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Lasers in the Manufacturing of LEDs

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Marco Mendes and Jeffrey P.Sercel, !%J.P. Sercel Associates Inc.%!

In today’s society, there is a continuous need for devices with lower energy consumption and higher efficiency. Light-emitting diodes (LEDs) are expected to see a 61 percent rise in worldwide demand in 2010, according to Barry Young of IMS Research, due in large part to the mobile handset. The market for large backlit LED TVs is rapidly expanding, and LEDs also are used in a large number of other applications, from projectors and flashlights to car tail- and headlights and general illumination. Solid-state white-light sources can be realized either by mixing different LEDs emitting red, green or blue light, or by using a phosphor material to convert monochromatic light from a blue or UV LED to broad-spectrum white light.

With the increase in LED production, manufacturers are looking for new process developments to optimize scribe width, speed and production throughput. New advances in laser liftoff (LLO) and laser wafer scribing for LEDs provide manufacturers with cost-effective industrial tools that are ready to meet increased demands.

High-brightness LEDs with vertical structure

Typically, blue/green LEDs are composed of a GaN film a few microns thick, grown epitaxially on a sapphire substrate. Some of the major costs of LED fabrication are the sapphire substrate itself and the scribe-and-break processes. For the traditional LED configuration, the sapphire is not removed, so both cathode and anode are installed on the same side of the GaN epitaxial (epi) layer (Figure 1).


Figure 1.
This diagram shows the traditional horizontal configuration for a blue LED. MQW = multiple quantum well.


There are several drawbacks to this configuration. For high-brightness LEDs, disadvantages include a high current density inside the material, current crowding, reduced reliability and shorter lifetimes. Also, there is significant light loss through the sapphire.

By using an LLO process, LED designers can create a vertical LED, which overcomes many of the limitations of the traditional horizontal configuration. Vertical configuration provides the possibility of pumping an LED with more current, eliminating the undesired current crowding and bottleneck inside the device and significantly increasing the maximum light output and efficiency of the LED (Figure 2).


Figure 2.
A model of a vertical configuration for a blue LED is shown.


The vertical LED structure requires removing the sapphire before attaching the electrical contacts. Excimer lasers have proved to be valuable tools for separating the sapphire and GaN thin film. LED laser liftoff dramatically reduces the time and cost of the LED fabrication process, enabling the manufacturer to grow GaN LED film devices on the sapphire wafer and to transfer the thin-film device to a heat sink electrical interconnect. The process allows for creation of freestanding GaN films and integration of GaN LEDs onto virtually any carrier substrate.

Laser liftoff principle

The basic concept behind UV LLO is to use the different absorptions of UV laser light in the epi material and the sapphire. With a high (9.9-eV) bandgap energy, sapphire is transparent to 248-nm KrF excimer laser radiation (5 eV), whereas GaN (approximately 3.3-eV bandgap) strongly absorbs the 248-nm laser light. As shown in Figure 3, the laser light travels through the sapphire and couples with the GaN, causing ablation at the GaN-sapphire interface. This creates a localized explosive shockwave and debonds the GaN from the sapphire at that location. The same principle applies to AlN on sapphire when using 193-nm ArF excimer laser radiation. Aluminum nitride with a bandgap of 6.3 eV can absorb the 6.4-eV ArF radiation, but AlN is still transparent to sapphire with a 9.9-eV bandgap.


Figure 3.
This is a schematic representation of laser liftoff at 248 nm.


To achieve successful liftoff, both beam homogeneity and wafer preparation are important. At J.P. Sercel Associates (JPSA) Inc., innovative and patented beam homogenization techniques with excimer lasers create a flattop beam on the wafer with uniform energy density distribution across an area as large as 5 x 5 mm.

Correct wafer preparation is crucial for successful LLO. It minimizes the residual stress from the high-temperature epi layer growth on sapphire, and it ensures adequate bonding between the epi layer and the carrier substrate to avoid fractures along the epi during liftoff. Figure 4 shows a typical liftoff result.


Figure 4.
This diagram illustrates single-pulse laser liftoff of GaN from sapphire at 248 nm (one pulse covers nine die).


Using LLO systems leads to high-speed, high-yield production at ambient temperature. Well-designed systems allow exposure of multiple die simultaneously with a single shot and permit accurate placement of each shot across the wafer using a novel “fire on the fly” technique.

Blue LED wafer scribing

There are traditional manufacturers who continue to supply horizontal-structure blue LEDs, and laser scribing is ideal for processing this wafer configuration. The extreme hardness of the sapphire causes significant problems for both saw dicing and diamond scribing, including low die yield, low throughput and high operating costs.

