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Electronics Letters

A contrasting technique

anonymous

Published Oct 1, 2014• 0 citations
Publisher

Abstract

Researchers at the Rochester Institute of Technology in New York have increased the switching contrast of a particular kind of all-optical flip-flop by 28 dB, resulting in a switching contrast of 36.6 dB. This could provide a huge leap in the performances of a range of photonic techniques, such as all-optical packet switching, all-optical label addressing, and square-wave clock generation, as well as other photonic devices housing semiconductor optical amplifiers or even passive nonlinear media. Lead author, Claudio Ippolito, investigating optical flip-flops in the Photonic Systems Laboratory at the Rochester Institute of Technology All-optical flip-flops provide a means of sequential signal processing – as opposed to combinational signal processing – in the optical domain. The sequential-processing nature of all-optical flip-flops provides a latchable control signal for devices based on combinational processing. Drew Maywar, one of the authors of the Letter, told us that “advances in optical-packet switching performed at the University of Ghent, the University of Tokyo, and Eindhoven University of Technology, for example, use optical flip-flops to drive data-wavelength converters to achieve wavelength routing of optical packets.” However, Maywar explained, the switching performance of some previous optical flip-flops is poor – control signals operate with only specific polarisation states, over a narrow wavelength range of operation, or with high optical power. “The cycle switching time of some flip-flops is longer than 1 ns,” he said, “which is not ideal for some applications, and the switching contrast is also poor ( < 10 dB) for some demonstrated flip-flops.” In order to realize their 28 dB contrast enhancement, the team exploited two disparate physical processes within a resonant-type nonlinear medium: optical dispersive bistability and nonlinear polarisation rotation. The resulting bistable polarisation rotation (BPR), in conjunction with a linear polariser, then led to the increased switching contrast. In essence, Maywar explained, the team have realised a latchable polarisation switch: “whereas the traditional polarisation switch (or Kerr shutter) is a combinational device, acting only when on present control signals, our device is sequential, exhibiting memory of past control pulses, and these two polarisation states can be switched back and forth by control signals whose polarisation states are themselves arbitrary.” Another interesting aspect of the enhancement of the switching contrast is that it outperformed the standard method for measuring the contrast. For switching contrasts around 5 dB (the previous standard), a photodiode and oscilloscope were sufficient but, as the contrast improved, this technique set a false upper bound of around 15 dB. “After some tinkering and reflection,” explained Maywar, “it was realised that a more sensitive diagnostic was needed, which provided a nice, educational-enriching hurdle that challenged the students’ notions of the actual signal vs the measured signal.” Maywar expects their work to be easily extended to other resonators, such as loops, rings, distributed feedback structures, and vertical cavities, and to other nonlinear media, such as passive InP and SiO2. Furthermore, enhanced-contrast flip-flops are building blocks and he hopes to make use of such devices in larger functional photonic subsystems. Contrast enhancement is fuelled by bistable polarisation rotation. The latchable state of polarisation exiting the all-optical flip-flop is controlled by arbitrarily polarised set and reset pulses This integration would be achieved through the miniaturisation of the team's all-optical flip-flops. “Such an effort is expected to increase the cycle-switching time, and lower energy consumption and heat dissipation,” said Maywar “and this work is aligned with our team's wider research goals of developing photonic devices and demonstrating optical-switching applications.” Looking to the future, Maywar told us that he thinks research in all-optical flip-flops will continue to improve switching performance and attack the major issues of drive power (energy consumption and heat dissipation), and device size: “I would like to see demonstration of miniaturised all-optical flip-flops, at least 100 times smaller than the millimetre-length devices used in present-day demonstrations. As such, nanophotonics may provide a path forward in keeping control-signal power reasonable with such small, nonlinear components.”

