Modern fiber-optic communication systems generally include optical transmitters that convert electrical signals into optical signals,
optical fiber cables to carry the signal, optical amplifiers, and optical receivers to convert the signal back into an electrical signal. The information transmitted is typically
digital information generated by computers or
telephone systems.
Transmitters module (shown here with its cover removed), is an optical and electrical
transceiver, a device combining a transmitter and a receiver in a single housing. The electrical connector is at the top right, and the optical connectors are at bottom left. The most commonly used optical transmitters are semiconductor devices such as
light-emitting diodes (LEDs) and
laser diodes. The difference between LEDs and laser diodes is that LEDs produce
incoherent light, while laser diodes produce coherent light. For use in optical communications, semiconductor optical transmitters must be designed to be compact, efficient and reliable, while operating in an optimal wavelength range and directly modulated at high frequencies. In its simplest form, an LED emits light through
spontaneous emission, a phenomenon referred to as
electroluminescence. The emitted light is incoherent with a relatively wide spectral width of 30–60 nm. The large spectrum width of LEDs is subject to higher fiber dispersion, considerably limiting their bit rate-distance product (a common measure of usefulness). LEDs are suitable primarily for
local-area-network applications with bit rates of 10– and transmission distances of a few kilometers. LED light transmission is inefficient, with only about 1% of input power, or about 100 microwatts, eventually converted into launched power coupled into the optical fiber. LEDs have been developed that use several
quantum wells to emit light at different wavelengths over a broad spectrum and are currently in use for local-area
wavelength-division multiplexing (WDM) applications. LEDs have been largely superseded by
vertical-cavity surface-emitting laser (VCSEL) devices, which offer improved speed, power and spectral properties, at a similar cost. However, due to their relatively simple design, LEDs are very useful for very low-cost applications. Commonly used classes of semiconductor laser transmitters used in fiber optics include VCSEL,
Fabry–Pérot and
distributed-feedback laser. A semiconductor laser emits light through
stimulated emission rather than spontaneous emission, which results in high output power (~100 mW) as well as other benefits related to the nature of coherent light. The output of a laser is relatively directional, allowing high coupling efficiency (~50%) into single-mode fiber. Common VCSEL devices also couple well to multimode fiber. The narrow spectral width also allows for high bit rates since it reduces the effect of
chromatic dispersion. Furthermore, semiconductor lasers can be modulated directly at high frequencies because of their short
recombination time. Laser diodes are often directly
modulated, that is the light output is controlled by a current applied directly to the device. For very high data rates or very long distance links, a laser source may be operated
continuous wave, and the light modulated by an external device, an
optical modulator, such as an
electro-absorption modulator or
Mach–Zehnder interferometer. External modulation increases the achievable link distance by eliminating laser
chirp, which broadens the
linewidth in directly modulated lasers, increasing the chromatic dispersion in the fiber. For very high bandwidth efficiency, coherent modulation can be used to vary the phase of the light in addition to the amplitude, enabling the use of
QPSK,
QAM, and
OFDM. "Dual-polarization quadrature phase shift keying is a modulation format that effectively sends four times as much information as traditional optical transmissions of the same speed."
Receivers The main component of an optical receiver is a
photodetector which converts light into electricity using the
photoelectric effect. The primary photodetectors for telecommunications are made from
Indium gallium arsenide. The photodetector is typically a semiconductor-based
photodiode. Several types of photodiodes include p–n photodiodes, p–i–n photodiodes, and avalanche photodiodes.
Metal-semiconductor-metal (MSM) photodetectors are also used due to their suitability for
circuit integration in
regenerators and wavelength-division multiplexers. Since light may be attenuated and distorted while passing through the fiber, photodetectors are typically coupled with a
transimpedance amplifier and a limiting
amplifier to produce a digital signal in the electrical domain recovered from the incoming optical signal. Further signal processing, such as
clock recovery from data performed by a
phase-locked loop may also be applied before the data is passed on. Coherent receivers use a local oscillator laser in combination with a pair of hybrid couplers and four photodetectors per polarization, followed by high-speed ADCs and digital signal processing to recover data modulated with QPSK, QAM, or OFDM.
Digital predistortion An optical communication system
transmitter consists of a
digital-to-analog converter (DAC), a
driver amplifier and a
Mach–Zehnder modulator. The deployment of higher
modulation formats (>
4-QAM) or higher
baud Rates (>) diminishes the system performance due to linear and non-linear transmitter effects. These effects can be categorized as linear distortions due to DAC bandwidth limitation and transmitter I/Q
skew as well as non-linear effects caused by gain saturation in the driver amplifier and the Mach–Zehnder modulator. Digital
predistortion counteracts the degrading effects and enables Baud rates up to and modulation formats like
64-QAM and
128-QAM with the commercially available components. The transmitter
digital signal processor performs digital predistortion on the input signals using the inverse transmitter model before sending the samples to the DAC. Older digital predistortion methods only addressed linear effects. Recent publications also consider non-linear distortions.
