Power Electronics

As the technological transformation of our society continues to take shape, one category of products playing an immense role in this transformation is power electronics. These are devices which convert, control and condition electrical power. Some examples of power electronics devices are diodes, rectifiers, inverters, converters, choppers and transistors. Since the dawn of electronic devices, silicon has been the predominant semiconductor material, and it continues to dominate power electronics devices. However, silicon-based power electronics have limitations that may prevent them from enabling more widespread technological transformations of our society.

Expanding Power Electronics Beyond Silicon

One development requiring higher performing power electronics is the growing adoption of electric vehicles (EVs) and expectations of longer driving ranges and faster charging times. Another trend calling for more advanced power electronics is the shift towards renewable energy sources which rely on efficient power conversion and reduced power losses. Additionally, further advancements in consumer electronics and telecom demand power electronics that can manage higher power densities and faster switching speeds while providing better thermal management.

Silicon-based power electronics are able to serve a portion of the applications described above, but they are mostly suitable for applications such as home appliances, power tools, and less demanding data center functions—for these types of applications, lower to mid-range switching frequencies are suitable, and cost often takes precedence over performance or form factor. But beyond mid-range switching frequencies, silicon-based power electronics fall short due to the inherent bandgap of silicon. Hence, semiconductors with wider bandgaps than silicon are necessary because they can provide higher power, switching frequency, operating temperature, switching voltages and better efficiency. Two materials in particular with wide bandgaps have already proven their worth for power electronics: silicon carbide (SiC) and gallium nitride (GaN). The bandgaps of SiC and GaN are over two and three times greater in electron volts (eV) than silicon's.

SiC-based power electronics are ideal for high-power/high-switching frequency applications. For instance, the potential for EVs with SiC-based power electronics includes longer driving ranges, faster charging times, and lighter vehicle weight. Also, more compact and more efficient energy storage systems may be possible with SiC. While GaN is limited to medium-power applications, it offers the highest operating frequency among these technologies. As such, GaN-based power electronics opens up many new possibilities in consumer electronics and telecom, such as ubiquitous use of wireless charging and faster communication speeds.

It is also important to recognize that all of these technologies overlap in roughly the mid-power/mid-frequency space, creating a "competing zone" amongst them. In this arena, silicon may be preferred when cost is the primary concern. But when higher performance, better efficiency, or smaller-sized products are desired, SiC or GaN should be considered.

SiC and GaN Manufacturing Challenges

Manufacturing of traditional silicon-based power electronics is well known and established, but SiC- and GaN-based power electronics presents new and more difficult challenges.

SiC as a raw material is much more costly than silicon is, and finished devices are about three times more expensive. SiC wafers are more brittle, thinner and smaller than silicon wafers are, so handling SiC wafers during the manufacturing process is more delicate, complex, and expensive.

GaN wafers are even more brittle, thinner and smaller than SiC wafers, so handling GaN wafers is even more complicated and costly than handling SiC wafers. Interestingly, however, GaN-based products can be cheaper than those made of silicon for equivalent power conversion specifications—this is due to GaN's higher efficiency, lower operating costs and smaller footprint.

While SiC and GaN wafer fabs share many steps used in silicon wafer manufacturing, there are some notable differences. For example, SiC and GaN wafer ingot slicing is typically performed by lasers instead of mechanical diamond saws to improve wafer yields and lower costs by reducing material waste and scrap. Also, an existing silicon wafer processing line cannot be used as is on SiC or GaN wafers—one reason is that wafer handling equipment developed for silicon my not be appropriate for SiC or GaN wafers.

The good news is that MKS has decades of experience with silicon wafer processing from the front-end to back-end and can work with you to develop and build the best solution for your SiC or GaN needs.

  Si (base case) SiC GaN
Device Cost $ $$$ $
Typical Maximum Wafer Diameter 300 mm 200 mm 150 mm
Typical Wafer Thickness 0.4-0.5 mm 0.35-0.5 mm 0.25-0.3 mm
Manufacturing Complexity ⚙⚙ ⚙⚙⚙

The MKS Advantage for SiC and GaN Manufacturing

As a leader in silicon wafer processing from the front-end to back-end for decades, MKS has a deep understanding of the challenges faced in designing and manufacturing power electronics. We've turned this knowledge into unique product features that provide an advantage when used for SiC- and GaN-based power electronics. Some of these features are described here.

Lasers

Lasers Provide Advantages Over Traditional Processes

SiC and GaN Processing Applications:

  • Ingot slicing
  • Scribing
  • Grooving
  • Dicing
  • Marking
Figure 1. Spectra-Physics laser scribing a GaN wafer

Lasers are superior to traditional mechanical methods such as blades and drills in applications including ingot slicing, scribing, grooving, dicing and marking. For example, the time-consuming process of slicing a SiC ingot with a mechanical diamond saw can waste up to 75% of the material. Moreover, as SiC is a significantly harder material than silicon is, a blade will wear faster, leading to increased replacement costs and more frequent downtime. By comparison, laser ingot slicing for SiC and GaN results in minimal material loss, and there is no tool wear. And by employing the appropriate laser and slicing methodology, laser ingot slicing can be considerably faster than mechanical slicing.

