VCSELs turn to high-speed transmission

Feb. 1, 2001
Lower costs and higher modulation rates have made VCSELs the preferred source for many local area networks. Now developers are hoping to push VCSEL technology all the way to the metro network.

The technology for vertical-cavity surface-emitting lasers is growing explosively. First demonstrated only about a decade ago, the VCSEL is a major shift in semiconductor-laser technology. Instead of a laser cavity in the plane of the junction layer, the VCSEL has resonator mirrors above and below the junction layer, so light oscillates in a "vertical cavity" perpendicular to the junction. This gives VCSELs properties quite different from conventional edge-emitters.

So far, the biggest applications of VCSELs have been in high-speed local-area networks such as Gigabit Ethernet, where 850-nm sources are used with multimode fibers. However, fiber dispersion and loss at 850 nm limit transmission rates and distances. Emerging higher-capacity networks like 10-Gigabit Ethernet will require longer-wavelength sources for most interbuilding applications. That poses some tough challenges, but developers are making progress and looking to push VCSELs all the way to the metro network.

VCSEL basics

Light emission in all semiconductor diode-lasers occurs at the junction layer, where current carriers from the n- and p-doped regions of the device recombine to produce stimulated emission. VCSELs differ from edge emitters in the structure of the resonant cavity and the way light energy is coupled out of the laser.

The mirrors above and below the junction layer are formed by depositing a series of thin layers of semiconductor material, with two alternating compositions that differ in refractive index. These function as distributed Bragg reflectors, with the refractive-index differential causing them to reflect wavelengths selected by the layer spacing back into the laser cavity. One is a total reflector, and the other transmits a small fraction of the incident light—around 1%—which forms the laser beam. The figure shows a common type of device in which the beam emerges through an n-doped substrate.

Other VCSEL structures differ in detail, but retain the idea of a pair of highly reflective mirrors that provide strong reflection back into the laser cavity. In this sense the cavity resembles that of a low-gain helium-neon gas laser because VCSELs have low gain per pass. Semiconductor lasers have much higher gain per unit length, but the VCSEL includes only a very short gain region because the beam passes vertically through the junction layer. One consequence is that VCSEL powers generally are in the milliwatt range, lower than edge emitters.

VCSEL cavities also include spacers, typically above and below the junction layer. These spacers control the length of the VCSEL cavity, and thus select the longitudinal modes and the output wavelength.

Properties and advantages

The internal structure of a VCSEL is more complex than that of an edge emitter, but in the end the design reduces costs. Both VCSELs and edge emitters can be fabricated in large numbers on a wafer, but the VCSEL structure is complete on the wafer, so devices can be tested before the wafer is diced. In contrast, edge emitters are incomplete until the wafer is cleaved to form facets, so they must be tested individually. Testing and packaging costs tip the economic balance toward VCSELs.

Normal fabrication techniques readily yield monolithic two-dimensional arrays of VCSELs. Separate inputs can drive individual devices for optical processing and switching, or for supplying input to separate fibers. Grading the spacer layer across the wafer produces lasers with a range of wavelengths, potentially useful for wavelength-division multiplexing (WDM).

The circular cross-section of VCSELs gives better control over beam size and divergence than for edge emitters. VCSELs normally emit from areas 5 to 30 µm across, avoiding the broad divergence of edge emitters perpendicular to the thin junction plane. This aids coupling of VCSEL output into fibers, with the smaller-aperture VCSELs compatible with single-mode fibers and larger ones compatible with the multimode graded-index fibers used for local-area networks.

Although standard VCSELs cannot match the output powers of edge-emitting lasers, they are more powerful and have better beam quality than LEDs. Together with their higher modulation speeds and low cost, this makes VCSELs preferred light sources for local-area networks such as Gigabit Ethernet.

Another advantage of VCSELs is a lower sensitivity to scattering of transmitted signals toward the fiber. The distributed-Bragg-reflection output mirror strongly rejects the laser wavelength, and any noise that reaches the inside of the laser cavity is overwhelmed by the high circulating power. In contrast, signals scattered back into an edge emitter can cause serious noise problems, requiring the use of optical isolators.

Wavelengths and materials

The first VCSELs were made in gallium-arsenide (GaAs) materials, and so far VCSELs have been most successful at wavelengths of 750 to 850 nm and 980 nm. Much of this success comes from the comparative ease of making distributed Bragg reflectors. The refractive index of gallium aluminum arsenide (GaAlAs) varies significantly with the mixture, so it's easy to make alternating layers with large enough refractive index for high Bragg reflection. The higher the index contrast, the fewer alternating layers are needed to make a reflector.

Intense development has focused on longer wavelengths of 1300 to 1700 nm, where fibers have lower attenuation and dispersion. However, the standard material used for edge emitters in that range, indium gallium arsenide phosphide (InGaAsP), has proven difficult for VCSELs. The refractive index changes little with composition, so thick stacks of alternating layers are needed for distributed Bragg reflectors. Unfortunately, material losses accumulate with the number of layers, which together with other problems such as low thermal conductivity makes InGaAsP VCSELs with thick mirrors impractical.

Dielectric mirrors offer higher reflectivity, but they don't conduct current, making electrical excitation difficult. Nonetheless, M. C. Amann et al. of the Technical University of Munich (Germany) reported encouraging results on an InP substrate in a postdeadline paper at the European Conference on Optical Communications (ECOC) last September. They excited the dielectric-mirror side of a 1500-nm VCSEL through a buried tunnel junction, and coupled light out through a distributed Bragg mirror of InGaAlAs.