The use of UV diode-pumped solid-state (DPSS) lasers has proved to dramatically increase die yields and wafer throughput as compared to traditional diamond scribing methods, without appreciable loss of brightness in LED wafers. The short wavelength enhances optical absorption at both the GaN and sapphire layers, lowering the irradiance required for ablation while simultaneously allowing for reduced cut width.

Scribe width, speeds and production throughput are essential to keeping manufacturing costs low and wafer yields high. JPSA has developed a patented beam delivery system that allows for a very narrow kerf of 2.5 μm wide (Figure 5) and offers proprietary surface protection that minimizes debris. Moving the wafer under a tightly focused laser beam produces an extremely narrow V-shape cut; starting at the epi side and extending into the sapphire, it is typically 20 to 30 μm deep. After laser scribing, V-shape laser cuts act as stress concentrators for the process of breaking with standard cleaving equipment.


Figure 5.
Shown here is the kerf width in a GaN-on-sapphire wafer.



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The narrower kerf width generated by 266-nm front-side scribing increases the number of usable die produced per wafer, potentially boosting the entire fab operation.

An easy comparison involves a typical 2-in. blue LED wafer on sapphire, with 250 x 250-μm devices. Using traditional diamond scribing with typical 50-μm streets (300-μm die pitch), there will be approximately 22,500 die on the wafer. The typical breaking yield is 90 percent for traditional diamond scribing and results in 20,250 usable die per wafer.

By using UV laser scribing, the street width can be reduced to 20 μm (a 270-μm pitch), increasing the number of die on the wafer to approximately 27,800 (a 23 percent increase). With increased breaking yields, the method produces about 27,500 usable die – a 35 percent total increase in usable die per wafer.

Since 1996, JPSA has been using 266-nm DPSS lasers to scribe blue LED sapphire wafers from the GaN front side at speeds of 150 mm/s, leading to a throughput of about 15 wafers per hour (for standard 2-in.-diameter wafers with a die size of 350 x 350 μm). With its high throughput and minimal impact on LED performance, the process is tolerant of wafer warp and bow, delivering much faster scribing speeds than traditional mechanical methods.

Scribing silicon carbide

In addition to sapphire, silicon carbide can be used as an epitaxial growth substrate for thin blue LEDs. Ultraviolet DPSS lasers at 266 and 355 nm (4.6 and 3.5 eV, respectively) excel at scribing silicon carbide, which has a large bandgap of around 2.8 eV. Because of the high photon energy, enhanced coupling is achieved, allowing for high-speed scribing and easy breaking. Thick III-nitrides such as GaN and AlN also can be scribed using UV DPSS lasers. While the scribing speed for 200- to 400-μm-thick GaN or AlN is significantly reduced compared with the speed for thin epi films on sapphire or silicon carbide, the cut quality is excellent and allows for a clean breaking step.

For vertical high-power LEDs, LLO detaches the sapphire while the epi film remains bonded, typically to a high-conductivity carrier substrate such as copper, copper-tungsten, molybdenum or silicon. For wafer-based silicon, cutting depths of 100, 150 and 200 μm can be achieved at 300, 150 and 100 mm/s, respectively. Beam delivery techniques allow these scribing speeds/depths while requiring only limited laser power and, consequently, minimizing thermal affectation. Scribing of metal-based wafers is challenging because of high thermal conduction that typically leads to a weld back effect. In addition, a full cut often is required for separation because the material is extremely ductile. At JPSA, we have developed advanced techniques that allow for successful scribing of these substrates up to 200 μm thick and that could prove extremely important for the high-brightness LED industry.


Figure 6.
This graph represents UV absorption in LED sapphire.


Dual scribing capability

Back-side scribing by 355-nm DPSS lasers allows scribing from the sapphire side of the LED. Wafer alignment can be performed from the front or back side using multiple inspection cameras, which is important if the sapphire has a metallic reflective layer. Also, the epi is not directly exposed to laser radiation, which may minimize light loss. When compared to a 266-nm laser, the longer 355-nm wavelength leads to reduced absorption in the sapphire (Figure 6). As a consequence, higher power typically is required, which leads to wider kerfs and streets. Additionally, back-side scribing is applicable only for sapphire wafers <150 μm thick, while front-side scribing allows for thicker wafers that may be lapped down to the final thickness required for breaking after processing.


Figure 7.
Shown here is a cross section of a GaN wafer scribed from the sapphire (back) side by a 355-nm diode-pumped solid-state laser.


