beam has different path lengths through attenuator.

The attenuation in Fig. 4 is much simpler than is normally used and it would

still cause distortion. The solution to this problem is to image the beam waist

with a lens, with the attenuation added to the image.

Fig 5. Focused spot profiler.


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This method can also be used with a scanning slit profiler to reduce the

power density of the beam, again geometrically. For example if one has a

15W laser beam that is focused to 10µm, the power density would exceed the

damage threshold of the slit material. However, by expanding the beam 10X,

the power density will be reduced by 100-fold, bringing it back to the safe

level.

Fig 6. Beam expander with slit profiler.

Collimation

Collimation is the opposite of focusing, that is, it is the process of making the

laser have the same diameter for as long a distance as possible. Laser

applications that need this type of adjustment include laser point-of-sale

scanners, LIDAR and rangefinders, guide stars and free-space optical

communications; basically anything that needs a beam that maintains a

uniform beam size over a long distance. Another application is the

collimation of a large beam that will then be focused to a small diameter.

There are actually two types of collimation; one can be described as the

minimum divergence, and the other as the maximum distance to the waist.

When collimating for minimum divergence, the following formula defines the

divergence angle, θ = Dƒ / ƒ, using a lens of known focal length. By placing a

beam profiler at the geometric focus of the lens, adjusting the collimation to

produce the minimum spot size at this point achieves the best collimation.

This type of collimation is important for situations where the mathematically

accurate value for θ is important, such as when creating a collimated beam to

be refocused to a specific size and Rayleigh range. In many cases, simply

adjusting for the maximum distance to the waist, or focusing to infinity, is

sufficient to provide the performance required.


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Fig. 7. Lens collimation method.

It is also possible to use the above divergence measurement technique to

achieve the divergence that will provide the proper distance-to-the-waist

desired. There is a more thorough discussion of collimation of Gaussian

beams in Donald O’Shea’s Elements of Modern Optical Design.1

High Power Beam Quality Measurements

High power lasers are used for many industrial applications, particularly

high precision welding, brazing and cutting operations. The laser is well

suited to these operations and can be a rapid and efficient method, but only if

the laser is operation properly and delivering the correct beam shape and

power to the work piece. In order to guarantee this, there are several things

that can and should be measured periodically.

• Output power or energy

• Spatial or Beam Profile

• Waist position

• Temporal profile (for pulsed beams)

All of these beam quality parameters can affect the performance of the laser

in accomplishing its assigned task. Measurements should be made in order to

establish the criteria of a laser process to ensure stable, reliable and

consistent performance and to monitor this performance over time. Lasers

and optical delivery systems degrade over time, and monitoring the laser

criteria can help to prevent waste and rework if the laser performance no

longer meets the requirements of the process. Measurements should be made

whenever one is moving or expanding a process to another system, for batch

validation and for laser maintenance and troubleshooting. Many

1 O’Shea, Donald C., Elements of Modern Optical Design, John Wiley and Sons, 1985, pp. 241-5


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organizations operating under ISO 9001, GMP or GLP protocols will mandate

routine periodic measurement to ensure consistent and traceable results.

The technologies available for laser measurement include power and energy

meters, which indicate the total power or energy being delivered by the laser

system; beam profilers, which show the shape and size of the beam; and fast

photodiodes to measure the pulse shape of pulsed laser beams. Power and

energy meters are available in many varieties, depending on the nature of

the laser to be measured. Power meters are used for continuous wave (CW)

lasers and energy meters are used for pulsed beams. For most industrial

strength lasers these are either thermal sensors or pyroelectric sensors.

Thermal sensors, which detect the temperature rise caused by the laser and

convert it to an electrical signal, can be used to measure average power or

single pulse energy up to kWs or 100s of Joules. Depending on the power or

energy levels that they are designed to handle, they will have convection,

fans or water for cooling. For measuring repetitive pulse energies,

pyroelectric sensors are used. These comprise a crystal lattice that expands

and contracts in response to the laser pulses, creating a proportional

electrical signal and can be used up to 20kHz repetition rates and 10s of

Joules of energy. These are typically cooled by convection.

Fig 8. Various power and energy sensors.

Further information about the laser’s performance is provided by beam

profiling, as discussed above. However with high power lasers, beam

profiling becomes more complicated due to the potential for damage to the

profiler. Using attenuation devices, lasers can be sampled by camera based

array profilers, which will provide measurement of beam size, shape, spatial

energy distribution and beam wandering. Both array-based and scanning slit

based profilers can be used to measure focused spots to ensure that the laser

beam being delivered to the work piece is of the proper size to do the required

job. Other types of profilers such as a rotating pinhole or a spinning wand


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are able to sample a small portion of the beam and construct an image of the

profile, beam caustic and energy distribution of the beam.

