
Figure 1: Intensity distribution of experimentally measured Gaussian beams (left) and top hat beams (right).
Most laser beams have Gaussian intensity distributions; however, in some applications, it may be more beneficial to use non-Gaussian beams. A Gaussian beam has an intensity distribution cross-section that decreases symmetrically with increasing distance from the center. In contrast, a top hat beam maintains a constant intensity distribution across the cross-section, allowing for consistent irradiation intensity on the target during processing (see Figure 1). As a result, more accurate and predictable results can be achieved in applications such as semiconductor wafer processing, other materials processing and nonlinear frequency conversion for high-power lasers.
top hat beams produce cleaner cuts and sharper edges than Gaussian beams, but generating top hat beams adds additional system cost and complexity. Understanding the benefits of top hat beams and the different methods of generating them can help laser system integrators select the right type of laser beam for their type of application.
Characteristics of Gaussian Beams
Gaussian lasers are more common and cost-effective than other beam types of laser sources. Most high-quality, single-mode lasers emit a beam that follows a low-order Gaussian irradiance profile, which is also known as the TEM00 mode. Lesser quality sources will also have some degree of other laser modes present, but usually assume the laser has a desirable Gaussian profile to simplify system modeling.
If the Gaussian beam has the same average optical power as the top hat beam, the peak irradiance of the Gaussian beam will be twice that of the top hat beam. As a Gaussian beam propagates through an optical system, it maintains a Gaussian irradiance profile distribution even if the peak intensity or beam size changes. This means that the Gaussian beam remains constant as it propagates.
What are the problems with Gaussian beams?
Gaussian beams have their drawbacks. In applications where the high intensity portion of the beam in the center is used, the low intensity portion of the beam on either side (the so-called "wings") is often wasted, because the laser intensity is higher than the threshold required for the application, whether it is material processing, laser surgery, or other applications.
In addition, the wings of the Gaussian beam may also damage areas beyond the target zone, thereby enlarging the heat-affected zone. This is detrimental to applications such as laser surgery and precision material processing, where high precision and minimal heat-affected zones are prioritized. As a result, materials processed with Gaussian beams will not have particularly smooth edges, thus reducing the accuracy of the system.
Why use top hat beams?
Compared to Gaussian beams, top hat beam profiles do not have winged sections and have steeper edge transitions, resulting in more efficient intensity transfer and a smaller heat affected zone. [2] Etching, welding, or cutting with a top hat beam will be more precise and less damaging to the surrounding area.
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This major advantage of top hat beams makes them suitable for many different situations. In laser-induced damage threshold (LIDT) testing and other metrology systems, the uniform intensity distribution of top hat beams minimizes measurement uncertainty and statistical variance. top hat beams are also advantageous in fluorescence microscopy, holography and interferometry systems.
One way to assess whether an actual laser beam is close to a perfect top hat beam is to analyze its flatness factor (Fη), which is calculated by dividing the average irradiance value by the maximum irradiance value of the beam, as described in the ISO 13694 standard.

What are the disadvantages of top hat beams?
The top hat beam is not suitable for all applications. It is not as cost-effective as a Gaussian beam because an additional beam shaping component is required to shape the Gaussian beam into a top hat beam. This component can either be built directly into the laser source or used in a system outside the laser. These beam shaping components depend on the size of the input beam and are sensitive to X-Y plane alignment. In addition, unlike Gaussian beams, top hat beams do not remain constant during propagation. This means that an incident top hat beam will not maintain its top hat shape as it travels through the system, and will eventually evolve to resemble an Airy spot distribution.
How is a top hat beam realized?
If a top hat beam is desired, but the system cost is very limited and the performance does not need to be very high, the Gaussian beam can be physically truncated using a small aperture to create a pseudo-top hat profile. This method cuts off and wastes energy from both wings of the Gaussian beam and does not even out the intensity distribution in the center of the beam. This method may be useful if maintaining low cost is a major factor.
For high-performance systems that require efficient use of laser energy, beam shaping components can be used to shape the Gaussian beam into a top hatped beam. There are several different types of beam shaping components, including refractive, reflective, holographic, and diffractive devices. Refractive beam shaping devices use field-mapped aspherical or free-form lenses and other refractive components to modulate the phase of the beam (see Figure 2). The advantage is a uniform intensity distribution and a flat phase front. The amplitude and phase of the incident beam are modulated by optical elements in a Galilean or Keplerian lens assembly. This process is typically highly efficient (greater than 96%) and wavelength independent over the range of device designs. Refractive beam shapers produce collimated, top hatped beams that are particularly well suited for applications that operate over long distances, such as holographic imaging and microscopy systems.

Figure 2: Shaping a Gaussian beam into a top hat beam using the AdlOptica πShaper top hat beam shaper from AdlOptics of Edmund Optics, based on operating principles such as wavefront aberrations and energy conservation conditions.
Other types of refractive beam shapers that shape the Gaussian beam into a quasi-straight Airy spot. The advantage of this is that the Airy spot, when focused by a diffraction-limited lens set, forms a focusing point with a top hat profile. In many applications such as micromachining, lithography, and microwelding, the focusing point requires a top hat profile.
On the other hand, diffractive beam shapers utilize diffraction, rather than refraction, to change the intensity distribution of the incident laser beam. Specific micro- and nanostructures are prepared on a substrate using an etching process to form diffractive elements. The effect and wavelength range of the diffractive element usually depends on the height and region spacing of the structure. Therefore, diffractive optical elements must be used within the designed wavelength range to avoid performance errors.
Diffractive beam shapers are more sensitive to divergence angle, alignment and beam position than refractive beam shapers. However, diffractive beam shapers have a particular advantage in space-constrained laser systems, as they usually consist of a single diffractive element instead of multiple refractive lenses, and can form both top hat beams and Airy spots.
Laser beam integrators, or homogenizers, are another type of beam shaping component. They consist of an array of small lenses that separate the incident light into smaller beams. A focusing lens then superimposes the smaller beams onto the target plane. The final output beam is the sum of the diffraction patterns produced by each small lens in the array. They can shape the incident Gaussian beam into a uniform top hat profile. However, these systems often encounter random irradiance fluctuations, resulting in an output beam profile that is not perfectly intensity uniform. Table 1 compares various beam shapers.
Top hat beams are suitable for a variety of laser systems where accuracy and efficiency are more important than cost. With refractive, diffractive, and other types of beam shapers currently on the market, laser system integrators have a variety of choices when selecting a beam shaper.