MKS' lasers are very high-precision devices, so they can cut and drill accurately and repeatably on the order of microns with ease, which may not be the case with mechanical tools. SiC and GaN wafers are already more brittle than silicon and must be handled more delicately, and as SiC and GaN devices become more complex, they might be even more difficult to produce solely through mechanical means. In addition to the high precision, lasers also offer more flexible patterns for cutting and drilling, which further enables more complex designs and higher performing devices to be made.

Another important advantage that lasers present over traditional processes is the quality of their results. With slicing, scribing, grooving and dicing, lasers produce fewer burrs and less damage to the surrounding areas than mechanical cuts do. This results in higher manufacturing yields, as less of the material is wasted. Additionally, laser operations result in fewer latent defects and cracks compared to mechanical operations, which can lead to better quality and reliability of the product in the field, as not all of these types of issues are discovered before products leave the factory. And like laser ingot slicing, laser scribing, grooving, dicing and marking are contact-free operations, so there is no tool wear, and the replacement downtime is exceedingly infrequent compared to mechanical methods.

Taken all together, SiC and GaN processing with lasers will enable the production of devices that are mainstream enough to complement and compete with silicon-based electronics.

Laser Advantages:

  • High precision
  • Flexible and complex patterns
  • Fewer burrs
  • Less surrounding damage
  • Fewer latent defects and cracks
  • Contact-free operation

Spectra-Physics Lasers for Power Electronics Processing Selection Guide

For marking, the Talon UV nanosecond laser works well, as does the Explorer One UV and green nanosecond lasers. And even though there’s no check-mark in the table for it, Talon Ace can also perform marking, although that probably wouldn’t be its primary application. Ingot slicing can be performed with the IR version of our IceFyre picosecond and IceFyre FS femtosecond IR lasers, or with the green version of the Talon nansecond laser. Scribing is a process to create deep cuts in the substrate material – like an SiC or GaN wafer – in preparation for dicing. We think the best choice is a UV wavelength, so Talon Ace, Talon, IceFyre and IceFyre FS are great choices. Additionally, the Spirit green femtosecond laser and the IR version of the IceFyre FS are also well suited for scribing. Grooving is done to make shallow cuts to precise target depth and desired features. Examples include v-grooves and also possibly removal of thin film. Here again, we think the best choice is a UV wavelength. Other lasers that can perform grooving well are the green versions of the IceFyre and Spirit, and also the IR version of the IceFyre FS.

  Talon® Ace™ (ns) Talon (ns) IceFyre® (ps) IceFyre FS (fs) Spirit® (fs) Explorer® One™ (ns)
  UV UV Green UV Green IR UV IR Green UV Green
Marking                
Ingot Slicing                
Scribing          
Grooving        
Dicing      
Via Hole Drilling              

Motion Control

Wafer positioning performance for processes including lithography, inspection and dicing can be very challenging, often with sub-micron and even nanometer scale accuracy and repeatability required. Moreover, this very precise level of operation must be delivered quickly, with speeds up to 1 meter/sec, to maximize throughput.

To address the wafer positioning demands of the semiconductor manufacturing industry, MKS developed the Newport DynamYX® series positioner, a high-throughput, high-accuracy solution based on air bearing and linear motor technology. With over 20 years of field-proven success in more than 1,000 systems installed worldwide, DynamYX provides the highest level of commercially available positioning performance. Additionally, MKS offers the Newport HybrYX® series positioner, a hybrid air and mechanical bearings system with linear motors, that also delivers high throughput and accuracy.

Figure 2. DynamYX GT Air Bearing Wafer Positioning Stage

All DynamYX and HybrYX systems are custom-designed, so the techniques and solutions developed for silicon processing can be adapted and applied to SiC and GaN processing.

Wafer and Reticle Positioners Selection Guide

Below is a selection guide for the various applications and our recommended motion platforms. Please keep in mind that this is only a guide, and we’d love to discuss your application and requirements in detail with you so we can help provide the best solution for you. For wafer inspection, our DynamYX systems are the best-in-class, and HybrYX is also a good value. The IDL and XM Series linear stages can also be used depending on your requirements. For lithography, reticle inspection and repair, and mask writing, DynamYX is also the best. For wafer dicing, HybrYX is ideal because of its outstanding price-to-performance value, but you can also consider the DynamYX and the IDL stages.

  DynamYX® HybrYX® IDL XM
Wafer Inspection ★★★ ★★
Lithography ★★★      
Wafer Dicing ★★ ★★★ ★★  
Reticle Inspection & Repair ★★★      
Mask Writing ★★★      

Optics

There are many factors to consider when selecting optics for power electronics applications. Here are the criteria to start with.

First is the wavelength required. For the laser, it’s likely going to be 355 nanometers UV, and sometimes 532 nanometers green or 1064 nanometers IR. There are broadband and laser line optics available, but when you know specifically which wavelength you’ll have, we recommend using laser line optics when possible because they’re optimized for a specific wavelength and will perform better than a broadband optic.

