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Signal-induced birefringence and dichroism in a tensile-strained bulk semiconductor optical amplifier and its application to wavelength conversion (2005)

by L Q Guo, M J Connelly
Venue:J. Lightw. Technol
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Polarizationdependent gain in SOA-based optical multistage interconnection networks

by Odile Liboiron-ladouceur, Student Member, Keren Bergman, Misha Boroditsky, Senior Member, Misha Brodsky - J. Lightwave Technol , 2006
"... Abstract—The small polarization dependence (< 1 dB) of optical components becomes significant in optical multistage interconnection networks. The cumulative effect can ultimately limit physical layer scalability by changing the maximum number of internal nodes that optical packets can traverse er ..."
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Abstract—The small polarization dependence (&lt; 1 dB) of optical components becomes significant in optical multistage interconnection networks. The cumulative effect can ultimately limit physical layer scalability by changing the maximum number of internal nodes that optical packets can traverse error free. It is shown that for nodes based on commercial semiconductor optical amplifier (SOA) switches with polarization-dependent gains of less than 0.35 dB, the maximum number of cascaded nodes changes by as much as 20 nodes, depending on both the packet wavelength and its state of polarization. This deviation in the number of nodes could correspond to a 100-fold decrease in the number of interconnected ports of an optical interconnection network such as the data vortex. This dramatic effect is explained in terms of optical signal-to-noise ratio degradation due to accumulated amplified spontaneous emission noise originating from the SOA device in the node. Index Terms—Multistage interconnection networks (MINs), optical packet switching, polarization-sensitive devices, semiconductor optical amplifier (SOA). I.
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...gher PDG is associated with higher gain, as the balance achieved between the differences in confinement factors and the strain in this particular SOA design is more difficult to maintain at high gain =-=[17]-=-. In a real system, the cumulative PDG will oscillate between the minimum and maximum gains with the number of nodes, due to the structure of the recirculating loop [18], [19]. V. N ETWORK PHYSICAL LA...

Impact of Cumulative Polarization-Dependent Gain on SOA-Based Optical Packet Switching Networks

by Odile Liboiron-ladouceur, Student Member, Keren Bergman, Misha Boroditsky, Senior Member, Misha Brodsky
"... Abstract—The physical layer scalability of multistage interconnection networks is determined by the maximum number of internal switching nodes that packets can traverse error-free. We show that for nodes based on commercial semiconductor optical amplifier switches with polarization-dependent gain of ..."
Abstract - Cited by 1 (0 self) - Add to MetaCart
Abstract—The physical layer scalability of multistage interconnection networks is determined by the maximum number of internal switching nodes that packets can traverse error-free. We show that for nodes based on commercial semiconductor optical amplifier switches with polarization-dependent gain of less than 0.35 dB, the maximum number of cascaded nodes could vary by as much as 20 nodes, depending both on the packet wavelength and its state of polarization. We explain such a dramatic effect by optical signal-to-noise ratio degradation due to accumulated amplified spontaneous emission noise with the number of nodes. Index Terms—Optical packet switching (OPS), polarization-sensitive devices, semiconductor optical amplifier (SOA). I.
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... dB at 1528 nm and 0.10 dB at 1550 nm at a gain set to 13 dB. Higher PDG is associated with higher gain as the balance achieved between the difference in confinement factors and the strain in the SOA =-=[10]-=- is more difficult to maintain at high gain. We now turn to the investigation of the impact of cumulative PDG on the network size scalability. For each channel. three BER curves (corresponding to the ...

of polarization effects in semiconductor optical amplifiers to perform all-optical… THE USE OF POLARIZATION EFFECTS IN SEMICONDUCTOR OPTICAL AMPLIFIERS TO PERFORM ALL-OPTICAL SIGNAL PROCESSING

by El Uso, De Efectos, De Polarización, En Amplificadores, Ópticos Semiconductores, Para Realizar, El Procesamiento, De Señales, En El, Dominio Óptico, Brendan F. Kennedy Frederic Surre , 2007
"... En los servicios de telecomunicaciones, la necesidad de hacer uso intensivo de las aplicaciones ha presionado por un constante incremento del ancho de banda. Particularmente una de las tecnologías más promisorias, que ha permitido estos incrementos de ancho de banda, son los elementos ópticos, de ta ..."
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En los servicios de telecomunicaciones, la necesidad de hacer uso intensivo de las aplicaciones ha presionado por un constante incremento del ancho de banda. Particularmente una de las tecnologías más promisorias, que ha permitido estos incrementos de ancho de banda, son los elementos ópticos, de tal manera que en las redes de comunicación los elementos electrónicos sean sustituidos por dichos elementos ópticos. En esta publicación se discute una técnica basada en la rotación no lineal del estado de polarización de una señal óptica conectada al amplificador semiconductor óptico. Se presenta un experimento, basado en este efecto, para realizar la conversión a 2,5 Gbits/s. La característica del conversor de longitud onda es probada en propagación directa e inversa. Se ha encontrado que conversión de la longitud de onda es independiente de longitud de onda (la conversión no depende del valor de la longitud de onda) en la modalidad de propagación directa no invertida. Palabras clave: Amplificador semiconductor óptico, conversión de la longitud de onda, rotación no lineal del estado de polarización. As the need for higher and higher bandwidths in telecommunication systems continues, it is widely predicted that at some point in the future optical processing will need to be performed all-optically. Several techniques have been proposed to perform such all-optical signal processing. In this paper a technique based on the nonlinear rotation in the state
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... gain and polarization nonlinearities in the two devices. It should be noted that whilst the results presented in figure 5 are in contrast to [13], they are in agreement with the results presented in =-=[14]-=-. the Figure 3. BER as a function of received converted power for XGM, inverted XPolM and non-inverted XPolM in (a) co- and (b) counter-propagation. Pump wavelength = 1538 nm, probe wavelength = 1535 ...

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