Berenguer et al models the Mach–Zehnder modulator as an independent
Wiener system and the DAC and the driver amplifier are modeled by a truncated, time-invariant
Volterra series.
Khanna et al use a memory polynomial to model the transmitter components jointly. In both approaches, the Volterra series or the memory polynomial coefficients are found using
indirect-learning architecture.
Duthel et al records, for each branch of the Mach-Zehnder modulator, several signals at different polarities and phases. The signals are used to calculate the optical field.
Cross-correlating in-phase and quadrature fields identifies the
timing skew. The
frequency response and the non-linear effects are determined by the indirect-learning architecture.
Fiber cable types An
optical fiber cable consists of a core,
cladding, and a buffer (a protective outer coating), in which the cladding guides the light along the core by using the method of
total internal reflection. The core and the cladding (which has a lower-
refractive-index) are usually made of high-quality
silica glass, although they can both be made of plastic as well. Connecting two optical fibers is done by
fusion splicing or
mechanical splicing and requires special skills and interconnection technology due to the microscopic precision required to align the fiber cores. Two main types of optical fiber used in optical communications include
multi-mode optical fibers and
single-mode optical fibers. A multi-mode optical fiber has a larger core (≥50
micrometers), allowing less precise, cheaper transmitters and receivers to connect to it as well as cheaper connectors. However, a multi-mode fiber introduces
multimode distortion, which often limits the bandwidth and length of the link. Furthermore, because of their higher
dopant content, multi-mode fibers are usually expensive and exhibit higher attenuation. The core of a single-mode fiber is smaller (<10 micrometers) and requires more expensive components and interconnection methods, but allows much longer and higher-performance links. Both single- and multi-mode fibers are offered in different grades. In order to package fiber into a commercially viable product, it typically is protectively coated by using ultraviolet-cured
acrylate polymers and assembled into a cable. After that, it can be laid in the ground and then run through the walls of a building and deployed aerially in a manner similar to copper cables. These fibers require less maintenance than common twisted pair wires once they are deployed. Specialized cables are used for long-distance subsea data transmission, e.g.,
transatlantic communications cable. New (2011–2013) cables operated by commercial enterprises (
Emerald Atlantis,
Hibernia Atlantic) typically have four strands of fiber and signals cross the Atlantic (NYC-London) in 60–70 ms. The cost of each such cable was about $300M in 2011. Another common practice is to bundle many fiber optic strands within long-distance
power transmission cable using, for instance, an
optical ground wire. This exploits power transmission rights of way effectively, ensures a power company can own and control the fiber required to monitor its own devices and lines, is effectively immune to tampering, and simplifies the deployment of
smart grid technology.
Amplification The transmission distance of a fiber-optic communication system has traditionally been limited by fiber attenuation and by fiber distortion. By using
optoelectronic repeaters, these problems have been eliminated. These repeaters convert the signal into an electrical signal and then use a transmitter to send the signal again at a higher intensity than was received, thus counteracting the loss incurred in the previous segment. Because of the high complexity of modern wavelength-division multiplexed signals, including the fact that they had to be installed about once every , the cost of these repeaters is very high. An alternative approach is to use
optical amplifiers, which amplify the optical signal directly without having to convert the signal to the electrical domain. One common type of optical amplifier is an
erbium-doped fiber amplifier (EDFA). These are made by
doping a length of fiber with the rare-earth mineral
erbium and
laser pumping it with light with a shorter wavelength than the communications signal (typically 980
nm). EDFAs provide gain in the ITU C band at 1550 nm. Optical amplifiers have several significant advantages over electrical repeaters. First, an optical amplifier can amplify a very wide band at once, which can include hundreds of
multiplexed channels, eliminating the need to demultiplex signals at each amplifier. Second, optical amplifiers operate independently of the data rate and modulation format, enabling multiple data rates and modulation formats to co-exist and enabling upgrading of the data rate of a system without having to replace all of the repeaters. Third, optical amplifiers are much simpler than a repeater with the same capabilities and are therefore significantly more reliable. Optical amplifiers have largely replaced repeaters in new installations, although electronic repeaters are still widely used when signal conditioning beyond amplification is required.
Wavelength-division multiplexing Wavelength-division multiplexing (WDM) is the technique of transmitting multiple channels of information through a single optical fiber by sending multiple light beams of different wavelengths through the fiber, each modulated with a separate information channel. This allows the available capacity of optical fibers to be multiplied. This requires a wavelength division multiplexer in the transmitting equipment and a demultiplexer (essentially a
spectrometer) in the receiving equipment.
Arrayed waveguide gratings are commonly used for multiplexing and demultiplexing in WDM. Using WDM technology now commercially available, the bandwidth of a fiber can be divided into as many as 160 channels to support a combined bit rate in the range of . == Parameters ==