DOI
10.1049/el.2014.3604

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Researchers at the Rochester Institute of Technology in New York have increased the switching contrast of a particular kind of all-optical flip-flop by 28 dB, resulting in a switching contrast of 36.6 dB. This could provide a huge leap in the performances of a range of photonic techniques, such as all-optical packet switching, all-optical label addressing, and square-wave clock generation, as well as other photonic devices housing semiconductor optical amplifiers or even passive nonlinear media. Lead author, Claudio Ippolito, investigating optical flip-flops in the Photonic Systems Laboratory at the Rochester Institute of Technology All-optical flip-flops provide a means of sequential signal processing – as opposed to combinational signal processing – in the optical domain. The sequential-processing nature of all-optical flip-flops provides a latchable control signal for devices based on combinational processing. Drew Maywar, one of the authors of the Letter, told us that “advances in optical-packet switching performed at the University of Ghent, the University of Tokyo, and Eindhoven University of Technology, for example, use optical flip-flops to drive data-wavelength converters to achieve wavelength routing of optical packets.” However, Maywar explained, the switching performance of some previous optical flip-flops is poor – control signals operate with only specific polarisation states, over a narrow wavelength range of operation, or with high optical power. “The cycle switching time of some flip-flops is longer than 1 ns,” he said, “which is not ideal for some applications, and the switching contrast is also poor ( < 10 dB) for some demonstrated flip-flops.” In order to realize their 28 dB contrast enhancement, the team exploited two disparate physical processes within a resonant-type nonlinear medium: optical dispersive bistability and nonlinear polarisation rotation. The resulting bistable polarisation rotation (BPR), in conjunction with a linear polariser, then led to the increased switching contrast. In essence, Maywar explained, the team have realised a latchable polarisation switch: “whereas the traditional polarisation switch (or Kerr shutter) is a combinational device, acting only when on present control signals, our device is sequential, exhibiting memory of past control pulses, and these two polarisation states can be switched back and forth by control signals whose polarisation states are themselves arbitrary.” Another interesting aspect of the enhancement of the switching contrast is that it outperformed the standard method for measuring the contrast. For switching contrasts around 5 dB (the previous standard), a photodiode and oscilloscope were sufficient but, as the contrast improved, this technique set a false upper bound of around 15 dB. “After some tinkering and reflection,” explained Maywar, “it was realised that a more sensitive diagnostic was needed, which provided a nice, educational-enriching hurdle that challenged the students’ notions of the actual signal vs the measured signal.” Maywar expects their work to be easily extended to other resonators, such as loops, rings, distributed feedback structures, and vertical cavities, and to other nonlinear media, such as passive InP and SiO2. Furthermore, enhanced-contrast flip-flops are building blocks and he hopes to make use of such devices in larger functional photonic subsystems. Contrast enhancement is fuelled by bistable polarisation rotation. The latchable state of polarisation exiting the all-optical flip-flop is controlled by arbitrarily polarised set and reset pulses This integration would be achieved through the miniaturisation of the team's all-optical flip-flops. “Such an effort is expected to increase the cycle-switching time, and lower energy consumption and heat dissipation,” said Maywar “and this work is aligned with our team's wider research goals of developing photonic devices and demonstrating optical-switching applications.” Looking to the future, Maywar told us that he thinks research in all-optical flip-flops will continue to improve switching performance and attack the major issues of drive power (energy consumption and heat dissipation), and device size: “I would like to see demonstration of miniaturised all-optical flip-flops, at least 100 times smaller than the millimetre-length devices used in present-day demonstrations. As such, nanophotonics may provide a path forward in keeping control-signal power reasonable with such small, nonlinear components.”
This thesis experimentally characterizes the polarization dependence of an all-optical flip-flop (AOFF) based on a resonant-type semiconductor optical amplifier. Previous demonstrations of such an optical-memory device have exhibited poor on-off contrasts of around 3 dB (2:1). Our work maps out the dependence of the bistable hysteresis on the injected polarization state for the first time and clearly shows how to optimize the on-off contrast to achieve 8 dB. Beyond this optimization technique, it also demonstrate a novel technique to achieve and on-off contrast exceeding 30 dB (1000:1).
An all-optical flip-flop, the memory of which is based on dispersive bistability in a single vertical cavity semiconductor optical amplifier, is demonstrated experimentally. Flip-flop control is achieved using two mechanisms: cross-phase modulation to set the flip-flop and cross-gain modulation of the holding beam within a remote SOA to reset it. Optical control signals are sub-milliwatt in power and derived from a single 5 ns, 1539 nm initial pulse. Flip-flop operation at 1542 nm is polarisation insensitive to control signals and achieved with an on-off contrast greater than 3 dB.
The Kerr nonlinearity can be a key enabler for many digital photonic circuits as it allows access to bistable states needed for all-optical memories and switches. A common technique is to use the Kerr shift to control the resonance frequency of a resonator and use it as a bistable, optically-tunable filter. However, this approach works only in a narrow power and frequency range or requires the use of an auxiliary laser. An alternative approach is to use the asymmetric bistability between counterpropagating light states resulting from the interplay between self- and cross-phase modulation, which allows light to enter a ring resonator in just one direction. Logical high and low states can be represented and stored as the direction of circulation of light, and controlled by modulating the input power. Here we study the switching speed, operating laser frequency and power range, and contrast ratio of such a device. We reach a bitrate of 2 Mbps in our proof-of-principle device over an optical frequency range of 1 GHz and an operating power range covering more than one order of magnitude. We also calculate that integrated photonic circuits could exhibit bitrates of the order of Gbps, paving the way for the realization of robust and simple all-optical memories, switches, routers and logic gates that can operate at a single laser frequency with no additional electrical power.
We have demonstrated for the first time an all-optical flip-flop based on optical bistability of an integrated SOA/DFB-SOA by applying an input signal with the period of 25.2 ns. An all-optical flip-flop based on optical bistability is expected to process the signal at an ultra-high speed in a light-wave communication. All-optical flip-flop has various applications such as all optical memory, demultiplexing, packet-header buffering, and retiming. Moreover, an integrated SOA/DFBSOA can perform all-optical logic operation and wavelength conversion by cross gain modulation.
We present an experimental demonstration of an all optical memory consisting of a single semiconductor optical amplifier as the active medium based on wave mixing. The circuit is a fiber ring consisting of a semiconductor amplifier, a bi-directional 2x2 fiber coupler, an isolator, a polarization controller, and a Faraday mirror. The output is observed on the spectrum analyzer, which consists of the peak wavelength of the SOA plus an additional signal generated through wave mixing, which is tunable within the band gap of the SOA. We shall demonstrate two modes of operation of the device, which will consist of a flip flop switch between three states, as well as a single data storage memory. The stable states consist of two modes, where the mode amplitude represents the state. Mode 1 corresponds to 1500 nanometers and mode 2 corresponds to 1530 nanometers. A contrast ratio between an “on” and “off” state is measured for each mode and the mode of operation is based on the polarization. We shall present the states for the circuit, the effect of drive current on the system, the effect of the SOA structure, wave mixing effects, and how to operate the device for both logic operation and data storage.