Close

Search

Search Menu
Photonics Media Photonics Buyers' Guide Photonics EDU Photonics Spectra BioPhotonics EuroPhotonics Industrial Photonics Photonics Showcase Photonics ProdSpec Photonics Handbook
More News
SPECIAL ANNOUNCEMENT
2016 Photonics Buyers' Guide Clearance! – Use Coupon Code FC16 to save 60%!
share
Email Facebook Twitter Google+ LinkedIn Comments

Diode-Pumped Solid-State UV Lasers Improve LED Sapphire Wafer Scribing

Photonics Spectra
Oct 2010
Rajesh S. Patel, Ashwini Tamhankar and Tim Edwards, Spectra-Physics, a Division of Newport Corp.

The green movement, energy conservation efforts and global warming headlines have made the world aware of the need for more energy-efficient lighting alternatives. The range of applications for high-brightness LEDs continues to expand. Laser scribing of wafers used to make LEDs is helping lead the way to great advancements in the area of optoelectronic devices used in LCD backlighting for cell phones, televisions and touch-screen displays. Most exciting is the advent of white LEDs for illumination.

Currently, about 12 billion electric lights on the planet use incandescent bulbs, or about 40,000 trillion lumen hours per year. This takes a lot of fuel – the equivalent of nearly a billion tons of coal annually. Lighting using white LEDs offers the promise of greatly reduced energy consumption through greatly improved efficiency.

It is quite an undertaking to replace every lightbulb on the planet. The rapidly growing demand for LED lighting has pushed manufacturers to constantly improve the production process for brighter, more efficient and less expensive devices. Laser scribing has rapidly become the industry standard for producing wafers for high-brightness LEDs.

Scribing LED wafers using lasers improves yield by creating much narrower scribe lines than traditional mechanical scribing. Laser scribing is a noncontact process that allows better scribing of hard or brittle materials while reducing micro-cracking and damage to the wafer substrate. This allows the LED devices to be much more closely spaced, improving both yield and throughput, and it increases the long-term reliability of the LED devices. The wider process tolerance of lasers and the elimination of blade wear and breakage translate to a more robust manufacturing process at a lower cost.

Because typically there might be more than 20,000 discrete LED devices on a single 2-in. wafer, cut width critically affects yield. Reducing microcracking during the die separation process has also been shown to improve the long-term reliability of the LEDs. Yield is improved with laser scribing by reducing wafer breakage. The speed of the laser scribe-and-break process is also much faster than traditional mechanical scribing.

LED devices, such as InGaN blue, green and white LEDs, are fabricated on single crystal sapphire (Al2O3) substrates that have excellent thermal conductivity but are quite hard. Because there are usually several thousand LED devices on a single wafer, the street widths available between dies are very narrow, typically 20 to 50 µm. Traditional mechanical and diamond saws are often too wide, with kerf widths up to 250 µm, and they can produce undesirable effects such as chipping, microcracking and delamination, negatively affecting yield and throughput.

Laser scribing LED wafers is a challenge since the material is relatively transparent through the visible portion of the electromagnetic spectrum. GaN is transparent below 365 nm, and sapphire is semitransparent above 177 nm. Thus frequency-tripled (355 nm) and frequency-quadrupled (266 nm) diode-pumped solid-state (DPSS) Q-switched lasers are the best choice for LED scribing.

When scribing LED substrates, the desirable UV Q-switched DPSS lasers have short pulses and high repetition rates and can be optimized at fluences that reduce microcracking and damage to the wafer substrate. Short-pulse-width and high-peak-power lasers result in cleaner scribing, less displaced material and less thermal damage to the substrate.

These lasers can create very narrow scribe lines that allow the wafers to then be broken into individual devices. The laser is tightly focused on the wafer substrate, ablating material to create a narrow scribe line between the active devices. Typically, a scribe depth of one-third to one-half the substrate thickness is required to obtain a clean break. The need for both narrow and deep scribe lines at a high speed can be met using short pulse widths, high beam quality, high peak powers and high repetition rates such as those found in DPSS lasers.

For 266-nm laser-based processes, typically the front side of the sapphire wafer is irradiated. In contrast, back-side scribing is the preferred technique while using a 355-nm laser to scribe sapphire wafers <150 µm thick. Scribing from the back side of the device has been shown to have the advantage of reducing impact on LED performance. Among the research conducted for sapphire scribing application with a 355-nm wavelength, limited information is available in the literature about the effect of laser parameters on the laser scribing process. Here we characterize the effect of 355-nm Q-switched DPSS laser parameters such as fluence, pulse width and repetition rate on the laser scribing process by measuring sapphire wafer cutting depth and scribe kerf width.

The samples used in this study were blank single-crystal sapphire wafers measuring 2 in. in diameter and approximately 400 µm thick, with diffused and polished sides. All of the laser processing was performed at room temperature on the diffused back side of the wafer with no assist gas. The lasers used were the Spectra-Physics Tristar 355-3 with >3 W at 50 kHz and the Pulseo 355-10 with >10 W at 90 kHz. Both had <23-ns pulse durations and good beam quality.