Developers are working on many alternative approaches, with some companies so secretive they decline to provide details. Bonding GaAs reflectors to InGaAsP active layers has worked in the laboratory, but that elaborate process is not attractive for industrial production.1

An alternative is to grow GaAs materials on InP substrates, called metamorphic growth because of the 3.7% difference in lattice spacing.2 At CLEO last May in San Francisco, W. Yuen et al. of Bandwidth9 (Fremont, CA) reported using this approach to make 1600-nm VCSELs emitting up to 0.45 mW. Starting with an InP substrate, they deposited a lattice-matched stack of InAlGaAs/InAlAs layers, and an active region containing InGaAs quantum wells. Then using metamorphic growth, they deposited a stack of alternating GaAs/AlGaAs layers as the top distributed Bragg reflector.

Larry Coldren's group at the University of California-Santa Barbara (UCSB) is investigating alternative materials for use with InP. In another ECOC postdeadline paper, the group reported a continuous-wave 1550-nm VCSEL with aluminum-gallium-arsenide-antimonide (AlGaAsSb) distributed Bragg reflectors grown on an InP substrate. Cladding layers of InP separated the reflectors from an InGaAs active layer.

Another promising approach is developing long-wavelength materials compatible with GaAs. A team at Sandia National Laboratories turned to InGaAsN, a nitride compound compatible with GaAs that also has been tested for solar cells. The researchers made 1300-nm VCSELs on a GaAs substrate, with distributed Bragg reflectors of GaAs/GaAlAs, and used InGaAsN only for quantum wells in the active layer. They licensed the technology to Cielo Communications (Broomfield, CO), and at the LEOS annual meeting (Rio Grande, Puerto Rico) last November reported output powers to 0.8 mW near 1300 nm.

Speed and applications

Gallium-arsenide VCSELs now dominate the gigabit generation of local-area networks. Devices that can be directly modulated at speeds to 2.5 Gbit/s are readily available, and 10-Gbit/s versions are in the development pipeline. Speeds to 12.5 Gbit/s have been demonstrated in devices emitting single and multiple transverse modes, says Felix Mederer of the University of Ulm in Germany.

Both dispersion and attenuation can limit 850-nm transmission. The proposed 10-Gigabit Ethernet standard (see table) envisions a 65-m limit in conventional 50/125-µm graded-index multimode fiber, but developers have gone well beyond that. In a postdeadline paper at CLEO, Martin C. Nuss's group at Bell Labs (Holmdel, NJ) reported transmitting a single 10-Gbit/s signal through 1.6 km of a high-bandwidth 50/125 graded-index fiber developed by the parent Lucent Technologies. At ECOC in September, the same group reported extending its experiments to coarse wavelength-division multiplexing (CWDM), with 10-Gbit/s channels at 815, 822, 828, and 835 nm squeezing 40 Gbit/s through 310 m of the same fiber. In a CLEO postdeadline paper, a team from Ulm and Bell Labs reported sending 10 Gbit/s through 2.8 km of the high-speed multimode fiber, limited by attenuation. The Ulm group is even testing single-mode fibers at short wavelengths, a technology largely abandoned 20 years ago with the opening of the 1300-nm window.

The 10-Gigabit Ethernet plan envisions 1300-nm transmission through hundreds of meters of multimode fiber using four wide-WDM channels, but turns to single-mode fiber for longer distances. The current upper limit is 40 km for a single channel at 1550 nm, but "many applications would love 60 to 100 km," says Eric Hall, a member of Coldren's group at UCSB. VCSELs are not required, but their low cost and wide bandwidth at shorter wavelengths makes them very attractive.

The next step is tunable VCSELs, which are already starting to emerge. Last year CoreTek (Burlington, MA) announced an optically pumped tunable VCSEL in a postdeadline paper at the Optical Fiber Communications Conference (OFC; Baltimore, MD). Tuning was based on changing the cavity length by moving an external cavity formed by a MEMS micromirror suspended above the surface. Bandwidth9 now has a long-wavelength electrically pumped VCSEL tunable across a range of 30 nm, says Charles Duvall, head of applications. The VCSEL also uses MEMS technology: the entire structure is grown; then a filler layer is etched away to leave a flexible mirror that moves up and down in response to an applied voltage . The company already has demonstrated direct modulation at 2.5 Gbit/s, and "it looks like we have a structure capable of going to 10 Gbit/s," says Duvall. Power is limited to 0.1 mW, but the company hopes to reach the milliwatt level this year.

Expect to see more new devices next month at OFC.


  1. Y. Qian et al., Appl. Phys. Lett. 71, 25 (July 1997).
  2. J. Boucart et al., IEEE J. of Sel. Areas in Quant. Elec. 5, 520 (May/June 1999).
About the Author

Jeff Hecht | Contributing Editor

Jeff Hecht is a regular contributing editor to Laser Focus World and has been covering the laser industry for 35 years. A prolific book author, Jeff's published works include “Understanding Fiber Optics,” “Understanding Lasers,” “The Laser Guidebook,” and “Beam Weapons: The Next Arms Race.” He also has written books on the histories of lasers and fiber optics, including “City of Light: The Story of Fiber Optics,” and “Beam: The Race to Make the Laser.” Find out more at

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