Abstract:Abstract-We experimentally demonstrate a four-wave mixingbased wavelength conversion scheme at 1.55µm using a 1.1m length of highly nonlinear, dispersion tailored W-type leadsilicate optical fibre.
“…The outer cladding was made of a different glass with a higher refractive index, Schott SF6, (n=1.76 @ 1550nm). The nonlinear coefficient, dispersion and loss at 1550nm were 820W -1 km -1 , -3ps/nm/km and 2.1±0.2 dB/m respectively [4]. The dispersion profile of the fibre is shown in the inset to Fig.…”
Section: Experimental Setup and Resultsmentioning
confidence: 92%
“…However, compound glasses generally suffer from high normal material dispersion around 1.55µm and counter-balancing this with waveguide dispersion is a non-trivial fabrication task. We have recently shown a fibre design with a W-type refractive index profile as a possible solution to this problem [4] and fabricated a fibre with a highly nonlinear coefficient and low and flat dispersion profile at telecom wavelengths.…”
Section: Introductionmentioning
confidence: 99%
“…However, compound glasses generally suffer from high normal material dispersion around 1.55µm and counter-balancing this with waveguide dispersion is a non-trivial fabrication task. We have recently shown a fibre design with a W-type refractive index profile as a possible solution to this problem [4] and fabricated a fibre with a highly nonlinear coefficient and low and flat dispersion profile at telecom wavelengths.Here we experimentally demonstrate the generation of high repetition rate (160GHz and 200GHz) pulses through stable injection-locking of two semiconductor lasers in a 3m-long sample of the fabricated W-type fibre and investigated the role of the tailored dispersion profile for the generation of ultra-short high repetition rate pulses.
…”
Abstract:The generation of ultrastable optical pulses beyond 160GHz is demonstrated based on two injection-locked CW lasers through nonlinear temporal compression in a high SBSthreshold highly nonlinear dispersion tailored compound glass W-type fibre.
IntroductionThe generation of high repetition rate pulses through four-wave-mixing (FWM) based nonlinear temporal compression of a dual-frequency beat signal in a highly nonlinear fibre followed by a linear dispersive medium has proven to deliver high quality pedestal-free (sub-) picosecond signals [1][2][3]. The initially sinusoidal signal can be obtained from the beating of two continuous wave (CW) lasers with a frequency separation corresponding to the desired repetition rate. Usually, independent CW sources are used [1-2] leading to significant timing jitter on the pulses generated over a timescale inversely proportional to the laser linewidths and which can be a significant issue for many applications. In [3] this issue was addressed using stable injection-locking of two semiconductor lasers to an optical comb, then simultaneously performing narrow-bandwidth filtering and amplification. In that case the two phase-locked lasers were then combined together into 2-m-long highly nonlinear bismuth oxide fibre (Bi-NLF), which has high nonlinear coefficient, but also a high dispersion and dispersion slope. Efficient generation of FWM components generally requires a high nonlinear coefficient and a low dispersion and dispersion slope: much higher repetition rates can be envisaged and much higher pulse compression factors can be achieved as the pulses do not temporally broaden in the nonlinear medium. Compound-glass technology has enabled fibres with much higher values of effective nonlinearity than that achievable in silica. However, compound glasses generally suffer from high normal material dispersion around 1.55µm and counter-balancing this with waveguide dispersion is a non-trivial fabrication task. We have recently shown a fibre design with a W-type refractive index profile as a possible solution to this problem [4] and fabricated a fibre with a highly nonlinear coefficient and low and flat dispersion profile at telecom wavelengths.Here we experimentally demonstrate the generation of high repetition rate (160GHz and 200GHz) pulses through stable injection-locking of two semiconductor lasers in a 3m-long sample of the fabricated W-type fibre and investigated the role of the tailored dispersion profile for the generation of ultra-short high repetition rate pulses.
“…The outer cladding was made of a different glass with a higher refractive index, Schott SF6, (n=1.76 @ 1550nm). The nonlinear coefficient, dispersion and loss at 1550nm were 820W -1 km -1 , -3ps/nm/km and 2.1±0.2 dB/m respectively [4]. The dispersion profile of the fibre is shown in the inset to Fig.…”
Section: Experimental Setup and Resultsmentioning
confidence: 92%
“…However, compound glasses generally suffer from high normal material dispersion around 1.55µm and counter-balancing this with waveguide dispersion is a non-trivial fabrication task. We have recently shown a fibre design with a W-type refractive index profile as a possible solution to this problem [4] and fabricated a fibre with a highly nonlinear coefficient and low and flat dispersion profile at telecom wavelengths.…”
Section: Introductionmentioning
confidence: 99%
“…However, compound glasses generally suffer from high normal material dispersion around 1.55µm and counter-balancing this with waveguide dispersion is a non-trivial fabrication task. We have recently shown a fibre design with a W-type refractive index profile as a possible solution to this problem [4] and fabricated a fibre with a highly nonlinear coefficient and low and flat dispersion profile at telecom wavelengths.Here we experimentally demonstrate the generation of high repetition rate (160GHz and 200GHz) pulses through stable injection-locking of two semiconductor lasers in a 3m-long sample of the fabricated W-type fibre and investigated the role of the tailored dispersion profile for the generation of ultra-short high repetition rate pulses.
…”
Abstract:The generation of ultrastable optical pulses beyond 160GHz is demonstrated based on two injection-locked CW lasers through nonlinear temporal compression in a high SBSthreshold highly nonlinear dispersion tailored compound glass W-type fibre.
