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Optoelectronics & Communications

Coherently coupled laser arrays for low-dispersion, ultra-high-bandwidth data transfer

A novel design and operation technique based on an array of vertical-cavity surface-emitting lasers enables high-performance optical transmission.
2 June 2015, SPIE Newsroom. DOI: 10.1117/2.1201505.005958

For short-reach optical interconnects in data centers, server clusters, and supercomputer applications, the vertical-cavity surface-emitting laser (VCSEL) has emerged as the dominant emitter. It is estimated that the demand for optical interconnects for these applications will reach a market revenue of $520 million by 2019.1 VCSELs are currently being optimized for modulation rates of 25Gb/s, but demand for bandwidth is expected to reach serial data rates of 40–100Gb/s in the coming years. Furthermore, as data centers become physically larger in size, the optical interconnects used must achieve high bandwidth over longer fiber transmission distances, requiring both narrow spectral width and sufficient output power from the emitter. These demands constitute a formidable challenge and encourage the development of alternative designs and modulation concepts that maintain the significant advantages in performance, power efficiency, packaging, and manufacturing costs inherent in VCSELs.

Purchase SPIE Field Guide to Optical Fiber TechnologyOne such concept is the direct modulation of a single-mode, coherently coupled VCSEL array.2, 3 A transverse-coupled-cavity VCSEL—one with an integrated lateral feedback resonator—was shown to produce enhanced modulation amplitude at high frequency, demonstrating a 29GHz modulation bandwidth and a 36Gb/s modulation rate.4 Using resonance and coherence tuning of planar, phased photonic crystal 2×1 VCSEL arrays, we have been working on an approach to enhance modal control and allow strong optical coupling of array elements. Using this approach, we have developed a novel structure with significantly improved performance in addition to an operation technique that enables control over the enhanced frequency response.2, 3

The optically coupled phased VCSEL array is formed by combining a photonic-crystal-etched hole pattern with a laser gain structure defined by ion implantation: see Figure 1. The photonic crystal is a hexagonal lattice of circular holes. In this lattice, defects define the optical apertures of each array element. We designed the gain apertures such that they overlap both the top metal contacts and the photonic crystal apertures with an ion-implanted semiconductor, which acts as a non-conductive separation between the array elements. Optical coupling between the elements is enhanced by an anti-guiding laser array structure.5

Figure 1. (a) Optical image in which I1and I2 indicate bias currents applied to the left and right elements, respectively, and (b) scanning electron microscope image of 2×1 phased, photonic crystal vertical-cavity surface-emitting laser (VCSEL) array.

The photonic-crystal-etched hole pattern, which provides stable index guiding for the fundamental mode of array elements and greater optical loss for transverse modes, improves the modal control.6,7 Inter-element current confinement enables independent biasing of array elements and, in combination with the increased modal control, results in a method for controlling the enhanced modulation response.2, 3,8

Tuning the resonance and coherence of the phased VCSEL array under stable coherently coupled operation allows us to control this enhanced modulation response. Preferential current injection to an array element changes the cavity refractive index for that element via ohmic heating and electronic suppression, thereby varying its natural resonance.5 In effect, by varying the bias conditions, we are able to tune the resonance of each element as well as the phase relation and coherence of the array.9 By tuning the resonances of each array element into spectral overlap, with relative phase differences between the coupled cavities near zero (in phase) or pi (out of phase), stable coherently coupled operation can be achieved. Resonance detuning and variation of the phase relation of the array under coherently coupled operation enables the enhanced modulation response to be tuned.2, 3

The modulation response of a 2×1 phased photonic crystal VCSEL array under varying bias conditions is shown in Figure 2. An array can be tuned to produce an enhanced frequency response to better suit a specific application. Modulation bandwidths beyond 30GHz are particularly useful for ultra-fast optical interconnects in data center, server cluster, and supercomputer applications. A narrow bandwidth amplifier, centered at a millimeter-wave frequency, is useful for ultra-fast wireless communications and radio-frequency photonic-link technologies.

Figure 2. Modulation response of the 2×1 VCSEL array under different bias conditions (bias currents in milliamps). Bandwidth enhancement beyond 30GHz is shown by the red curve. Narrow-band enhanced modulation amplitudes, tuned to center frequencies between 20 and 30GHz, are shown by the cyan, magenta, and green curves. For comparison, the modulation response of the array at bias conditions that do not produce coherent coupling is shown by the blue curve.

