Abstract

Silicon photonics is the guiding of light in a planar arrangement of silicon-based materials to perform various functions. We focus here on the use of silicon photonics to create transmitters and receivers for fiber-optic telecommunications. As the need to squeeze more transmission into a given bandwidth, a given footprint, and a given cost increases, silicon photonics makes more and more economic sense.

Highlights

  • Until circa 2002, fiber-optic communication for metropolitan distances (80—600 km) and longhaul distances (600–15,000 km) employed mostly simple on-off keying (OOK) transmission

  • While these silicon-on-insulator (SOI) wafers are what makes low-loss silicon photonic waveguides possible, they are used mostly for low-power complementary metal-oxide-semiconductor (CMOS) circuits, because of the low leakage currents they offer

  • One is the surface-emitting grating coupler, as shown in Figure 7A [5, 6]. It consists of a strong grating in the waveguide with a pitch approximately equal to the wavelength in the waveguide. This causes light to emit or be received vertical to the surface, which is well-suited for wafer level measurements and/or coupling to an optical fiber

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Summary

Introduction

Until circa 2002, fiber-optic communication for metropolitan distances (80—600 km) and longhaul distances (600–15,000 km) employed mostly simple on-off keying (OOK) transmission. I.e., a lower bit-error rate (BER) for the same received optical power and/or for the same optical signal-tonoise ratio (OSNR), can be obtained by using phase-modulated formats, such as binary phase-shift keying (BPSK) or quadrature phase-shift keying (QPSK). In today’s coherent CFP, there is a single silicon photonic (SiPh) integrated circuit (PIC) containing both the transmitter and receiver [4]. A dominant cost for the DSP and optics is the packaging; one can further reduce cost, power, and footprint by co-packaging the DSP and optics Such transceivers are expected in 2–3 years. The main advantages of photonic integration are a small footprint, due to strongly confining waveguides and lens-free connections between parts; low power, due to an obviation of 50- RF lines; higher bandwidth RF connections; and low price, due to fewer touch points, no mechanical adjustments, less test equipment, and less material. The main disadvantages of PICs are typically a higher insertion loss and the inability to optimize components independently

PIC Material Systems
Si Photonic Passive Elements
Si Photonic Active Elements
PIC Material System Comparison
PIC Design
Short Reach PICs
Metro and Long-reach PICs
Conclusion

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