Fig.9. High power monitoring setup.

For pulsed beam measurement the temporal profile of the pulses can provide

additional important information about the performance of the laser for a

particular operation. Leading edge spikes can cause a laser to create uneven

welds or ragged cuts. A fast photodiode can provide a good picture of the

temporal profile to see if poor performance of the laser system is the result of

irregular pulses, or some other cause.

Proper Attenuation Design for Laser Measurement

There are two basic types of attenuators used when making laser

measurements, reflective and absorptive. Within these two categories there

are different types and materials, but they effectively work in the same

manner. Absorptive attenuators are the colored or gray-glass filters that

work by absorbing some portion of the light, and they may be made of glass,

plastic or Inconel. Because they absorb light, they are subject to heating,

which then changes the optical properties of the material in a process called

“thermal lensing.” The localized heating in the filter material forms a lens

that can then modify the beam, causing erroneous profile information.

Reflective attenuators, such as laser end mirrors, quartz wedges or prisms

are not as susceptible to this phenomenon, and therefore should usually be

used for the first stages of attenuation of any lasers with powers greater than

100mW per millimeter diameter, or 12.7W/cm2 . This happens fast, and may

give the appearance of a stable laser profile. The following experiment shows

this dramatically:


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Experimental Design

An unfocussed CW beam from a Coherent DPSS 532 Laser (532nm

wavelength) with a nominal power of 500mW was measured using three

methods.

Method 1

Using the camera array beam profiler with all the attenuation provided by

absorptive filters, the beam was measured at a point 30cm from the exit

aperture of the laser. The attenuation comprised a 2.8OD gray-glass fixed

filter and the Photon ATP-K continuously variable wedge attenuator (1.7—

4.6OD).

Method 2

The first stage of attenuation was provided by using a front surface reflection

with additional attenuation provided by the ATP-K. The rest of the

measurement set up remained identical to that in Method 1.

Method 3

Measurements were then taken at the same measurement plane with the

Photon NanoScan scanning slit profiler, which needed no attenuation for this

laser power.

Results and Discussion

Because we expected to see thermal effects in the initial experimental design

(Method 1), we used time charting to observe the measurement of the laser.

In order to see any effects and eliminate any contribution from the laser

itself, we started the camera and then uncovered the laser beam. There was an immediate spike of the beam size to around 700µm. It settled to a value

around 500µm (1/e2) within a few milliseconds. With each measurement we

saw a similar pattern; however the value of the initial spike was somewhat

variable.


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Fig 10. Time chart of beam measurement made with absorptive attenuation only, showing

initial spike of beam size with stabilization to lower value.

Had time charting not been employed, the measurement would have appeared to be stable at the 400-500µm beam size.

Fig 11. Data display of beam size measurements made with absorptive attenuation only.

When this same experiment was repeated using the front surface reflection

attenuator, the spiking effect was no longer visible and the beam measurement was ~850µm in one axis and 914µm in the other.

Fig 12. Data display of camera beam size measurements with 4% front surface reflector

and ATP-K.

Measurement with the NanoScan showed a beam size measurement of ~850µm


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Fig 13. Data display of beam size measurements made with NanoScan profiler.

The measurements of the properly attenuated beam in the camera and the

NanoScan were within 2% agreement, which is the specification for accuracy

of these measurements. The beam measurements subject to thermal lensing

were 30-40% low, indicating that a very rapid lensing effect was taking place

in the first attenuator. Because this effect is so rapid, it is quite possible for

such errors to go unnoticed. The measurements did not exhibit the

“blooming” effect that might we expected from slower heating. Instead they

achieved equilibrium within a matter of milliseconds.

The power density of this laser beam was ~80W/cm2. The power going into

the ATP-K attenuator after the front surface reflector was 3.2W/cm2, which is

well below the theoretical thermal lensing limit of 12.7 W/ cm2. The

comparable results from this configuration and the NanoScan confirm that

thermal lensing effects do not occur at when the beam power incident on the

absorptive attenuator properly adjusted.

Conclusion

Matching your profiling technique to your laser application will allow you to

monitor and adjust you laser system to meet the requirements of the job at

hand. In many cases a laser profiler will make the process of building a laser

system much more efficient and accurate.

tutorial modifying laser beams -...

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