Further performance advantages are also possible using our novel design. Due to the modal control and the nature of coherently coupled operation, the laser-array emission has narrow single-mode spectral width and increased output power.2, 7 Additionally, because of the decoupling of electrical and optical apertures and the independence of the operation technique from the bias-to-threshold current ratio, the device is operational at low current density.2, 10 This design has enabled us to achieve a bandwidth of 37GHz, obtained under highly single-mode (40dB side-mode suppression ratio) coherent operation, with a narrow spectral width (0.043nm root mean squared) and an increased output power (3.4mW) when the laser array is biased at low current density (8kA/cm2).2

In summary, our novel design concept and operation technique enables enhanced modulation response with narrow single-mode spectral widths and a relatively high output power under low-current-density operation. These properties are particularly desirable for reliable, ultra-fast data transmission over large distances in fiber. Additionally, the device benefits from the advantages inherent in the VCSEL structure and its evolution as the dominant emitter in short-reach optical communications. We are now working to optimize devices for use in optical interconnects and photonic link technologies by focusing on different designs to enhance operation in either the broadband, high-resonance frequency, or the high-gain regimes of modulation response.

Stewart Fryslie
Department of Electrical and Computer Engineering
University of Illinois at Urbana-Champaign
Champaign, Illinois

Stewart Fryslie is a PhD candidate in the department of electrical and computer engineering.

Kent Choquette
Photonic Devices Research Group / ECE
University of Illinois at Urbana-Champaign
Champaign, Illinois

1. http://cir-inc.com/reports/reports-current-reports-oicvii Revenue opportunities for optical interconnects: market and technology forecast 2013 to 2020, vol. 2. Accessed 27 April 2015.
2. S. T. M. Fryslie, M. P. Tan, D. F. Siriani, M. T. Johnson, K. D. Choquette, 37-GHz modulation via resonance tuning in single-mode coherent vertical-cavity laser arrays, IEEE Photon. Technol. Lett. 27(4), p. 415-418, 2014.
3. S. T. M. Fryslie, M. T. Johnson, M. P. Tan, D. F. Siriani, K. D. Choquette, Modulation bandwidth enhancement via resonance detuning in coherently coupled vertical cavity laser arrays, IPC , p. 93-94, 2014.
4. H. Dalir, F. Koyama, 29 GHz directly modulated 980 nm vertical-cavity surface emitting lasers with bow-tie shape transverse coupled cavity, Appl. Phys. Lett. 103, p. 091109, 2013.
5. D. F. Siriani, K. D. Choquette, Implant defined anti-guided vertical-cavity surface-emitting laser arrays, IEEE J. Quantum Electron. 47(2), p. 160-164, 2011.
6. J. J. Raftery Jr., A. J. Danner, J. C. Lee, K. D. Choquette, Coherent coupling of two-dimensional arrays of defect cavities in photonic crystal vertical cavity surface-emitting lasers, Appl. Phys. Lett. 86, p. 201104, 2005.
7. D. F. Siriani, P. O. Leisher, K. D. Choquette, Loss-induced confinement in photonic crystal vertical-cavity surface-emitting lasers, IEEE J. Quantum Electron. 45(7), p. 762-768, 2009.
8. M. T. Johnson, D. F. Siriani, M. P. Tan, K. D. Choquette, Beam steering via resonance detuning in coherently coupled vertical cavity laser arrays, Appl. Phys. Lett. 103, p. 201115, 2013.
9. M. T. Johnson, D. F. Siriani, J. D. Sulkin, K. D. Choquette, Phase and coherence extraction from a phased vertical cavity laser array, Appl. Phys. Lett. 101, p. 031116, 2012.
10. M. P. Tan, S. T. M. Fryslie, J. A. Lott, N. N. Ledentsov, D. Bimberg, K. D. Choquette, Error-free transmission over 1-km OM4 multimode fiber at 25 Gb/s using a single mode photonic crystal vertical-cavity surface-emitting laser, IEEE Photon. Technol. Lett. 25(18), p. 1823-1825, 2013.