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Optoelectronic Thin-Film Characterization

Guray Tas, Priya Mukundhan, Timothy A. Johnson and Selezion A. Hambir, Rudolph Technologies, Flanders, N.J., Brian Howard, Spectra-Physics Semiconductor Lasers, Mountainview, Calif. -- Semiconductor International, 11/1/2001

At a Glance
The growing market for GaAs optoelectronic devices is requiring manufacturers to ramp up production and increase the standard wafer size from 100 to 150 nm. Once large-scale production begins, this transition will also require metrology tools to control the new processes in an effort to detect and prevent errors.
Sidebars:
PULSE Technology

Compound semiconductor technology is not new. Devices based on GaAs, the most mature of the III-V technologies, have been used for more than 30 years, mostly in aerospace and military applications. In these applications, their ability to operate at very high frequencies and power despite extreme temperatures and radiation was required. However, in the past 10 years or so, GaAs devices have come to be used in high-volume commercial applications such as cellular phones and other wireless applications, which require operating frequencies that are difficult to achieve with silicon-based devices. The growing market for GaAs optoelectronic devices is adding to this demand, and GaAs manufacturers are now ramping up production and increasing the standard wafer size from 100 to 150 mm.1

As with the current increase in silicon wafer size from 200 to 300 mm, the larger GaAs wafer presents both opportunities and risks. If the risks are properly managed, significant cost savings can be obtained through this more than doubling of the number of chips on a single wafer. Metrology tools will be required to control the new processes in 150 mm GaAs manufacturing. Once large-scale production begins, metrology will also be required to provide early detection of costly process deviations and misprocessing. Because a 150 mm GaAs wafer, after epitaxial growth of the device structure, can cost about 60 times more than an equivalent Si wafer,2 reducing or eliminating test wafers and detecting or preventing errors will be critical for manufacturers that successfully transition to 150 mm GaAs production.

One of the fastest growing segments of the optoelectronics market is vertical-cavity, surface-emitting lasers (VCSELs). These devices convert electronic signals to optical signals by producing a narrow laser beam that can be switched on and off electrically, and can easily be coupled to optical fibers with an efficiency of up to 80%.3 They also have many other advantages over their edge-emitting competition, including smaller size, greater efficiency, and a short cavity that allows the beam to be turned on and off without an external modulator. Finally, unlike edge-emitting lasers, VCSELs can be tested while still on the wafer, allowing bad devices to be eliminated before costly packaging.

The market for VCSELs is predicted to triple over the next three years, reaching 3.4 billion by 2004. GaAs-based VCSELs operating at 850 nm all but replaced standard transmitters in short-haul local area networks within the first two years of commercial availability.4 InP-based VCSELs are now on the cutting edge of technology, but will have the capability to operate at 1310 and 1550 nm, which are the low-loss transmission windows for optical fibers. Once commercially available, these devices are expected to be hugely successful in the marketplace for mid- and long-range transmission applications. For manufacturers to successfully compete in this market, they will need metrology tools that can characterize the GaAs- or InP-based materials accurately and reproducibly.

High-volume optoelectronic production will require new metrology solutions. The non-contact, non-destructive picosecond ultrasonic laser sonar (PULSE) thin-film measurement technology (see "PULSE Technology," this page), currently being used to effectively characterize and monitor copper and other opaque films in silicon-based technology, also has the characteristics needed for the optoelectronics market. All measurements shown in this article were taken with Rudolph Technologies'Meta PULSE-II metrology system. While a variety of applications are possible, this paper will concentrate on these critical applications: GaAs metalization and VCSELs.

GaAs metalization

Metalization is the foundation of the process that establishes an electrical contact with each device terminal and connects the individual devices by means of metal wires to form circuits. Although metalization schemes in silicon-based and compound semiconductor devices display some similarities, GaAs metalization processing is significantly different. GaAs forms no stable oxides that can be used for isolation. In addition, As dissociates from the GaAs substrate at temperatures above 400°C, restricting the thermal budget. This and other processing considerations require that GaAs metalization be formed at temperatures below 100°C, precluding many of the higher-temperature processes common in silicon-based devices. The effect of these complications is that the advantages GaAs materials offer in terms of higher electron mobility and lower power consumption may be lost due to poor metalization. Also, poor metalization can increase resistance, resulting in slow device speed and degraded performance.

GaAs metalization uses materials seldom encountered in silicon-based manufacturing. Aluminum, the old standard for silicon-based contacts, cannot be used because it readily forms eutectics such as AlGaAs.2 Gold (Au), despite its expense, is the most commonly used contact metal. Au is an excellent conductor, has a high resistance to oxidation and, being a noble metal, reacts with few other materials. Other common interconnect materials compatible with III-V semiconductors include platinum (Pt), nickel (Ni) and germanium (Ge).

Perhaps of more interest is metrology for multilayer metal stacks. In the new 150 mm fabs, these stacks may be deposited by cluster tools that lay down several layers in the single process tool. These cluster tools not only reduce the total time required for processing, but also reduce the possibility of interlayer contamination and the chances of breaking the brittle wafers. However, cluster tool processing requires a metrology tool that can simultaneously measure the multiple layers of the contact film stack after deposition.

Ni/Ge/Au STACK THICKNESS
 
1. Measurement from a Ni/Ge/Au stack on GaAs. The thickness of all three layers was simultaneously determined as 177 Å of Ni, 142 Å of Ge, and 505 Å of Au. The graph on the left shows the acoustic signal (black) and the best fit simulation (red).