IntroductionThe generation of high repetition rate pulses through four-wave-mixing (FWM) based nonlinear temporal compression of a dual-frequency beat signal in a highly nonlinear fibre followed by a linear dispersive medium has proven to deliver high quality pedestal-free (sub-) picosecond signals [1][2][3]. The initially sinusoidal signal can be obtained from the beating of two continuous wave (CW) lasers with a frequency separation corresponding to the desired repetition rate. Usually, independent CW sources are used [1-2] leading to significant timing jitter on the pulses generated over a timescale inversely proportional to the laser linewidths and which can be a significant issue for many applications. In [3] this issue was addressed using stable injection-locking of two semiconductor lasers to an optical comb, then simultaneously performing narrow-bandwidth filtering and amplification. In that case the two phase-locked lasers were then combined together into 2-m-long highly nonlinear bismuth oxide fibre (Bi-NLF), which has high nonlinear coefficient, but also a high dispersion and dispersion slope. Efficient generation of FWM components generally requires a high nonlinear coefficient and a low dispersion and dispersion slope: much higher repetition rates can be envisaged and much higher pulse compression factors can be achieved as the pulses do not temporally broaden in the nonlinear medium. Compound-glass technology has enabled fibres with much higher values of effective nonlinearity than that achievable in silica. However, compound glasses generally suffer from high normal material dispersion around 1.55µm and counter-balancing this with waveguide dispersion is a non-trivial fabrication task. We have recently shown a fibre design with a W-type refractive index profile as a possible solution to this problem [4] and fabricated a fibre with a highly nonlinear coefficient and low and flat dispersion profile at telecom wavelengths.Here we experimentally demonstrate the generation of high repetition rate (160GHz and 200GHz) pulses through stable injection-locking of two semiconductor lasers in a 3m-long sample of the fabricated W-type fibre and investigated the role of the tailored dispersion profile for the generation of ultra-short high repetition rate pulses.
“…The complex interdependence between temperature, surface tension and internal pressure within the holes, however, causes small-scale longitudinal cross sectional variations, which are very difficult to control in practice. To solve this issue we have proposed in [3] a new all-solid fibre concept based on the use of three commercial lead silicate glasses (Schott SF57, LLF1, SF6) arranged in a W-type index profile. The fabricated fibre presents a flattened and near-zero dispersion profile and a high nonlinearity of 820W -1 km -1 at the telecom wavelengths.…”
Section: Introductionmentioning
confidence: 99%
“…The fabricated fibre presents a flattened and near-zero dispersion profile and a high nonlinearity of 820W -1 km -1 at the telecom wavelengths. Accurate polishing of the glass preform before the fibre drawing has allowed us to reduce the propagation losses from an initial value of ~5dB/m [3] down to ~2dB/m [4] in the 1.55µm region. In this talk we will review some examples of successful applications of the fabricated single-mode, highly nonlinear dispersion tailored lead silicate glass fibre for high speed optical communication.…”
Recent advances in optical fibre technology, most notably in the area of microstructured optical fibres (MOFs), offer a host of new opportunities within future high speed communication systems. Herein we review how our recent progress on the implementation of lead silicate fibre designs, allowing both flexible dispersion control and a high effective nonlinearity, can be integrated into various all-optical signal processing devices for high speed optical communication systems. Highly nonlinear lead silicate fibres have already proven to be well suited for achieving efficient four-wave mixing (FWM) due to their high effective nonlinear coefficient, low dispersion profile and short length. Keywords: All-optical signal processing, nonlinear optics, optical communications, four-wave mixing.
INTRODUCTIONThe ability to fabricate small core soft-glass holey fibres (HFs) with tailored dispersion properties (in particular with flattened and near-zero values) and 2-3 orders of magnitude higher effective nonlinearity than silica fibres opens new prospects in the implementation of compact, all-optical nonlinear devices [1], such as wavelength conversion, signal regeneration and the like, which can radically transform future optical networks. Four-wave-mixing (FWM)-based switches are particularly attractive, since they offer transparency both in terms of modulation formats and repetition rates. Key fibre parameters for achieving broadband, highly efficient FWM processes are: (i) a highly nonlinear medium, (ii) low dispersion values over a broad wavelength range and (iii) short lengths in order to enhance the phase matching process. While several high-nonlinearity and dispersionflattened air/glass HFs have been demonstrated using either silica [2] or non-silica [1] glass as the host material, the precise control of their corresponding dispersion is extremely hard to achieve. This is because precise dispersion control requires extreme precision in the dimensions and spacing of the µm-scale holes of the microstructure. The complex interdependence between temperature, surface tension and internal pressure within the holes, however, causes small-scale longitudinal cross sectional variations, which are very difficult to control in practice. To solve this issue we have proposed in [3] a new all-solid fibre concept based on the use of three commercial lead silicate glasses (Schott SF57, LLF1, SF6) arranged in a W-type index profile. The fabricated fibre presents a flattened and near-zero dispersion profile and a high nonlinearity of 820W -1 km -1 at the telecom wavelengths. Accurate polishing of the glass preform before the fibre drawing has allowed us to reduce the propagation losses from an initial value of ~5dB/m [3] down to ~2dB/m [4] in the 1.55µm region. In this talk we will review some examples of successful applications of the fabricated single-mode, highly nonlinear dispersion tailored lead silicate glass fibre for high speed optical communication.
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