The next thing to consider is an optic’s LIDT, or how much laser power or energy the optic can withstand before it gets damaged, and if that will work in your system. You’ll want to use not only substrates that are known for high laser damage thresholds but also coatings that are properly tested for high damage thresholds as well.

You should then look at how well it reflects light if it’s a mirror, or how well it transmits light if it’s a lens. And for other types of optics like a beamsplitter or waveplate, you’ll want to evaluate how well light passes through them as well. The less light you lose as a result of the optic itself, the easier it will be for you to manage the light throughout the rest of your system, and the better your results will be.

Lastly, optics are available in all different sizes and shapes depending on your requirements.

High-Energy Laser Mirrors

High-energy laser mirrors optimized for 355, 532 and 1064 nm offer very high reflectivity and damage thresholds.

  High-Energy Laser Mirrors
Wavelength 355 nm 532 nm 1064 nm
CW Damage Threshold 3 kW/cm2
Pulsed Damage Threshold 3.5 J/cm2 @ 10 ns, 20 Hz 10 J/cm2 @ 20 ns, 20 Hz 45 J/cm2 @ 10 ns, 20 Hz
Reflectivity Rs > 99.7%
Rp > 99%
Diameter 1 and 2 inch
Substrate Material UV Grade Fused Silica
Angle of Incidence 45°

High-Energy Plano-Convex Lenses

High-energy lenses optimized for 355, 532 and 1064 nm offer very high transmission and damage thresholds.

  High-Energy Spherical Lenses
Wavelength 355 nm 532 nm 1064 nm
Pulsed Damage Threshold 15 J/cm2 @ 20 ns, 10 Hz
Average Reflectivity per Surface < 0.25%
Diameter 1 inch
Substrate Material High Purity Fused Silica

Nanotexture Surface Lenses

Highest laser damage resistance and lowest reflection loss.

  Nanostructure Surface Fused Silica Plano-Convex Lenses
Wavelength 250 to 550 nm or 500 to 1100 nm
CW Damage Threshold 15 MW/cm2
Pulsed Damage Threshold 35 J/cm2 @ 10 ns, 1064 nm
Reflection Loss 0.1%
Diameter 0.5 in.
Shapes Plano-Convex or Plano-Concave
Substrate Material High Purity Fused Silica
Other Features Sub-λ AR nanotextures etched directly into surface (no thin film coatings)

Beam Analysis

Even with the advantages that lasers have over traditional tools, laser systems can still degrade over time. Some causes of degradation include thermal effects on a laser system's internal components, vibrations or shock, and debris near the processing site. These issues could affect laser performance in a number of ways. First, output power may be reduced, causing the laser to be less efficient. Another problem that may be caused is a change in the focus or other profile of the beam, which may lead to a cut or drill to be off target, too deep, low quality or possibly damaging to another part of the material.

Therefore, to ensure the highest quality of manufacturing SiC and GaN wafers and to minimize the possibility of production down-time, it is crucial to monitor the laser beam frequently with appropriate instruments—like Ophir® power sensors, power meters and beam profilers—that can characterize the laser while handling its maximum output power level.

Figure 3. Beam profile displayed and analyzed with Ophir BeamGage® beam profiling software

Laser Beam Profilers

  SP932U  
Spectral Range 190-1100 nm (Optimized for NIR & Nd:YAG) SP932U
Damage Threshold 50 W/cm2
1 J/cm2, <100 ns pulse width
Beam Sizes 34.5 µm – 5.3 mm
Pixels 2048 x 1536 Effective Pixels
3.45 µm Pixel Size
PC Interface USB 3.0
Other Features BeamGage® software included
UltraCal™ correction algorithm
Measures cross-sectional intensity
72 dB true dynamic resolution
24 Hz frame rate in 12-bit mode
A variety of attenuators available

Laser Power Sensors

MKS offers a comprehensive portfolio of Ophir® laser thermal power sensors, several of which can measure the optical output power of short- and ultrashort-pulsed lasers such as IceFyre, Talon, Talon Ace and Quasar. These sensors have a very high damage threshold to withstand the high optical peak power delivered by each pulse. Ophir sensors and meters meet the ISO/IEC 17025 standard for calibrated devices.

  F150(200)A-CM-16 30(150)A-SV-17 F80(120)A-CM-17  
Spectral Range 0.248-9.4 µm 0.19-11 µm 0.248-9.4 µm laser-power-energy-meters
Power Range 300 mW - 200 W 100 mW - 150 W 100 mW - 120 W
Energy Range 50 mJ – 200 J 50 mJ – 300 J 50 mJ – 200 J
Max Avg Power Density 35 kW/cm2 60 kW/cm2 35 kW/cm2
Max Energy Density (2 msec) 45 J/cm2 50 J/cm2 45 J/cm2
Aperture Ø16 mm Ø17 mm Ø17.5 mm
Response Time 3 sec 1.7 sec 2 sec
Other Features Not water-cooled