When growing epitaxial layers of p-type or n-type GaAs, only the p-type can generally be grown with sufficient doping. When producing contacts to p-type, Au is the primary conductor, with a diffusion barrier such as Pt and an adhesion promoter such as Ti or TiW. However, forming a direct ohmic contact to n-type materials requires additional processing. A Ni/Ge/Au stack is commonly deposited and a short anneal is then performed to raise the dopant level and form the contact. Measurement results for a sample Ni/Ge/Au stack are shown in Figure 1. All three layers were measured simultaneously, and the measured results for the layers were 177/142/505 Å for the Ni/Ge/Au, respectively. Measurements such as this can be used to monitor the n-type metalization process and to check for process deviations that might cause insufficient doping and the possible failure of the completed devices.

VCSELs

The processes involved in VCSEL manufacturing are complex. A VCSEL's active region is sandwiched between highly reflective mirrors called distributed Bragg reflectors. These mirrors are comprised of alternating layers of two materials having different indices of refraction to form a stack having multiple opaque layers grown using either metal-organic chemical vapor deposition (MOCVD) or molecular beam epitaxy (MBE). The slightly different indices of the individual layers reflect a very narrow range of wavelengths back into the cavity, stimulating laser emission at only one specific wavelength. To do this, it is important to deposit films in both the active region and the mirror structures within tightly controlled process ranges. The thickness and uniformity of the Bragg reflectors is critical to ensure that their peak reflectivity occurs at the lasing wavelength.

 
2. A 43-point uniformity map of an InGaAs layer on an InP substrate with a 0.5 mm edge exclusion.

A key factor to consider when producing VCSELs is the planarity of the layers. Non-planar layers can cause improper alignment of the mirrors, resulting in defective devices. Therefore, the deposition process must be carefully monitored for uniformity across the wafer. The newest processes being developed for VCSELs involve InP wafers that can be used to produce 1310 or 1550 nm devices. A thick layer of InGaAs is commonly used as a base for the mirrors and the active region that will be deposited over it. A uniformity map of such a layer on an InP substrate is shown in Figure 2. The 43-point map shows the film is thinnest nearest the notch and gets progressively thicker as you move away from the notch. This information was acquired in <5 min and, because the measurement was non-destructive, the wafer could be sent on for further processing. Picosecond sonar metrology can also provide fast, non-destructive, on-product process control metrology of other steps in the VCSEL manufacturing process.

Conclusion

Picosecond sonar has been shown to have the ability to characterize and monitor certain processes in compound semiconductors. As the optoelectronic market grows, high-volume manufacturing is becoming the norm, and competition will demand ever tighter process control to maintain high yields and profits. In this environment, metrology is critical to success. Picosecond sonar is unique among metrology techniques because it is able to non-destructively measure opaque films and film stacks on product wafers.


Author Information
Guray Tas is manager of advanced applications at Rudolph Technologies . He has a Ph.D. in condensed matter physics from Brown University.
Priya Mukundhan, advanced applications scientist at Rudolph Technologies, is in charge of research and development of new applications for current metrology products and new metrology techniques. She has a Ph.D. in materials science and engineering from Stevens Institute of Technology.
Timothy A. Johnson, advanced applications scientist at Rudolph Technologies, is in charge of research and development of new applications for current metrology products and new metrology techniques. He has a Ph.D. and M.Sc. in physics from Brown University and a B.S. in physics from the College of William and Mary.
Selezion A. Hambir, advanced applications scientist at Rudolph Technologies, is in charge of research and development of new applications for current metrology products and new metrology techniques. He has a Ph.D. in analytical chemistry from Michigan State University.
Brian Howard, thin-film process engineer at Spectra-Physics Semiconductor Lasers , has 10 years of semiconductor processing experience in thin-film deposition. His areas of interest include thin-film deposition, defect identification/reduction, RTP and yield improvement. He has a B.S. in physics from the University of Arizona.


References
  1. M.R. Wilson, "Riding the Wireless Wave with 150-mm GaAs Manufacturing," Compound Semiconductor, September/October 2000.
  2. A. Bavin, "Cluster Tool Sputtering for Compound Semiconductors," Solid State Technology, July 2001, p. 145.
  3. "The Basics of Compound (vs. Silicon) Semiconductors," Compound Semi Online, April 4, 2001.
  4. "VCSELs vs. the Rest," Light Reading.com, Nov. 27, 2000.
 

PULSE Technology

In this technique, a picosecond laser flash generated by a pump laser induces an ultrahigh-frequency sound wave that travels from the top surface of the opaque structure down through the film stack. Some sound reflects from each interface, returning to the top surface as an echo. A film stack consisting of multiple layers produces a train of echoes, one from each layer, with the thickness of each film indicated by the time it takes the sound wave to transit through that layer. The time delay between echoes from interfaces of the multiple layers allows simultaneous measurements of underlying layers. The echoes are detected by a probe laser that senses changes in the optical reflectivity of the top surface that occur when the echo returns to the surface. Films with thickness ranging from 30 Å to 3 µm or more can be measured in this way. This capability has been demonstrated not only on blanket films, but also on a variety of line-array patterns. The measurement spot size is 15 µm in diameter, allowing measurements on test sites as small as 40 × 40 µm. For typical applications, 1 σ repeatability is 1% or better.

Picosecond sonar technology is best known for measuring metal films, but in many applications, measurement of transparent films over an opaque layer is also possible. In this case, the underlying opaque layer absorbs the light from the pump laser and generates the sound wave. The probe laser beam then detects the sound wave as it moves upward through the transparent film. The result is an oscillatory signal with a phase change when the sound wave inverts at the surface. The timing of the phase change indicates the transparent film's thickness. MetaPULSE-II can also be equipped with a reflectometer that can measure the thickness and optical properties of transparent films.

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