Abstract:A new scheme for coding optical signals using the polarization of light is described. The coding response is shown to be linear and invariant. As a consequence of the vectorial nature of the electromagnetic waves, this response takes a sinusoidal shape, which limits the number of channels to three. An application to fiber optics transmissions is presented; an experimental 50-m link is described. The performance and loss of the system are discussed as well as the influence of specific factors, such as the coher… Show more
“…Frequency-dependent delays, but with ∆T (c) = ∆T (c) for all c, increase the rates with respect to the fully synchronized case. We chose the single-carrier delays as ∆T = ∆T (−2) , ∆T (−1) , ∆T (0) , ∆T (1) , ∆T (2) = ( 5 where T 4SC = 4T . These delays were chosen randomly and optimization could increase the rates further.…”
Section: A Dual Polarization Systemmentioning
confidence: 99%
“…Dual-polarization (2-pol) transmission almost doubles the data rates of optical fiber links [1], [2]. The apparent small reduction from a factor of two is caused by nonlinear coupling of polarizations due to the Kerr effect [3], [4].…”
Regular perturbation is applied to the Manakov equation and motivates a generalized correlated phase-andadditive noise model for wavelength-division multiplexing over dual-polarization optical fiber channels. The model includes three hidden Gauss-Markov processes: phase noise, polarization rotation, and additive noise. Particle filtering is used to compute lower bounds on the capacity of multi-carrier communication with frequency-dependent powers and delays. A gain of 0.17 bits/s/Hz/pol in spectral efficiency or 0.8 dB in power efficiency is achieved with respect to existing models at their peak data rate. Frequency-dependent delays also increase the spectral efficiency of single-polarization channels.
“…Frequency-dependent delays, but with ∆T (c) = ∆T (c) for all c, increase the rates with respect to the fully synchronized case. We chose the single-carrier delays as ∆T = ∆T (−2) , ∆T (−1) , ∆T (0) , ∆T (1) , ∆T (2) = ( 5 where T 4SC = 4T . These delays were chosen randomly and optimization could increase the rates further.…”
Section: A Dual Polarization Systemmentioning
confidence: 99%
“…Dual-polarization (2-pol) transmission almost doubles the data rates of optical fiber links [1], [2]. The apparent small reduction from a factor of two is caused by nonlinear coupling of polarizations due to the Kerr effect [3], [4].…”
Regular perturbation is applied to the Manakov equation and motivates a generalized correlated phase-andadditive noise model for wavelength-division multiplexing over dual-polarization optical fiber channels. The model includes three hidden Gauss-Markov processes: phase noise, polarization rotation, and additive noise. Particle filtering is used to compute lower bounds on the capacity of multi-carrier communication with frequency-dependent powers and delays. A gain of 0.17 bits/s/Hz/pol in spectral efficiency or 0.8 dB in power efficiency is achieved with respect to existing models at their peak data rate. Frequency-dependent delays also increase the spectral efficiency of single-polarization channels.
“…Both transmission media and DoFP polarimeter filter array are represented by Mueller matrices [48]. Following approach of Herad and Lacourt the models for various transmission media can be derived and used for simulation of high-speed optical data communications systems [23]. The DoFP polarimeter filter array on the CMOS receiver separates optical signals with different polarization angles.…”
Section: Chapter 2 Background and Related Workmentioning
confidence: 99%
“…They showed effective signal separation with two optical channels arranged 90 o apart. Also, there has been some previous work where three optical signals with different polarization angles were sent thru a single-mode fiber cable (without polarization preservation) and these signals were recovered on receiver side of the experiment [23]. This experiment was also performed on an optical bench.…”
Section: Chapter 2 Background and Related Workmentioning
“…Herard and Lacourt [4] were the first to take advantage of this fact in an optical communication system, experimentally demonstrating a free-space IM/DD link with three SOPs and analog demultiplexing. This was followed by Herard and Lacourt [22], with an extended theoretical analysis accounting for the impact of various factors including polarization mode dispersion and mode coupling on the system's performance. At that time, no more than three SOPs were used for simultaneous data transmission in IM/DD scenarios, and no algorithm for real-time polarization tracking was presented.…”
We demonstrate for the first time an intensitymodulated direct-detection link using four states of polarization. The four data-independent tributaries are each assigned distinct states of polarization to enable the receiver to separate the signals. Polarization rotation due to propagation over optical fiber is tracked and compensated with simple digital signal processing in Stokes space. Transmission below the forward error correction limit is shown for maximum net bitrates of 100 Gb/s (4 × 27 GBd) and 120 Gb/s (4 × 32 GBd) over 2-km standard single-mode fiber at a center wavelength of 1550 nm.
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