Figure 1.
A top-view microscopy image reveals scribes on a sapphire wafer.


To determine the location of the “processing focal plane,” test scribes were generated at various focal positions. These scribes were processed using slow scan speeds to obtain more than 80 percent spatial pulse overlap. Figure 1 shows a top view of some example scribes. After the material was cleaved, an optical microscope was used to measure the cut depths. Figure 2 is a cross-sectional edge view demonstrating scribe depths at various focal positions. The “processing focal plane” corresponding to the deepest scribe was selected for conducting the studies. With the theoretical spot size of 2.5 µm, groove widths achieved at the “processing focal plane” during all of the experiments were 5 to 7 µm.


Figure 2.
This cross-sectional edge view shows scribe depths corresponding to various focal planes.


For the sapphire wafers, an optical fluence between 30 and 400 J/cm2 was determined to be a good process window. If the applied laser fluence was below the ablation threshold, no material was removed. At high fluence levels, however, excess energy was wasted in heating the material. This material heating can cause unwanted debris, cracking, melting and stress in the surrounding material, or what is commonly referred to as “HAZ” (heat-affected zone).

Material removal thresholds are dependent also upon pulse duration. Shorter-pulse-width lasers tend to have lower thresholds for material removal than longer-pulse-width lasers. Figure 3 shows scribe depth at various fluence values corresponding to 18- and 42-ns pulse widths. The data plot indicates that a clear processing advantage exists with shorter pulse duration (18 ns) over longer pulse duration (42 ns). Extrapolation of these logarithmic curves toward lower fluence values clearly demonstrates that the material removal threshold with 18-ns pulse duration is lower than that with 42-ns pulse duration. In addition, in the low fluence regime close to 500 J/cm2, an 18-ns pulse duration results in deeper scribes compared with those for 42-ns pulse duration. The data in Figure 3 indicates that with a short-pulse-width laser, deeper scribes are achieved at low fluence levels, whereas with a longer-pulse-width laser, more energy is needed to achieve the same depth.


Figure 3.
A graph of scribe depth versus fluence charts the advantage of short pulse widths.


The benefit of operating lasers at high repetition rates to increase throughput in laser processing is also well-known and is shown in Figure 4, where scribe depth increases with increasing repetition rate. At the higher repetition rates, the time between pulses is shorter and, thus, the thermal energy is deposited in the material at a rate faster than energy is dispersed from the focal volume by thermal diffusion. This facilitates increased heat accumulation at the focal volume, resulting in localized heating and melting of the material, which leads to increased material removal. Hence, for sapphire scribing, it is beneficial to operate the laser at a low energy per pulse and at high repetition rates to take full advantage of available laser energy for material removal.


Figure 4.
A plot of scribe depth versus repetition rate demonstrates the advantage of a high repetition rate.


With the significant efficiency gain offered by LEDs over traditional incandescent lighting, along with the movement toward energy conservation, the demand for LEDs has exploded. And DPSS 355-nm Q-switched lasers provide an effective tool for robust high-yield scribe-and-break wafer singulation processing for high-throughput LED manufacturing. The DPSS UV lasers offer the shorter pulse width, higher repetition rate and higher power needed to produce narrower and cleaner scribe lines at higher speeds.

Meet the authors


All three authors work for Spectra-Physics, a division of Newport Corp., in Santa Clara, Calif. Rajesh Patel is applications lab senior manager; e-mail: raj.patel@newport.com. Ashwini Tamhankar is senior laser applications engineer; e-mail: ashwini.tamhankar@newport. com. Tim Edwards is a senior marketing manager; e-mail: tim.edwards@newport.com.


GLOSSARY
backlighting
The forming of a clear silhouette of an object by placing a light source behind it. Used in machine vision when surface features of an object are not important.
electromagnetic spectrum
The total range of wavelengths, extending from the shortest to the longest wavelength or conversely, that can be generated physically. This range of electromagnetic wavelengths extends practically from zero to infinity and includes the visible portion of the spectrum known as light.
illumination
The general term for the application of light to a subject. It should not be used in place of the specific quantity illuminance.
optoelectronics
A sub-field of photonics that pertains to an electronic device that responds to optical power, emits or modifies optical radiation, or utilizes optical radiation for its internal operation. Any device that functions as an electrical-to-optical or optical-to-electrical transducer. Electro-optic often is used erroneously as a synonym.
transparent
Capable of transmitting light with little absorption and no appreciable scattering or diffusion.
wafer
A cross-sectional slice cut from an ingot of either single-crystal, fused, polycrystalline or amorphous material that has refined surfaces either lapped or polished. Wafers are used either as substrates for electronic device manufacturing or as optics. Typically, they are made of silicon, quartz, gallium arsenide or indium phosphide.
Comments
Terms & Conditions Privacy Policy About Us Contact Us
back to top

Facebook Twitter Instagram LinkedIn YouTube RSS
©2016 Photonics Media
x Subscribe to Photonics Spectra magazine - FREE!