With continued research and development in back-side scribing, such as new laser absorption enhancement techniques, JPSA has achieved high-throughput back-side scribing at speeds of up to 150 mm/s with no debris or damage to the epi layer (Figure 7).

Wafer scribing III-V semiconductors

An alternative method for separating brittle compound semiconductor wafer materials in GaAs, InP and GaP wafers is scribing with UV DPSS lasers that rapidly process wafers with kerfs around 3 μm with no edge chipping in any of the III-V materials, making straight, accurate and clean cuts (Figure 8). Typically, wafers up to 250 μm thick are scribed at 300 mm/s, allowing for easy breaking (Figure 9). The III-IV wafers are expensive, so wafer real estate is valuable. The tighter, narrower and cleaner cuts achieved using UV lasers provide a better die count per wafer as well as higher yields, due to fewer damaged die than with conventional saw scribing methods.


Figure 8.
Clean, well-defined edges are highlighted in this scribed and expanded GaAs wafer.


Outlook

LED technology is advancing rapidly as it strives for higher efficiency and lower manufacturing costs. This “green” technology undoubtedly has a bright future; however, it also faces considerable challenges.

The current explosion of worldwide demand for LEDs requires the development of new laser processes and technologies to produce even higher quality, yield and throughput. In addition to the ongoing development of laser systems, new machining techniques and applications, improved beam delivery and optical systems, and an enhanced knowledge of the interactions between laser beams and materials will be required to sustain the progress of this green revolution.


Figure 9.
Pictured is GaP scribing at 300 mm/s for a 30-m cut, which is deep enough to break wafers up to about 250 μm thick.


Equipment engineers are challenged to build flexible tools. Options, such as the capability for automated cassette loading and unloading, edge detection and auto-focus systems, define the state-of-the-art laser scribing solution. Companies such as JPSA continue to explore the forefront of laser technology to meet the demands of the LED manufacturing market.

Meet the authors

Jeffrey P. Sercel is chairman and chief technology officer of JPSA in Manchester, N.H.; e-mail: [email protected]. Marco Mendes is director of JPSA’s applications lab; e-mail: [email protected].


Published: June 2010
Glossary
anode
The part of an electrical circuit in which the electrons leave (a cathode-ray tube) or enter (an electrolytic cell) a unit in the circuit.
bandgap
In semiconductor physics, the term bandgap refers to the energy range in a material where no electronic states are allowed. It represents the energy difference between the valence band, which is the highest range of energy levels occupied by electrons in their ground state, and the conduction band, which is the lowest range of unoccupied energy levels. The bandgap is a crucial parameter in understanding the electrical behavior of semiconductors and insulators. Here are the key components...
beam
1. A bundle of light rays that may be parallel, converging or diverging. 2. A concentrated, unidirectional stream of particles. 3. A concentrated, unidirectional flow of electromagnetic waves.
cathode
1. The negative electrode of a device in an electrical circuit. 2. The positive electrode of a primary cell or storage battery. 3. The primary source of electrons in an electron tube, serving as the filament in a directly heated electron tube, and in a coated metal configuration surrounding the heater in an indirectly heated one.
efficiency
As applied to a device or machine, the ratio of total power input to the usable power output of the device.
iii-v material
In semiconductor physics and materials science, the term "III-V materials" refers to compounds composed of elements from group III and group V of the periodic table. More specifically, these materials are compound semiconductors formed by combining elements from column III (boron, aluminum, gallium, indium, thallium) and column V (nitrogen, phosphorus, arsenic, antimony, bismuth). Common examples of III-V materials include: Gallium arsenide (GaAs): This compound semiconductor is widely used...
illumination
The general term for the application of light to a subject. It should not be used in place of the specific quantity illuminance.
optical system
A group of lenses, or any combination of lenses, mirrors and prisms, so constructed as to refract or reflect light to perform some definite optical function.
phosphor
A chemical substance that exhibits fluorescence when excited by ultraviolet radiation, x-rays or an electron beam. The amount of visible light is proportional to the amount of excitation energy. If the fluorescence decays slowly after the exciting source is removed, the substance is said to be phosphorescent.
scribing
The process of perforating a silicon or ceramic substrate with a series of tiny holes along which it will break. Nd:YAG or CO2 lasers are now routinely used.
ultraviolet
That invisible region of the spectrum just beyond the violet end of the visible region. Wavelengths range from 1 to 400 nm.
white light
Light perceived as achromatic, that is, without hue.
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