
- •Fiber optics
- •Fiber optics
- •Erbium-doped fiber amplifiers
- •Nonlinearity
- •Fiber lasers
- •Figure 3
- •Doing it all with fiber?
- •The global electric circuit
- •III. Vocabulary and word study
- •The Global Electric Circuit
- •Generators and sources
- •Monitoring the global electric circuit
- •Challenge to established views
- •Energy from inertial fusion
- •III. Vocabulary and Word Study
- •Components
- •Solid-state lasers
- •Light-ion accelerators
- •Heavy-ion accelerators
- •Reactors
- •Cascade.
- •Power plant operating parameters
- •Target factory
- •Environmental, safety and health issue
- •Is getting a lot more precise
- •Optical Frequency Measurement Is Getting a Lot More Precise Abridged
- •The problem
- •The experiment
- •Testing qed
- •Spreading the technique
- •Ancient stardust in the laboratory
- •III. Vocabulary and word study
- •Searching for Stardust
- •Stellar parents: how many and what kind?
- •Forming stellar grains
- •Probing the early Solar System
- •A continuous model of computation
- •2. Write down the physical terms, known to you, in Russian.
- •A continuous model of computation
- •Two models of computation
- •Turing-machine model—pros and cons
- •Real-number model—pros and cons
- •Information-based complexit
- •The curse of dimensionality
- •The information level
- •Monte Carlo
- •Path integrals
- •III.Vocabulary and Word Study
- •IV. Reading for General Understannding
- •III. Vocabulary and Word Study
- •Planar imaging with X rays
- •Sectional imaging
- •Digital imaging
- •Treatment planning
- •Tomographic therapy
- •The cosmic rosetta stone
- •Write down the physical terms, known to you, in Russian.
- •III. Vocabulary and Word Study.
- •Abridged
- •Anisotropy in the cosmic background
- •Box 1. Big Bang Basics
- •The scientific harvest
- •Box 2. The Physics of cmb Anisotropy
- •The Scientific Harvest
Nonlinearity
13 An important new limit to long-distance transmission is caused by optical nonlinearity of the silica fiber.
Although nonlinearities of silica are extremely small, and one never had to consider them in the past because electronic repeaters reshaped the pulses, long optical interaction lengths without regeneration and higher-average optical powers make even these small non- linearities significant. Nonlinearities result in pulse broadening and cross talk between channels. A number of systems
have increased exponentially in capacity and distance over the last decade. Commercial implementation (red) of new systems has followed the first research results (blue) by about four years. Figure 2
studies have been carried out on non-linearities such as stimulated Brillouin scattering, stimulated Raman scattering, self-phase modulation, cross-phase modulation and four-photon mixing. Even at power levels as low as a few milliwatts one must now take these nonlinearities into account in designing a system. Despite these limitations, testbeds have demonstrated excellent performance at 5 Gb/sec over 9000 km.
14 Physicists have, however, yet another trump card to play. It turns out that a solution to Maxwell's equation in a lossless, single-mode optical fiber including the nonlinear term and chromatic dispersion is nondispersive in both the time domain and the frequency domain. The stable solution of this type for the optical pulse, called a "soliton," is u{z,t) = sech(f) exp(iz/2), where u{z,f) is the envelope of the pulse, z is the distance of propagation, and t is the elapsed time (both suitably normalized). If one launches such a pulse, with a correctly chosen width-to-peak-power relationship, into an ideal lossless fiber, it will propagate without change over arbitrarily long distances. Physically a pulse of this kind will maintain its shape because the chromatic dispersion and nonlinearity effects cancel each other out. Linn Mollenauer, Rogers Stolen and James Gordon at AT&T Bell Labs demonstrated soliton propagation in fibers experimentally in 1980.
15 For several years research on optical soliton propagation in fibers continued with little attention from optical systems designers, but the invention of the optical fiber amplifier has made long-distance soliton propagation a practical reality. In recent experiments solitons have retained their precise pulse shapes over thousands of kilometers. Furthermore, experiments with two wavelength channels showed that solitons of different wavelengths can pass through each other without changing shape. In these experiments the limits on distance and bit rate (per channel) were set by amplified spontaneous emission from the erbium amplifiers. The amplified spontaneous emission frequency modulates the signal frequencies via the nonlinearity, resulting in a distribution of pulse arrival times ("jitter"). This is known as the Gordon-Haus effect, after Gordon and Hermann Haus (MIT). This jitter can be reduced by using a guiding frequency filter, which guides the pulse in the frequency domain. The improvement is limited, however, by the need for more amplification (to compensate for the loss caused by the insertion of the filter), which in turn leads to more amplified spontaneous emission.
16 A major advance in 1992 overcame this limit and allowed error-free propagation of solitons over a distance of 20 000 km at a bit rate of 10 Gb/sec and over 13 000 km at 20 Gb/sec using two wavelength channels each at 10 Gb/sec. Mollenauer and coworkers achieved this breakthrough by using a sliding frequency filter in which the guiding filter frequency is slightly shifted after each amplification step. This concept creates a transmission line that is transparent to solitons, which can adjust to the frequency shift, but opaque to amplified spontaneous emission noise, which cannot adjust. Since this discovery has overcome the previous limitations of the Gordon-Haus effect, more research is now necessary to establish the new fundamental limit for soliton transmission! Solitons, with all of their advantages, are expected to find their way into commercial systems before the end of the decade.